a950fa_Science___22_October_2026_ebooksyard — 2026-10-24

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🧭 今日主编程控导读:聚焦「煽动者」、「AI 科学家智能体」等核心政经议题

今日《a950fa_Science___22_October_2026_ebooksyard》全报共收录 412 篇核心报道。在政经治理、法理制度与公共政策层面,版面重心聚焦于:**煽动者**(一名 FBI 特工促使美国国立卫生研究院(NIH)开展针对美国校园外国干预的行动。现在,他正在研究该问题的严重程度 JE...);**AI 科学家智能体**(虚拟生物技术公司(Virtual Biotech)由一名虚拟首席科学官(CSO)智能体、分布在四个研究部门的八名不同科学...);**急诊医学研究**(CPC病例由学术临床医生策划,而急诊(ED)病例则由当代的电子健康记录(EHR)笔记组成,这些笔记反映了常规工作流程和更...)。 在本土文化与城市记忆方面,今日重点关注**「书评等」**。

399 人
核心数据指标
600万美元
核心数据指标
170,000人
核心数据指标

🎭 本期时代思潮与社会文化雷达

🎭 当代文化观察

《a950fa_Science___22_October_2026_ebooksyard》本期社会思潮与时代切片

本期特写报道深入探索社会结构转型与文化心态变迁,详见【📖 双语精读】各专题深度报道。

🗂️ 全版面分栏导览目录 (点击标题直达正文)

📑 AI / 跨领域发现

📑 地球科学 / 内核研究

📑 研究安全 / 联邦调查

📑 社会科学 / 原住民教育

📑 经济 / 气候金融

📑 化学神经科学 / 毒理学

📑 植物生物学 / 生长机制

📑 癌症研究 / 分子生物学

📑 AI / 药物研发

📑 肿瘤免疫学 / 空间转录组

📑 生物医学工程 / 电催化

📑 细胞生物学 / 线粒体凋亡

📑 发育生物学 / 基因调控

📑 生态学 / 气候变化

📑 生物化学 / 酶结构

📑 凝聚态物理 / 热电输运

📑 医疗 AI / 诊断推理

📑 量子材料 / 电子结构

📑 材料科学 / 膜分离

📑 冰川学 / 古气候

综合要闻 1

AAAS

AI 在医学中的应用

引导临床检查以达成诊断 第 423 页

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2026 年 10 月 22 日

引发美国国立卫生研究院(NIH)针对中国调查的 FBI💡 特工 第 378 页

在冰河时代到来前将其拦截 第 381 & 455 页

科学倡导在艺术中找到盟友 第 386 页

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凯斯西储大学

在第 460 页了解更多关于我们的“教师 100 计划”(Faculty 100 Initiative)#

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增长最快的 AAU 研究型大学

全美

顶尖

—《时代》杂志

目录

2026 年 10 月 22 日 / 第 394 卷 / 第 6822 期

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381 & 455

加拿大巴芬岛巴恩斯冰帽的边缘及其在 1960 年左右的最大延伸位置

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社论

363 AI 辩论缺失了系统的一半

—P. Michelucchi

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新闻

364 疫苗试验为刚果的埃博拉疫情带来一线希望

研究将首先测试“不匹配”的疫苗,但针对 Bundibugyo 的特异性疫苗可能很快会被加入

—K. Kupferschmidt

366 跨领域 AI 发现隐藏在眼前的解决方案

“BootLoops”软件使研究人员能够快速发现并攻克 22 个学科中的问题

—C. Zhao

367 致命细菌的驯化如何导致肉毒杆菌毒素 (Botox) 的出现

研究发现,科学家在无意中将梭菌毒素杆菌 / 肉毒杆菌变成了医学和美容行业的工具

—J. Cohen

368 微波天文台窥探婴儿宇宙

在智利,西蒙斯天文台开始搜寻星系团和宇宙暴胀的迹象

—D. Clery

370 深海生物仍深受 BP 原油泄漏事故影响

一项为期 13 年的研究显示,墨西哥湾生态系统仍未恢复

—E. Stokstad

371 地球核心的铁可能呈现出令人惊讶的形式

X 射线实验揭示了立方晶体,这可能会使地核内部的图像变得复杂

—P. Voosen

372 被解雇的生物学家在诽谤诉讼中赢得 $6 百万美元赔偿

陪审团做出有利于大卫·萨巴蒂尼的裁决,驳回了原告关于性骚扰和报复的指控

—P. Jacobs

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特写

374 关注球路

本周,一个在美国职业棒球大联盟中判定好球和坏球的“机器人裁判”将在世界大赛中首次亮相。

它必须近乎完美

—J. Cohen

378 发起者

一名 FBI 特工促使美国国立卫生研究院(NIH)开展针对美国校园外国干预的行动。现在,他正在研究该问题的严重程度

—J. Mervis

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评论

观点

381 下一个冰河时代是否已经到来并离去?

大陆冰川的最后残余表明,全球变暖可能已经阻止了下一次冰期

—S. A. Marcott

研究论文 第 455 页

382 将葡萄糖代谢置于电子控制之下

一种电子设备控制调节小鼠葡萄糖浓度的氧化还原机制

—W. E. Bentley 和 G. F. Payne

研究摘要 第 400 页

两种使线粒体通透的蛋白质通过不同的机制促进细胞死亡

—C. Muñoz-Pinedo 和 S. J. Martin 研究摘要 第 401 页

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2026 年顶尖雇主:从 AI 到我愿意

Science Careers 的年度调查重点介绍了获得 Science 读者最高赞誉的生物技术和制药领军企业。

请阅读第 461 页的文章,并在 ScienceCareers.org / TopEmployers 在线探索这些高评价雇主

Science2026

顶尖雇主

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385 鸟类大脑的认知能力

寒鸦做出决定的速度比猴子和人类更快

—M. Colombo 和 O. Poutrain-Sorel 研究论文 第 445 页

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书评等

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386 显微镜与隐喻

科学告诉我们如何拯救地球——而诗歌帮助我们理解为什么要这样做

—P. Levin 和 D. Hassler 播客

387 君主熊

—L. Volski

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读者来信

388 原住民高等教育需要支持

—B. E. Soares 等

389 印度需要一项树木保护计划 —A. Dhyani

389 AI 生物安全必须涵盖农业

—J. Feldman 等

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分析

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政策文章

390 缺乏物理韧性的财政纪律

改革可以将财政纪律与韧性投资转化为增强力量,而非竞争力量

—A. Mishra 等

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研究

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亮点

394 来自《Science》及其他期刊

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研究摘要

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397 癌症

内含子保留调节 STAT2 功能并与肺癌的免疫治疗反应相关 —R. P. Englander 等

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398 太阳能电池

用于高效柔性太阳能组件的解耦自组装单层和钙钛矿沉积 —Y. Wu 等

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399 人工智能

虚拟生物技术:一个用于治疗药物发现与开发的多智能体 AI 框架 —H. G. Zhang 等

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400 代谢

用于无药管理糖尿病肥胖综合征的无线电催化闭环系统 —D. Maity 等

观点 p. 382

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401 细胞生物学

BAK 和 BAX 形成多蛋白复合物以驱动 mtDNA 外流和非 caspase 依赖性细胞死亡 —S. Yang 等

观点 p. 383

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研究论文

402 分子生物学

非编码转录控制远程基因调节的发育动力学

—P. J. Batut 等

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408 保育生物学

保护全球陆生脊椎动物免受未来海平面上升的影响 —Z.-W. Jiang 等

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413 天然产物

植物和细菌中鸟苷酸异戊烯基转移酶的天然产物生物合成

—D. Kolling 等

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419 凝聚态物理

蜂窝状反铁磁体中声子霍尔效应的热力学起源 —Q. Meng 等

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423 机器学习

利用语言模型进行顺序诊断 —H. Nori 等

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429 物理学

二维金属中的连续谱电子束缚态 —M. Thinel 等

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434 膜

纳米通道中动态功能实现的快速且选择性传输 —H. Zhang 等

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440 二维材料

可视化对称破缺的陈绝缘体及其量子熔融 —M. He 等

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445 比较认知

鸟类大脑中的超快速决策

—P. Schmidbauer 和 A. Nieder 观点 p. 385;播客

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385 & 445

乌鸦在随机点运动辨别任务中表现出超快速的决策时间。

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目录

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封面

这张图片描绘了一名患者和一名医生在人工智能(AI)的协作下共同得出诊断。研究人员开发了一种基于 AI 的方法,旨在帮助医生进行现实生活中的临床检查,从患者的主诉开始,系统地提出问题并决定订购哪些实验室和影像学检查,然后根据收到的答案继续评估。见第 423 页。插图:Jason Solo

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450 二维材料

广义维格纳晶体量子熔融中的电子-空穴不对称成像 —E. Berger 等

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455 冰川起始

晚全新世劳伦泰德冰盖的再次扩张 —N. E. Young 等

观点 p. 381

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职业生活

462 我隐藏的无家可归过去

—S. Raymond

362 Science 员工

460 Science 职业

Science 美国科学促进会 (AAAS)

总编辑 Holden Thorp, hthorp@aaas.org

执行编辑 Valda Vinson

研究编辑 Sacha Vignieri, Jake S. Yeston 评论编辑 Lisa D. Chong

副执行编辑 Lauren Kmec

副编辑 Stella M. Hurtley (英国), Phillip D. Szuromi 高级编辑 Michael A. Funk, Angela Hessler, Di Jiang, Priscilla N. Kelly, Marc S. Lavine (加拿大), Bianca Lopez, Mattia Maroso (英国), Yevgeniya Nusinovich, Ian S. Osborne (英国), Joana Osório (英国), Cheri Sirois, H. Jesse Smith, Keith T. Smith (英国), Jelena Stajic, Yury V. Suleymanov, Valerie B. Thompson, Brad Wible 助理编辑 Jack Huang, Sumin Jin, Sarah Ross (英国), Madeleine Seale (英国), Corinne Simonti, Unnati Sonawala 高级信函编辑 Jennifer Sills 高级时事通讯编辑 Christie Wilcox 研究与数据分析师 Jessica L. Slater 首席内容制作编辑 Chris Filiatreau, Harry Jach 高级内容制作编辑 Amelia Beyna, Julia Haber-Katris 内容制作编辑 Anne Abraham, Robert French, Nida Masiulis, Avery Shantha, Suzanne M. White 高级项目助理 Maryrose Madrid 编辑经理 Joi S. Granger 编辑助理 Aneera Dobbins, Lisa Johnson, Jerry Richardson, Anita Wynn 高级编辑协调员 Clair Goodhead (英国), Alexander Kief, Kat Kirkman, Ronmel Navas, Isabel Schnaidt, Alice Whaley (英国), Brian White 编辑协调员 Samuel Bates, Daniel Young 行政协调员 Karalee P. Rogers ASI 运营总监 Janet Clements (英国) ASI 办公室经理 Carly Hayward (英国) ASI 高级办公室管理员 Simon Brignell (英国), Jessica Waldock (英国) 通讯总监 Meagan Phelan 副总监 Matthew Wright 高级撰稿人 Walter Beckwith, Joseph Cariz, Abigail Eisenstadt 撰稿人 Mahathi Ramaswamy 高级通讯助理 Kiara Brooks, Zachary Graber, Mackenzie Williams, Sarah Woods

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新闻编辑 Tim Appenzeller

新闻执行编辑 John Travis 全球健康编辑 Martin Enserink 副新闻编辑 Rachel Bernstein, David Grimm, Eric Hand, David Malakoff (人工智能), Michael Price, Kelly Servick, Matthew Warren (国际) 高级记者 Daniel Clery (英国), Jon Cohen, Jocelyn Kaiser, Jeffrey Mervis 助理编辑 Michael Greshko, Katie Langin 新闻记者 Jeffrey Brainard, Adrian Cho, Phie Jacobs, Sara Reardon, Jennie Erin Smith, Erik Stokstad, Paul Voosen, Celina Zhao 顾问编辑 Elizabeth Culotta 特约记者 Vaishnavi Chandrashekhar, Dan Charles, Warren Cornwall, Andrew Curry (柏林), Ann Gibbons, Kai Kupferschmidt (柏林), Andrew Lawler, Mitch Leslie, Virginia Morell, Dennis Normile (东京), Catherine Offord, Cathleen O'Grady, Elisabeth Pain (职业), Charles Piller, Hannah Richter, Zack Savitsky, Richard Stone (高级亚洲记者), Gretchen Vogel (柏林), Lizzie Wade (墨西哥城) 实习生 Laura Martín Agudelo, Ailie McWhinnie, Mona Patterson, Julia Vaz 校对编辑 Julia Cole (高级校对编辑), Hannah Knighton, Cyra Master (校对主管) 行政支持 Meagan Weiland

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创意总监 Beth Rakouskas

设计执行编辑 Chrystal Smith 图形执行编辑 Chris Bickel 摄影执行编辑 Emily Petersen 多媒体执行制片人 Kevin McLean 数字总监 Kara Estelle-Powers 设计编辑 Marcy Atarod 设计师 Noelle Jessup 高级科学插画师 Noelle Burgess 科学插画师 Austin Fisher, Kellie Holoski, Ashley Mastin 高级图形编辑 Monica Hersher 图形编辑 Veronica Penney 高级照片编辑 Charles Borst 照片编辑 Elizabeth Billman 高级播客制片人 Sarah Crespi 高级视频制片人 Meagan Cantwell 社交媒体策略师 Jessica Hubbard 社交媒体制片人 Sabrina Jenkins 网页设计师 Jennie Pajerowski

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首席执行官兼执行出版人

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Sudip Parikh

《科学》系列期刊出版人 Bill Moran

业务运营与分析总监 Eric Knott 业务运营经理 Jessica Tierney 业务分析高级经理 Cory Lipman 业务分析师 Kurt Ennis, Maggie Clark, Isacco Fusi 业务运营管理员 Taylor Fisher 数字专家 Marissa Zuckerman 制作与平台副总监 Jason Hillman 出版与内容系统高级经理 Marcus Spiegler 内容运营经理 Rebecca Doshi 出版平台经理 Jessica Loayza 出版系统专家、项目协调员 Jacob Hedrick 制作主管 Kristin Wowk

营销总监 Sharice Collins 营销副总监 Justin Sawyers 全球营销经理 Allison Pritchard

营销经理 Ashley Evans 高级营销助理 Lorena Chirinos Rodriguez 营销协调员 Jonathan Moskowitz 高级设计师 Kim Huynh

定制出版总监兼高级编辑 Erika Gebel Berg 定制出版副总监 Michael Wheeler 广告制作运营经理 Deborah Tompkins 定制出版设计师 Jeremy Huntsinger 高级流量助理 Christine Hall

产品管理总监 Kris Bishop 产品开发经理 Scott Chernoff 合作伙伴营销副总监 Shawana Arnold SPJ 营销经理 Ashley Hylton 出版情报副总监 Rasmus Andersen 产品经理 Robert Koepke, Anne Mason 产品助理 Caroline Breul

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国际业务副总监 Roger Goncalves 美国广告副总监 Stephanie O'Connor 美国中西部、中大西洋及东南部销售经理 Chris Hoag 亚洲外展与战略合作伙伴关系总监 Shoupeng Liu ASI EMEA 销售广告经理 Sarah Lelarge 广告销售助理 (ROW) Victoria Glasbey 亚洲全球协作与学术出版关系总监 Xiaoying Chu 国际协作副总监 Grace Yao 销售经理 Danny Zhao 营销经理 Kilo Lan ASCA 公司(日本) Rie Rambelli (东京), Miyuki Tani (大阪)

版权、许可与特别项目总监 Emilie David 权利与许可助理 Elizabeth Sandler 许可助理 Virginia Warren 权利与许可协调员 Dana James

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AAAS 董事会

主席 Joseph S. Francisco

前任主席

Theresa A. Maldonado

主席

Marina Picciotto

候任主席

Eric D. Isaacs

财务主管 Mark F. Dingfield

理事会主席

Ichiro Nishimura

首席执行官

Sudip Parikh

董事会成员

Carolyn N. Ainslie

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Juan S. Ramírez Lugo

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Takuzo Aida, 东京大学

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审稿编辑委员会(统计学委员会成员以 S 标出)

Leslie Aiello, Wenner-Gren 基金会

Anastassia Alexandrova, 加州大学洛杉矶分校 (UCLA)

James Analysis, 加州大学伯克利分校 (UC Berkeley)

Amy Ando, 俄亥俄州立大学 (The Ohio State U.)

Paola Arlotta, 哈佛大学 (Harvard U.)

Madan Babu, 圣犹达 (St. Jude)

Jennifer Balch, 科罗拉多大学 (U. of Colorado)

Nenad Ban, 苏黎世联邦理工学院 (ETH Zürich)

Carolina Barillas-Mury, 美国国立卫生研究院 (NIH), 美国国立过敏和传染病研究所 (NIAID)

Christopher Barratt, 邓迪大学 (U. of Dundee)

François Barthelat, 科罗拉多大学博尔德分校 (U. of Colorado Boulder)

Joseph Bass, 西北大学 (Northwestern U.)

Franz Bauer, 塔拉帕卡大学 (Universidad de Tarapacá)

Andreas Baumler, 加州大学戴维斯分校 (UC Davis)

Carlo Beenakker, 莱顿大学 (Leiden U.)

Camilla Bellone, 日内瓦大学 (Geneva U.)

Sarah Bergbreiter, 卡内基梅隆大学 (Carnegie Mellon U.)

Kiros T. Berhane, 哥伦比亚大学 (Columbia U.)

Aude Bernheim, 巴斯德研究所 (Inst. Pasteur)

Joseph J. Berry, 国家可再生能源实验室 (NREL)

Aditi Bhargava, 加州大学旧金山分校 (UCSF)

Dominique Bonnet, 弗朗西斯·克里克研究所 (Francis Crick Inst.)

Chris Bowler, 巴黎高等师范学院 (École Normale Supérieure)

Ian Boyd, 圣安德鲁斯大学 (U. of St. Andrews)

Malcolm Brenner, 贝勒医学院 (Baylor College of Med.)

Ron Brookmeyer, 加州大学洛杉矶分校 (UCLA) (\$) Christian Büchel, 汉堡大学医学中心 (UKE Hamburg)

Johannes Buchner, 慕尼黑工业大学 (TUM)

Dennis Burton, 斯克里普斯研究所 (Scripps Res.)

Carter Tribley Butts, 加州大学欧文分校 (UC Irvine)

Erin Calipari, 范德堡大学 (Vanderbilt U.)

Annmarie Carlton, 加州大学欧文分校 (UC Irvine)

Jane Carlton, 约翰霍普金斯大学 (Johns Hopkins U.)

Pedro Carvalho, 牛津大学 (U. of Oxford)

Simon Cauchemez, 巴斯德研究所 (Inst. Pasteur)

Ling-Ling Chen, 中国科学院 (CAS) 生物物理研究所 (SIBCB)

Hilde Cheroutre, 拉霍亚研究所 (La Jolla Inst.)

Wendy Cho, 伊利诺伊大学厄巴纳-香槟分校 (UIUC)

Ib Chorkendorff, 丹麦技术大学 (Denmark TU)

Chunaram Choudhary, Kabelene Hervis 大学 (Kabelene Hervis U.)

Karlene Cimprich, 斯坦福大学 (Stanford U.)

Laura Colgin, 德克萨斯大学奥斯汀分校 (UT Austin)

James J. Collins, 麻省理工学院 (MIT)

Robert Cook-Deegan,

Carolyn Coyne, 杜克大学 (Duke U.)

Roberta Croce, 阿姆斯特丹自由大学 (VU Amsterdam)

Ismaila Dabo, 宾夕法尼亚州立大学 (Penn State U.)

Nicolas Dauphas, 芝加哥大学 (U. of Chicago)

Liset de la Prida, 西班牙国家研究委员会 (CSIC) 卡哈尔研究所 (Instituto Cajal)

Orsola De Marco, 麦考瑞大学 (Macquarie U.)

Claude Desplan, 纽约大学 (NYU)

Sandra Díaz, 科尔多瓦国立大学 (U. Nacional de Córdoba)

Samuel Díaz-Muñoz, 加州大学戴维斯分校 (UC Davis)

Ulrike Diebold, 维也纳技术大学 (TU Wien)

Stefanie Dimmeler, 法兰克福大学 (Cootho U. Frankfurt)

Hong Ding, 中国科学院 (CAS) 物理研究所 (Inst. of Physics)

Dennis Discher, 宾夕法尼亚大学 (UPenn)

Jennifer A. Doudna, 加州大学伯克利分校 (UC Berkeley)

Raissa M. D'Souza, 加州大学戴维斯分校 (UC Davis)

Bruce Dunn, 加州大学洛杉矶分校 (UCLA)

Scott Edwards, 哈佛大学 (Harvard) 6.

Todd A. Ehlers, 格拉斯哥大学 (U. of Glasgow)

Tobias Erb,

马克斯·普朗克学会 (MPS), 马克斯·普朗克陆地微生物学研究所 (MPI Terrestrial Microbiology)

Beate Escher, 亥姆霍兹环境研究中心 (UFZ) & 图宾根大学 (U. of Tübingen)

Vanessa Ezenwa, 佐治亚大学 (U. of Georgia)

Fleur Ferguson, 加州大学圣迭戈分校 (U. San Dieg)

Toren Finkel, 匹兹堡大学医学中心 (U. of Pitt. Med. Ctr.) Natascha Förster Schreiber, 马克斯·普朗克地外物理研究所 (MPI Extraterrestrial Phys.)

Simon Greenhill, 奥克兰大学 (U. of Auckland)

Gillian Griffiths, 剑桥大学 (U. of Cambridge)

Nicolas Gruber, 苏黎世联邦理工学院 (ETH Zürich)

Hua Guo, 新墨西哥大学 (U. of New Mexico)

Osvaldo Gutierrez, 加州大学洛杉矶分校 (UCLA)

Taekjip Ha, 约翰霍普金斯大学 (Johns Hopkins U.)

Daniel Haber, 马萨诸塞州总医院 (Mass. General Hos.)

Hamida Hammad, VIB IRC

Brian Hare, 杜克大学 (Duke U.)

Kelley Harris, 华盛顿大学 (U. of Wash)

Sheng-Yang He, 杜克大学 (Duke U.)

Carl-Philipp Heisenberg, 奥地利科学技术研究所 (IST Austria)

巴塞尔大学 (U. of Basel) & 剑桥大学 (U. of Cambridge)

Heather Hickman, 美国国立卫生研究院 (NIH), 美国国立过敏和传染病研究所 (NIAID)

Brian Hie, 斯坦福大学 (Stanford U.)

Janneke Hille Ris Lambers, 苏黎世联邦理工学院 (ETH Zürich)

Pinshane Huang, 伊利诺伊大学厄巴纳-香槟分校 (UIUC)

Christina Hulbe, 奥塔哥大学 (U. of Otago), 新西兰

Gwyneth Ingram, 里昂高等师范学院 (ENS Lyon)

Darrell Irvine, 斯克里普斯研究所 (Scripps Res.)

Bharat Jalan, 明尼苏达大学 (U. of Minnesota)

Erich Jarvis, 洛克菲勒大学 (Rockefeller U.)

Sheena Josselyn, 多伦多大学 (U. of Toronto)

Matt Kaeberlein, 华盛顿大学 (U. of Wash.)

Daniel Kammen, 加州大学伯克利分校 (UC Berkeley)

Kisuk Kang, 首尔国立大学 (Seoul Nat. U.)

V. Narry Kim, 首尔国立大学 (Seoul Nat. U.)

Logan Kistler, 史密森学会 (Smithsonian Inst.)

Nancy Knowlton, 史密森学会 (Smithsonian)

Etienne Koechlin, 巴黎高等师范学院 (École Normale Supérieure)

Peter Koo, 冷泉港实验室 (Cold Spring Harbor Lab)

Paul Kubes, 卡尔加里大学 (U. of Calgary)

Yulong Li, 北京大学 (Peking U.)

Ryan Lively, 佐治亚理工学院 (Georgia Tech)

Luis Liz-Marzán, CIC biomaGUNE

Omar Lizardo, 加州大学洛杉矶分校 (UCLA)

Jeffery Molkentin, 辛辛那提儿童医院医学中心 (Cincinnati Children's Hospital Medical Center) Alison Motsinger-Reif, 美国国立卫生研究院 (NIH), 美国国立环境健康科学研究所 (NIEHS) (S)

Rosa Moysés, 圣保罗大学 (U. of São Paulo) 医学院

Carey Nadell, 达特茅斯学院 (Dartmouth College)

Thi Hoang Duong Nguyen, 英国医学研究委员会分子生物学实验室 (MRC LMB)

Pilar Ossorio, 威斯康星大学 (U. of Wisconsin)

Andrew Oswald, 华威大学 (U. of Warwick)

James Owen, 伦敦帝国学院 (Imperial College London)

Pierre Paoletti, 巴黎高等师范学院 (Ecole Normale Supérieure, Paris)

Philip Phillips, 伊利诺伊大学厄巴纳-香槟分校 (UIUC)

Kathrin Plath, 加州大学洛杉矶分校 (UCLA)

Martin Plenio, 乌尔姆大学 (Ulm U.)

Katherine Pollard, 加州大学旧金山分校 (UCSF)

Julia Pongratz, 路德维希-马克西米利安大学 (Ludwig Maximilians U.)

Philippe Poulin, 法国国家科学研究中心 (CNRS)

Suzie Pun, 华盛顿大学 (U. of Wash)

Lei Stanley Qi, 斯坦福大学 (Stanford U.)

Simona Radutoiu, 奥胡斯大学 (Aarhus U.)

Joeri Rogelj, 伦敦帝国学院 (Imperial College London)

Sylvie Roke, 洛桑联邦理工学院 (École Polytechnique Fédérale de Lausanne)

Sarah Ross, 匹兹堡大学 (U. of Pittsburgh)

John Rubinstein, SickKids

Yvette Running Horse Collin, 图卢兹大学 (Toulouse U.)

Mike Ryan, 德克萨斯大学奥斯汀分校 (UT Austin)

Alberto Salleo, 斯坦福大学 (Stanford U.)

劳伦斯伯克利国家实验室

Nitin Samarth, 宾夕法尼亚州立大学

Bhaven Sampat, 约翰霍普金斯大学

Erica Ollmann Saphire,

拉霍亚研究所

Vladimir Shalaev, 普渡大学 Jie Shan, 康奈尔大学

Jay Shendure, 华盛顿大学

Steve Sherwood,

新南威尔士大学

Robert Siliciano, 约翰霍普金斯大学医学院

Emma Slack,

苏黎世联邦理工学院 & 牛津大学

Richard Smith, 北卡罗来纳大学 (S)

卡内基科学研究所

V. S. Subrahmanian,

西北大学

Sandip Sukhtankar, 弗吉尼亚大学

Christopher Summerfield,

牛津大学

Tavneet Suri, 麻省理工学院

Naomi Tague, 加州大学圣巴巴拉分校

A. Alec Talin, 桑迪亚国家实验室

Patrick Tan, 杜克-新加坡国立大学医学院

Fuchou Tang, 北京 BIOPIC

Dörthe Tetzlaff, 莱布尼茨淡水生态学与内陆渔业研究所 Amanda Thomas, 加州大学戴维斯分校

Bozhi Tian, 芝加哥大学

Rocio Titiunik, 普林斯顿大学

Shubha Tole,

塔塔基础研究学院

Kimani Toussaint, 布朗大学

Li-Huei Tsai, 麻省理工学院

Jason Tylianakis, 坎特伯雷大学

Jo Van Ginderachter,

VIB, 根特大学

Matthew Vander Heiden, 麻省理工学院

Ivo Vankelecom, 鲁汶大学

Henrique Veiga-Fernandes,

Champalimaud 基金会

Elizabeth Villa, 加州大学圣迭戈分校

Bert Vogelstein, 约翰霍普金斯大学

David Wallach, 魏茨曼科学研究所

Jane-Ling Wang, 加州大学戴维斯分校 (\$) Jessica Ware,

美国自然历史博物馆

David Waxman, 复旦大学

Alex Webb, 剑桥大学

Marjorie Weber, 密歇根大学

Chris Wikle, 密苏里大学 (\$)

Ian A. Wilson, 斯克里普斯研究所 (\$)

Sylvia Wirth, ISC Marc Jeannerod

Catherine Wolfram, 麻省理工学院

Amir Yacoby, 哈佛大学

Benjamin Youngblood, 圣犹达

Kenneth Zaret, 宾夕法尼亚大学医学院

Magdalena Zernicka-Goetz, 加州理工学院

Bing Zhai, 深圳先进技术研究院

Lidong Zhao, 北京航空航天大学

Bing Zhu, 中国科学院生物物理研究所

Xiaowei Zhuang, 哈佛大学

Maria Zuber, 麻省理工学院

AI 辩论缺失了系统的一半

Pietro Michelucci

上个月,人工智能(AI)公司的顶尖高管们向联合国安理会警告,人们可能会失去对这项飞速发展技术的控制。他们的建议重点集中在 UCLA 模型和系统的保障、评估与治理上,在很大程度上忽视了 UCLA 与人及机构交互时产生的风险。 UCLA 安全需要在“人- 系统”层面来解决,而不仅仅是针对 UCLA 模型本身。

赌注很高。人们已经嵌入到那些从人类与 UCLA 交互中获取能力和行为的系统中。 UCLA 正在影响人们选择什么样的医疗方案、公司在何处投资、城市如何优化民用基础设施,甚至影响国家如何处理国家安全。人类不再是独立思考,而是与 UCLA 处于一个持续的反馈循环中——他们并非系统的外部存在。随着社会日益依赖 系统,一个“紧急停止开关”本身无法成为一个可行或可持续的安全特性。

真正的问题是整个“人- 系统”的安全。没有任何单一组件(无论是人还是机器)能被打造得绝对可靠。因此,即使其组件变得不可靠,系统本身也必须保持安全。但如何在这个复杂的系统中构建自我修正和韧性?

虽然这看起来似乎难以逾越,但在人类计算(human computation)领域,构建由不可靠组件组成可靠系统的方法一直在开发中,该领域研究依赖于反馈循环中人类的计算系统。例如,一种方法是实施一种基于基本社会原则的“信任分”机制,即信任建立缓慢但破坏迅速。为了实现这一点,系统将已知正确答案的测试问题随机混入答案未知的工作中。当个人答错测试题或试图作弊时,其信任分会下降。如果分数低于某个阈值,该人员可以继续工作,但其答案不再影响系统输出。该个人可以通过再次提供正确答案来缓慢恢复信任。通过动态监测,参与者的贡献可以保持价值,而其影响力则根据其表现的实时波动而变化。关键在于,信任、影响力和权威不需要是固定不变的。它们可以随着新证据的出现而不断调整。

以最近的 Hugging Face 事件为例,运行网络安全评估的 UCLA 代理绕过了测试环境的限制,寻求关于其如何被评估的信息,并协调对一个外部开源平台发起网络攻击。一种动态评估方法可以监测 系统在执行指定任务时是否开始采取有害行动,并迅速降低该系统对工具或数据的访问权限,或降低其自主行动的能力。只有在出现持续的可靠行为证据后,这些能力才能被恢复。

同样的原则可以应用于更广泛的人- 系统。关于人- 系统执行任务效果的可靠证据,可用于在条件变化时调整各种参数(例如数据访问权限)。这将讨论的重点从“ 是否足够安全可以部署”,转移到“信任、影响力和自主权应如何在人- 系统中分布”。

许多 科学家和社会科学家正致力于开发可靠且具有韧性的人- 系统。例如,美国国家标准与技术研究院的“评估 风险与影响”项目正在扩大 评估

模型之外,还包括在现实场景中与人类用户的交互。然而,为系统性能提供证据本身就可能成为评估其是否安全的障碍。性能并不总是能针对已知结果进行测试,或对决策进行独立审计。监测性能本身可能会在人类参与者之间产生涉及隐私、同意和权限的风险。因此,任何可持续的方法不仅必须解决信任和影响力如何调整的问题,还必须解决什么样的证据能证明这些调整是合理的、谁可以观察这些调整,以及谁有权采取行动。

监管机构不应将 AI 模型视为一个通过初始测试后就再也不用检查的设备,而需要考虑 AI 在现实世界中与人类用户共同协作时的表现,以及系统的权限如何基于随时间证明的可靠性而得到持续的监测和调整。这意味着要开发安全协议,使其从静态护栏转向动态评估,并从仅关注 AI 模型转向关注完整的人机系统。□

Pietro Michelucci 是美国纽约州伊萨卡的人类计算研究所(Human Computation Institute)执行主任。pem@hcinst.org

传染病

疫苗试验为刚果(金)埃博拉疫情带来一线希望

研究将首先测试“不匹配”疫苗,但针对 Bundibugyo 的特异性疫苗可能很快被加入 KAI KUPFERSCHMIDT

在刚果民主共和国(DRC)北基伍省,一线响应人员排队接受基于“同情”原则接种的名为 Ervebo 的埃博拉疫苗。

在关于刚果民主共和国(DRC)Bundibugyo 埃博拉病毒爆发式疫情的接连噩耗中,出现了一些希望的曙光。经过数月的辩论和准备,一项名为 Tumaini(斯瓦希里语意为“希望”)的疫苗试验预计将在近期通过最后的监管和伦理审查,首批疫苗可能在本周内开始接种。该试验将首先测试 Ervebo,这是一种针对另一种名为 Zaire 的埃博拉病毒物种开发的“不匹配”疫苗。但另外两种专门设计用于防御 Bundibugyo 的疫苗可能会在 11 月被加入到研究中。

与此同时,在报告病例超过 9500 例、死亡人数超过 4600 人的情况下,疫情在震中且受灾最严重的伊图里省似乎正在放缓。刚果民主共和国国家生物医学研究所负责人 Jean-Jacques Muyembe-Tamfun 表示,新报告病例的数量和检测阳性率都在下降:“虽然还没达到理想状态,但已经有所改善。”

此外,一项测试两种潜在埃博拉治疗药物——名为 MBP134 的抗体鸡尾酒疗法和抗病毒药物瑞德西韦(remdesivir)的试验已经招募了 600 多名患者。非洲疾病预防控制中心(Africa Centres for Disease Control and Prevention)的 Placide Mbala 是该试验的主任研究员,他表示可能很快就会有足够的数据来观察疗效。世界卫生组织(WHO)健康应急项目负责人、流行病学家 Chikwe Ihekweazu 表示,有效的治疗将极大地增强应对能力。“武器库中每增加一件工具都有帮助。”

尽管如此,挑战依然巨大。疾病仍可能扩散到更多地方。本月早些时候,肯尼亚宣布了首例 Bundibugyo 病例,一名 40 岁的肯尼亚男子在经由乌干达从刚果民主共和国旅行后在内罗毕死亡。四名家庭成员和四名医护人员也检测呈阳性并处于隔离状态。10 月 20 日,尼日利亚也报告了一例病例,一名曾前往乌干达的女性;乌干达今年早些时候曾出现 20 例病例,但已于 7 月宣布疫情结束。

在刚果民主共和国,三分之二死于埃博拉的人员仍然是在社区中而非在专门的治疗中心死亡,这造成了进一步传播的风险。接触者追踪工作仍然运行不畅;约 40% 的新确诊病例不在任何已知埃博拉病例的接触者名单上。世界卫生组织非洲区域办事处疫情事件经理 Marie Roseline Belizaire 表示,这一比例已从疫情初期的约 70% 下降。“这是进步,但还不够。”

尽管伊图里省的病例数有所下降,但在受影响第二严重的北基伍省,病例数呈上升趋势。世卫组织和其他团体正紧急向该地转移更多资源。Ihekweazu 表示:“我认为观察其发展轨迹将非常重要。”他警告说,随着每天报告数十例新病例,疫情不会迅速结束。“唯一的转折点将是我们是否能拥有一种可以大规模部署的高效疫苗。”

这就是为什么疫苗试验的赌注如此之高。Ervebo 开发于 25 年多前,它将 Zaire 埃博拉病毒的一种表面蛋白整合到一种对人类无害的牲畜病毒中。它首次被用于 2013–16 年毁灭性的西非 Zaire 埃博拉疫情期间,并在 2015 年的一项试验中显示出完全的保护作用。动物研究表明,它可能对 Bundibugyo 同样有效。Tumaini 试验将通过向已知埃博拉病例的直接接触者接种候选疫苗来验证这一前景,其采用的“环形接种”设计与 2015 年试验中所使用的类似。

在那项在几内亚开展的研究中,整个接触者环被随机分配,分别在立即或 3 周后接种埃博拉疫苗。在 Tumaini 试验中,环内的每个人都将被随机分配。目前,一半的人将在第 1 天接种 Ervebo 疫苗,并在 4 周后接种伤寒疫苗;另一半人的接种顺序则相反。

参与设计这两项试验的佛罗里达大学生物统计学家 Ira Longini 表示,随机分配个人而非整个接触者环应该能更快地获得有效性数据。但给予对照组的伤寒疫苗可能会增加检测埃博拉疫苗益处的难度,因为伤寒疫苗可能会增强免疫系统。这可能会保护对照组中的部分人员免受埃博拉感染,从而使疫苗的实际益处看起来比实际情况略小。

安特卫普大学的流行病学家、该试验的主要研究者之一 Jean-Pierre Van geertruyden 表示,团队在 2 周前开始向受影响地区的人们解释试验的设置。使他们的外展工作复杂化的是,在该国部分地区,Ervebo 已经以“同情”使用原则提供给一线响应人员。它还被用于伊图里(Ituri)的医疗工作者,这是一项名为 BRAVO 的独立试验,且没有对照组。Van geertruyden 承认,人们可能会质疑为什么 Ervebo 足以提供给医疗工作者,但却需要在其余人群中进行测试:“人们可能会感到有些困惑。”

一旦 Tumaini 启动并运行,专门针对埃博拉 Bundibugyo 病毒的候选疫苗将在可用时被加入。进展最快的是由牛津大学研究人员开发的一种疫苗,它将 Bundibugyo 的一种表面蛋白缝合到黑猩猩腺病毒中。

牛津大学疫苗学家 Teresa Lambe 表示,目前对在英国和乌干达进行的一期临床试验数据的分析表明,该疫苗可以进入下一阶段,她希望它能“尽快进入试验”。一款由 Moderna 制造的信使 RNA 疫苗紧随其后。Van geertruyden 认为,这两款疫苗都可能在 11 月初被加入到 Tumaini 中。他说,新疫苗的有效性数据可能要到 2027 年 2 月或 3 月才会出现。

到那时,疫情的中心可能已经转移,试验也必须随之移动。组织者必须转移团队,确保住房和食物供应,并在基础设施薄弱的地区维持实验室和冰箱的运行:“我们必须追随疫情,而这并不容易,”Van geertruyden 说。也许到那时,疫情可能不仅在转移,而且在消退。□

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其他新闻

不再有闰秒 国际计量局上周宣布将告别闰秒——它是闰年的一个尴尬“亲戚”,闰年每 4 年在日历中增加一天,以考虑到地球每 365.24 天绕太阳运行一周的事实。闰秒用于补偿地球自转中不可预测的变化,并且仅在原子钟和观测结果表明协调世界时(UTC)——用于根据恒星调节全球时钟的标准——偏差 0.9 秒时,才会添加到 UTC 中。自 1972年以来,闰秒已被添加了 27 次,但其特有的性质给计算机网络和网站带来了问题。该局现在将在 UTC 偏差达到相应幅度时增加一个“闰时”,这意味着下一次调整将在数千年之后才会发生。——Adrian Cho

美国司法部将资助性别研究 美国司法部(DOJ)正准备资助关于性别焦虑(gender dysphoria)的研究,即当一个人的性别认同与其出生时被指定的性别不一致时所产生的痛苦感。9 October 的资助通知称,将拨款最多 $1 百万用于研究“性别焦虑、其治疗以及暴力的实施”,包括研究性别焦虑人群中暴力犯罪的普遍程度。该计划引起了科学家和活动人士的担忧,他们担心这是由政治偏见驱动的,可能会对跨性别者造成伤害,而研究表明,跨性别者成为暴力犯罪受害者的风险更高,而非实施者。——Julia Vaz

西尼罗河病毒在欧洲激增 今年夏天,西尼罗河病毒(WNV)在欧洲传播得更远,导致患病人数达到前所未有的规模。在上周发布的一份报告中,欧洲疾病预防控制中心报告称,自 5 月以来共有 1715 例当地感染的人类病例,其中包括 130 例死亡。受影响最严重的国家是意大利和希腊。但随着比利时报告了其首例由蚊子传播的该疾病病例,该机构表示“病毒目前正在向更北的地方传播,预计这一趋势在未来几年将继续”。大多数西尼罗河病毒感染不产生症状,但大约五分之一的人会生病,大约 100 分之一的人会发展为严重的神经系统疾病,这可能是致命的。

——Kai Kupferschmidt

人工智能

跨领域 AI 寻找显而易见却被忽视的解决方案

“BootLoops”软件使研究人员能够快速发现并攻克 22 个学科中的问题 CELINA ZHAO

一项由 BootLoops 驱动的针对《伏尼契手稿》(一本充满无法破译文字的 15 世纪书籍)的分析得出结论:该手稿并不包含隐藏信息。

借鉴一个研究学科的想法来解决另一个学科中的棘手问题,是一个古老的科学技巧。例如,查尔斯·达尔文(Charles Darwin)的自然选择理论启发了计算机科学中的算法,用于“进化”出复杂问题的解决方案。

但这种巧妙的跨越极其罕见。Hugging Face(一个 AI 工具平台)的科学 AI 负责人 Georgia Channing 表示,通常情况下,“一名物理研究人员不会花 6 个月时间阅读语言学研究,以便弄清楚如何重新利用语言学方法”。

然而,对于 AI 来说,在不同领域之间跳转可以轻而易举。研究人员在本月早些时候发布了 36 篇由名为 BootLoops 的 AI 工具套件生成的预印本,以此凸显了这种能力。这个所谓的“框架”可以与任何大语言模型(LLM)配合使用,例如 Anthropic 的 Claude 或 OpenAI💡 的 ChatGPT。在短短 3 个月内,研究人员使用配备了 BootLoops 的 Claude 进行了大规模的跨领域交叉研究,发现了——并解决了——在看似无关但具有相同数学结构的领域中的问题。由此产生的论文范围广泛,从计算太阳黑子的年龄到尝试破译一份中世纪手稿。

本质上,BootLoops “不断注意到同一个模式:许多领域存在的问题,如果有人知道数学、物理或计算机科学中的某种技术存在,那么这种技术可以直接解决这些问题,”哈佛大学(Harvard University)的物理学家、Anthropic 的访问研究员且该工具的开发者 Matthew Schwartz 在 10 月 1 日揭晓预印本的博客文章中写道。

Schwartz 和其他研究人员表示,该项目还有助于将 AI 引入那些采用速度较慢的科学学科。Channing 说:“这项技术正在渗透到更多领域,这太惊人了。”

研究人员警告说,BootLoops 仍需要大量的人类参与才能产生有用的结果。他们还补充说,它也面临着 AI 驱动的科学研究中常见的局限性。

Schwartz 在 2025 年 12 月开始探索 AI 的研究能力,当时他将 Claude Opus 4.5 视为他的虚拟“研究生”。在密切的指导下,它在短短 2 周内就成功撰写了一篇合理的物理研究论文。对此产生兴趣的 Schwartz 开始给这个 LLM 布置更大的挑战,最终目标甚至雄心勃勃到要重新定义量子力学。但他说:“它还没准备好。”

于是,他想到:与其强迫 AI 像人类研究员那样工作,为什么不发挥它的优势?

一个明显的优势是编程。Schwartz 任务 Claude Fable 5 编写代码,以解决高能粒子碰撞理论分析中使用的一种积分。它检索了物理和数学论文中该积分的其他示例,然后构建了软件来解决其中的 30 个,包括 15 个此前从未被解决的积分。这个工具随后变成了 BootLoops。

接着,他将其应用于更广泛的科学文献,很快就在其他学科中发现了许多类似的未解决问题。Schwartz 说,从那时起,“项目爆发了”,他开始招募其他领域的专家进行合作。

其中一篇由哈佛大学的进化生物学家 Scott Edwards 合著的论文,涉及利用 DNA 数据构建进化树。BootLoops 计算出,关于人类、黑猩猩、大猩猩和红毛猩猩进化关系的两种可能进化树具有相同的可能性——这是以往的估算策略无法确定的。“这是我第一次体验基于 Claude 的科学研究,我绝对能看到它的潜力,”Edwards 说。

BootLoops 还能够找到一种最优方法,对美国政府 Medicare 计划下提供的医疗保险方案进行排名。目前的分类系统基于患者体验等指标,使用一种近似聚类算法来设定五种可能评级之间的分界点。这些分界点随后决定了政府向保险公司支付的奖金。然而,BootLoops 能够计算出精确的最优分箱。随附的预印本表明,实施这些建议可以在 2025 到 27 年间为纳税人节省大约 10 亿美元 billion。

很快,合作范围从数学问题扩展到了其他适合大语言模型(LLM)的工作。在另一个项目中,Schwartz 和三位语言学家使用 AI 智能体搜寻学术文献,并汇总了有史以来最大的语言重音和声调模式标准化目录,同时使用 BootLoops 来检查智能体是否遗漏了某种语言可能使用的任何额外重音系统。由此产生的名为 ACCSTACK 的数据库比此前同类最大的数据集大 8 倍以上,记录了 6000 多种语言的语音系统。马萨诸塞大学阿默斯特分校的预印本共同作者 Joe Pater 表示,ACCSTACK 的“规模真的远远超出了我们仅凭人类之力所能完成的程度”。

但随着 BootLoops 的探索范围进一步扩大,Schwartz 发现,虽然 LLM 可以告诉他它能计算什么,但它无法识别科学家真正关心的是什么。简单来说,它缺乏研究品味。例如,Claude 发现了一个测试生态学中中性生物多样性理论的机会——该理论认为个体和种群之间的许多遗传差异是由随机变异引起的。AI 根据巴拿马一个研究岛屿的数据生成了一个反例,表明树木多样性的变化速度快于仅凭随机机会所预期的速度。

当 Schwartz 请伊利诺伊大学厄巴纳-香槟分校的生态学家 James O'Dwyer 审查结果时,O'Dwyer 认为这些结果“有趣”,但不足以改变领域现状。他说:“我认为它目前还无法取代任何类型的生态学家,但我确实知道,在这种合作下,一切进展得快得多。”

并非所有研究人员都接纳这些工具。一篇预印本分析了伏尼契手稿(Voynich manuscript),这是一本 15 世纪的书,充满了几个世纪以来令学者们困惑的无法破译的文字。该论文声称,这本手稿最终可能并没有编码隐藏的语言信息。但在一个专门讨论该手稿的在线论坛中,一些贡献者抱怨该论文过于晦涩,简直是 AI 生成的“垃圾内容”(slop)。

Schwartz 承认需要谨慎:在同事的建议下,他保留了一些验证不足的结果。但他认为,许多领域的研究人员将从使用跨学科 AI 工具中受益。他说:“一旦每个人都跟上步伐,这个人类-AI 协作时代将会非常令人兴奋。”

微生物学

致命细菌的驯化如何催生了肉毒杆菌毒素 (Botox)

研究发现,科学家在无意中将肉毒杆菌 (C. botulinum) 变成了医学和美容行业的工具 JON COHEN

一场发生在 1919 年、最终导致五人死亡的奢华晚餐派对。一次在 20 世纪 20 年代拯救罐头工业的尝试。一项二战时期的生物武器计划以及美国中央情报局 (CIA) 针对菲德尔·卡斯特罗的阴谋。一种以 Botox 为人熟知的美容产品,它能消除面部皱纹,并迅速发展成为一个价值数十亿美元的产业。

一项对 1000 多个细菌基因组的新分析,通过一项微生物学侦查工作,将美国历史上这些截然不同的片段联系在了一起。这项于 10 月 15 日发表在《美国国家科学院院刊》(PNAS) 上的研究表明,科学家在无意中触发了一种危险细菌的进化,使其具备了巨大的医学和商业优势。

这种微生物就是肉毒杆菌 (Clostridium botulinum),其神经毒素会干扰神经传导,导致肌肉瘫痪并使受害者窒息。这种毒素(简称为 BoNT)是已知最致命的天然物质之一。在无氧条件下(例如在保存食品中),肉毒杆菌的孢子会“苏醒”,发育成为产生毒素的细菌。

这就是在“1919 年大橄榄中毒事件”中,被困在加州罐装橄榄中的孢子所发生的情况。此次事件包括一场由底特律工业家默里·赛尔斯 (Murray Sales) 及其妻子主持的、被广泛报道的晚餐会,该晚餐会导致这对夫妇的两个孩子、一名宾客和两名女佣死亡。另外两个州的九个人也因此丧生。

这些悲剧对新兴的罐头食品工业构成了重大威胁,并引发了新一轮的微生物学研究。参与这场斗争的研究人员中包括加利福尼亚大学的细菌学家伊万·克利福德·霍尔 (Ivan Clifford Hall),他收集了一系列肉毒杆菌的分离株。

其中一个被命名为 Hall A 的菌株成为了实验室的“主力军”,被反复传代。在这个过程中,它被“驯化”了——就像无数其他植物、动物和微生物一样,被人类驱动的进化所重塑。 Hall A

伊万·克利福德·霍尔收集了许多肉毒杆菌菌株,其中包括现在被称为 Hall A 的实验室主力菌株。

失去了形成孢子的能力,这使得科学家更容易纯化 BoNT,并且能产生极高水平的毒素。这些特性使霍尔的菌株成为美国军事研究人员的最爱,他们于 1942 年开始利用它制造生物武器和肉毒杆菌疫苗。

军方将 Hall A 分享给了他人。20 世纪 60 年代初,美国中央情报局 (CIA) 发起了一项阴谋(最终被取消),试图通过在菲德尔·卡斯特罗的一盒雪茄中掺入 BoNT 来暗杀这位古巴领导人。大约在同一时间,一名军事研究人员在搬到威斯康星大学时带走了一份 Hall A 亚培养物,并将其分享给了一位加州的眼科医生。该医生开始进行猴子实验,以观察 BoNT 是否能放松眼部肌肉,希望能找到

治疗眼球失调(一种称为斜视的病症)的方法。北亚利桑那大学 (NAU) 的微生物学家保罗·凯姆 (Paul Keim) 是这项新研究的第一作者,他表示:“这确实是一个‘化剑为犁’的故事。”

20 世纪 80 年代,英国微生物学家安迪·皮克特 (Andy Pickett) 等人与制药公司合作发现,由 Hall A 后代产生的极微量 BoNT(仅十亿分之一克)可以治疗人类的斜视。1989 年,美国食品药品监督管理局批准了这种纯化毒素用于治疗该疾病和眼睑痉挛。这种药物现在由数十家公司生产,在被发现能暂时麻痹产生眼周、额头和鼻周线条的面部肌肉后,以商品名 Botox 广为人知。

Pickett 和 Keim 都曾被聘请为专家证人,参与多场围绕 BoNT 所有权和制造秘密的法律争端。为了帮助理清争议菌株之间的差异,Keim 建议律师们还应招募理查德·伦斯基(Richard Lenski),他是密歇根州立大学的一位进化生物学家,曾在 1988 年启动了一项如今著名的实验,旨在追踪 12 个相同的大肠杆菌(Escherichia coli)种群,并记录它们在数十年间的进化过程。(该研究仍在进行中,至今已历经近 85,000 代。)

作为该案件工作的一部分,研究人员根据公开可用的基因组序列以及他们自行测序的序列,构建了肉毒杆菌(C. botulinum)的家族树。PNAS 论文的共同作者伦斯基表示,他们发现 Army Hall A 菌株及其商业后代处于家族树中一个“出乎意料的长分支”上,这表明该谱系中的菌株比其近亲的突变速度快得多。

“这让我想起了我们在大肠杆菌实验中看到的情况,”伦斯基解释道。在那些研究中,一些突变速度开始快于常态的实验室培养菌株,在涉及 DNA 修复的基因中存在缺陷。在伦斯基的建议下,Keim 和北亚利桑那大学(NAU)的微生物基因组学家杰森·萨尔(Jason Sahl)在 Hall A 的近亲菌株中寻找类似的缺陷。果然,他们发现了一个名为 mutS 的基因突变。

Keim 表示,该突变很可能产生于 处理该菌株期间。他说,在自然界中,这种突变可能很快就会消失,但在实验室中却蓬勃发展,部分原因是科学家们更青睐那些表现出该突变效应的肉毒杆菌培养物。mutS 变体防止肉毒杆菌在产生孢子时浪费能量,使其能够良好生长并产生异常大量的毒素。Keim 说,这种细菌的代谢途径现在已被“精细调整,以适应实验室生活,而非自然环境中的生活”。

“这项工作真正填补了一个巨大的知识空白,”现已退休且未直接参与该研究的 Pickett 表示。他很高兴这项研究也让 CMB 受到了关注,在他看来, CMB 是一位无名英雄。尽管 收集的那些“令人惊叹的”厌氧生物样本中的一部分流向了其他实验室,但其中大部分已不复存在。“没有人想要它,”Pickett 说。他认为,揭开 A 菌株的遗传之谜,是对这位基本上是个谜的人的一种“很好的致敬”。

天文学

微波天文台窥探婴儿宇宙

在智利,西蒙斯天文台开始搜寻星系团和宇宙暴胀的迹象 DANIEL CLERY

在智利阿塔卡马沙漠的高处,一组望远镜正瞄准宇宙中最古老的光——宇宙微波背景(CMB),这种光在宇宙大爆炸后仅 380,000 年便发射出来。凭借比早先 CMB 巡天观测更高的灵敏度和更清晰的分辨率,西蒙斯天文台将深化宇宙学家对宇宙组成的理解,并寻找“宇宙暴胀”的迹象,这是一种假设在宇宙最初时刻发生的指数级爆发式扩张。约翰霍普金斯大学的理论物理学家马克·卡米翁科夫斯基(Marc Kamionkowski)表示:“初步来看,它将完成那些(早先的巡天观测)所做的工作,但效果更好。”

宾夕法尼亚大学的共同主任马克·德夫林(Mark Devlin)表示,该天文台远不止是一个简单的 CMB 实验。通过将 CMB 作为背光,该天文台还将研究自光线产生以来宇宙是如何演化的。它将发现数以万计的星系团,并观察整个宇宙历史中物质的分布。德夫林说,数以千计的科学家社区正在等待这些数据。“你必须具有广泛的吸引力。”

地球大气中的水分会阻挡微波,因此观测者通过卫星、气球或在干燥的高地地面上绘制 CMB 图谱。首选地点是南极和

西蒙斯天文台的大口径望远镜将绘制宇宙中最古老的光——宇宙微波背景。

阿塔卡马沙漠。这个耗资 1.2亿美元 的项目主要由西蒙斯基金会资助,已在此建造了三台口径 0.5 米的小口径望远镜,以及一台口径 6 米的大口径望远镜,后者计划于本月开始对其天空巡天观测。

西蒙斯天文台在启动之际,CMB 研究人员正努力适应一个规模大得多的计划实验被取消带来的损失。去年,美国国家科学基金会和能源部停止了对“CMB-S4”实验的支持,这是一个原计划在智利和南极开展的下一代项目,旨在搜寻宇宙暴胀的信号。普林斯顿大学的西蒙斯天文台发言人乔·邓克利(Jo Dunkley)表示:“虽然我们的灵敏度不如原计划的 CMB-S4,但我们涵盖了所有相同的科学目标……而且我们现在就在执行。”

CMB 是超高温婴儿宇宙发出的光辉,它被宇宙膨胀拉伸,现在看起来像是来自所有方向的微弱微波薄雾。其中分布着微小的温度波动,这些波动对应于婴儿宇宙中物质(包括不可见的暗物质)的聚集——这些种子在引力作用下生长,最终形成了由星系、纤维状结构和空洞组成的宇宙网。通过精确测量这些波动,宇宙学家重建了宇宙的基本配方:大约 5% 的普通物质,26% 的暗物质,以及 69% 的暗能量(一种加速宇宙膨胀的神秘力量)。

西蒙斯天文台不仅将完善这些数字,还将利用其 CMB 波动图谱来解决其他问题,包括中微子的质量,这是一种在空间中高速穿行的幽灵粒子。中微子不像低速运动的物质和暗物质那样聚集,因此它们会抑制宇宙网的生长。通过将编码在 CMB 中的早期宇宙模式与后期的物质分布进行比较,西蒙斯的研究人员可以约束这些难以捉摸的粒子的质量。朴茨茅斯大学的宇宙学家塞沙德里·纳达图尔(Seshadri Nadathur)表示:“我们应该能够对这一质量获得一个正向的测量值。”

该天文台还将探测一个被认为甚至早于宇宙微波背景(CMB)的事件:在宇宙诞生后第一秒的一小部分时间内,一次短暂的指数级增长爆发。在那个“宇宙暴胀”的瞬间,宇宙将从小于质子尺寸万亿分之一的大小,迅速膨胀到大约像个沙滩球那么大。暴胀将抹平新生宇宙中的大部分不均匀性,这解释了为什么如今的宇宙在大尺度上如此平滑且均匀,但在小尺度上却包含着星系网。

这种增长爆发会导致时空产生引力波共振,而这些引力波可能会在CMB上留下印记:即光极化中的旋涡。在南极运行一台名为“宇宙河外极化背景成像2”(Background Imaging of Cosmic Extragalactic Polarization 2)的CMB望远镜的研究人员曾宣布在2014年发现了此类旋涡,但一年后在发现大部分信号来自我们银河系中的尘埃后,撤回了这一主张。

西蒙斯天文台希望取得更好的结果。其小口径望远镜经过优化,可观测尺度大于 $1^{\circ}$ 的波动,预计原初极化信号在该尺度上最强。它们还观测多个波长,有助于将旋涡与来自银河系尘埃的极化发射以及来自近宇宙的其他信号区分开来。前两台望远镜在近 2 年前开始观测,第三台则在近期加入。“从现在起,我们应该开始深入挖掘,”邓克利(Dunkley)说。“大约 5 年后,我们或许能够看到 [这些旋涡]。”一些模型表明这可能需要更长时间。

在小望远镜追寻暴胀极化信号的同时,大口径望远镜的 6 米镜面将为CMB的大部分区域创建精细尺度的地图。它将光线汇聚到一个装有 60,000 个探测器的接收器上,这些探测器被冷却至绝对零度以上十分之一度,以记录微弱的CMB信号。

纳达图尔(Nadathur)表示,这些地图可能包含触发暴胀原因的线索。标准版本的暴胀是由一种由名为“暴胀子”(inflaton)的粒子介导的单一场驱动的。但纳达图尔说,“也许在早期宇宙中存在多种相互作用的场”。这两种情景会导致CMB中波动尺寸的不同分布。

西蒙斯天文台的研究人员还将把CMB作为背光。星系之间稀薄气体中的热电子会散射CMB光子,在一种被称为苏尼亚耶夫-泽尔多维奇效应(Sunyaev-Zeldovich effect)的过程中改变其能量。即使在星系过于遥远或微弱而无法被看见时,这种畸变也能作为星系团的标志。此前在阿塔卡马(Atacama)场地的望远镜曾以此方式发现了数千个星系团。德夫林(Devlin)表示,凭借其宽广的视野,西蒙斯天文台应该能探测到多达 40,000 个,包括早期宇宙中的星系团,这些星系团引发了关于宇宙结构形成的问题:“那么早的时候是如何形成如此巨大的物体的?其物理机制又是怎样的?”

研究人员还希望利用一种相关的现象,称为运动学苏尼亚耶夫-泽尔多维奇效应(kinematic Sunyaev-Zeldovich effect),其中移动的气体团会改变流向地球的CMB光子的波长。这种“红移”或“蓝移”可以在没有可见恒星这一常规标志的情况下揭示暗物质的存在。卡米翁科夫斯基(Kamionkowski)说:“我们一直假设暗物质和 [普通物质] 在早期宇宙中的分布方式相同。现在我们将能够对此进行测试。”

德夫林期待利用该设施开展除研究CMB之外的更多工作。“我觉得我们现在正在服务于一个以前无法接触的群体。这也非常有意思。” □

生态学 深海生物仍深受 BP 原油泄漏事故影响

一项为期 13 年的研究表明,墨西哥湾生态系统仍未恢复 ERIK STOKSTAD

2010 年,深水地平线(Deepwater Horizon)钻井平台发生致命的喷出事故,原油涌入墨西哥湾,一支应急响应团队尝试了一项前所未有的策略。他们派遣机器人潜水器前往水下 1500 米的井口,注入化学分散剂,将原油分解成微小液滴并使其溶解。人们希望通过稀释原油,这种方法能最大限度地减少对野生动物的伤害。这一举措可能使许多海鸟、海龟和浅水鱼类免受原油的影响,否则原油会在海面聚集。但这可能给深海带来了意想不到的代价。

一项始于泄漏次年的 13 年调查发现,墨西哥湾深水区的鱼类、甲壳类动物和头足类动物数量出现了剧烈且持续的下降。该团队本周在《美国国家科学院院刊》(Proceedings of the National Academy of Sciences)上得出结论,最可能的原因是原油泄漏,尽管研究并未直接指责分散剂。

“他们见证了一个我们原以为是孤立且或许受到保护的生态系统发生了重大变化,”蒙特雷湾水族馆研究中心的海洋生态学家 Bruce Robison 表示,他没有参与这项研究。“我只是不知道该系统本身是否具有足够的韧性来恢复,”他说,“这是一个巨大的问号。”

这项研究始于灾难发生 10 个月后,该灾难导致 BP 原油钻井平台上的 11 名船员死亡,并释放了 500 万 桶原油。诺瓦东南大学的生物海洋学家 Tracey Sutton 作为联邦调查泄漏损害工作的一部分,组织了一次深海生态系统调查。从 2011, 2 月开始,该团队利用配备声纳的研究船收集数据,从而能够估算鱼群和甲壳类动物的丰度。研究人员还在墨西哥湾周围的 46 个地点投放拖网,捕捉不同深度的海洋生物。他们分昼夜班工作,捕获并清点了约 1200 个物种,以创建泄漏后生态系统的快照。

当团队 4 年后返回时,希望看到恢复的迹象。相反,研究人员发现了进一步的剧烈下降。调查中三大动物类群——鱼类、甲壳类动物和头足类动物——的数量远低于 2011. 记录的水平。在随后的调查中,情况也没有好转。直到 2023 年,数量依然顽固地处于低位。

深海鱼类,例如这种蛇牙鱼,数量出现了剧烈下降。

鱼类种群的下降幅度最大,与 2011 年相比下降了 64%。由于团队没有泄漏前的基准数据,实际下降幅度可能比报告的还要大。

该团队没有测量生态系统中目前还残留多少原油。但他们怀疑,在泄漏很久之后,原油仍通过食物网持续产生影响。灾难发生多年后,研究共同作者、南卡罗来纳大学的化学海洋学家 Isabel Romero 在深海鱼类的卵和组织中发现了多环芳烃——原油中一种毒性极强的成分。

“这是一个令人警醒的例子,展示了人类在海上活动所带来的意外后果,”领导国家海洋哺乳动物基金会的保护兽医 Cynthia Smith 表示,她没有参与这项工作。夏威夷大学马诺阿分校的海洋生态学家 Jeffrey Drazen 对此次调查的规模印象尤为深刻,该调查涉及使用拖网采集 2000 次样本,且深度通常超过 1 公里。“这是在中层带(mesopelagic realm)开展的最全面的采样工作之一。”

这对于更靠近表层的生物也产生了影响。灯笼鱼(一种眼睛大且带有蓝色、黄色和绿色发光斑块的小鱼)经历了最剧烈的数量下降。这些鱼白天在深海中生活,夜晚向上迁移以捕食浮游动物,而它们反过来又被金枪鱼、剑鱼和鲸鱼捕食。灯笼鱼的匮乏,加上许多幸存者可能被碳氢化合物污染,这或许可以解释近期该海湾中鲸鱼数量下降的原因。例如,抹香鲸在当地的出现频率比原油泄漏前减少了约 30%。

南佛罗里达大学的海洋生态学家 Steven Murawski 对缺乏恢复迹象感到惊讶。他认为,来自附近种群(例如在海湾西部或南部)的动物迁入应当能增强该枯竭区域的种群数量。他说:“从原油泄漏的影响范围到海湾中更广泛的整体群落,一定存在某种级联效应。”

Smith 表示,这项新研究强化了在原油泄漏中审视何时以及是否使用分散剂的必要性。“这些决定应当考虑到原油泄漏影响范围内从海面到海床的所有动物。”

作者们还表示,这对于深海中的其他工业活动(如海底采矿)也是一个警示。佛罗里达国际大学的进化生物学家、共同作者 Heather Bracken-Grissom 说:“人们一直认为深海环境中的种群数量丰富且不会受到伤害。”但研究表明事实并非如此。Sutton 说:“深海是一个比我们想象中脆弱得多的系统。” □

地球物理学

地球核心的铁可能呈现出令人惊讶的形式

X射线实验揭示了可能使内核图像复杂化的立方晶体 PAUL VOOSEN

四年前,十几位科学家挤在德国欧洲X射线自由电子激光(XFEL)设施的一个控制室里。一片比人类头发还细的铁片被挤压在金刚石砧尖之间,承受着深层地球的压力,然后被X射线激光加热至极高温度。领导这项名为 HotCores 且耗资 $2.500 万 的项目的里尔大学地球物理学家 Sébastien Merkel 表示,控制台上出现了一幅令人惊讶的图像。铁的晶体结构是立方体的——这是该排列首次在产生地球磁场的发电机区域被观察到。“如果结构不同,那么性质也会不同,”罗切斯特大学的高压研究员 Shuai Zhang 说道。

这项发现很难发表。Merkel 表示,在被几本知名期刊拒绝后,它最终于 8 月发表在《物理评论 B》(Physical Review B)杂志上。这种延迟可能反映出人们对于重新探讨一个许多研究人员认为已经解决的问题存在抵触心理。然而,对于劳伦斯利弗莫尔国家实验室的材料物理学家 Jon Eggert 来说,“数据非常清晰。我确信他们看到了 BCC(体心立方结构)。”

---

它重新开启了一个我认为已经结束的话题。

Sébastien Merkel

里尔大学

如此高的压力和温度。Merkel 表示,结果似乎是不可能的。“这真的是我们最没想到的,”他说,“它重新开启了一个我认为已经结束的话题。”

几十年来,针对地球内核(一个位于地表下方约 5000 公里的固体铁异世界)的实验和计算机模拟表明,那里的铁原子形成了紧密堆积的六方结构。但这一新结果的消息已在规模较小的内核研究群体中悄然引起波动。如果其结构实际上是通常所说的体心立方(BCC),这可能会改变热传导方式,从而改变地质历史上内核开始凝固的时间,以及热量和元素释放到熔融外核的方式。这些过程影响着外核的翻腾方式,从而驱动

试图模拟地球深处极端压力和温度的实验伴随着严重的复杂性。金刚石压砧单元可以产生深地压力,但可能会引入改变铁结构的杂质;而传统的激光实验可以将样本加热到高温,但仅能维持极短的一瞬——时间太短,无法进行进一步测量。

通过将 XFEL 与金刚石单元相结合,HotCores 团队可以用重复的、30-femtosecond x-ray pulses 轰击样本。Merkel 说,X 射线同时充当“泵浦和探测”的角色。每个脉冲加热样本,且 X 射线在原子上散射以产生其排列的快照——即衍射图样。

起初,快照显示出预期的六方结构。但 Merkel 说,一旦压力和温度升至 229 万 个大气压和约 $5700^{\circ}\mathrm{C}$ 以上,一个清晰的立方信号便出现了。这一发现并非定论。在随后的样本中,由于金刚石单元无法达到相同的压力,尝试重复该结果的努力失败了。而且尚未发表的

新闻

研究人员准备一片铁片,以便对其进行加热和挤压,使其达到类似地核的条件。

使用传统激光冲击技术的实验仅产生了六方铁。

然而,马德里康普顿斯大学的地球物理学家 Maurizio Mattesini 觉得这一结果证明了他的观点。“我忍受了这么长时间,”他说。Mattesini 认为,只有立方铁才能解释穿过内核的地震波中观察到的一些特征,例如出人意料的低速。BCC 的结构比六方铁更松散、刚性更低,会阻碍波的传播,就像软沙减缓跑者的速度一样。但其他建模者也发现了更致密的六方铁同样能减缓地震波的合理方式。

厦门大学的矿物物理学家 Yang Sun 及其同事在 2021 年发表的一篇论文中提出,内核中凝固的铁在最终稳定为六方形式之前,会先结晶成立方结构。“首先形成的相不一定是最终占据主导地位的相,”Sun 说。该模型可以解释为什么 HotCores 团队看到了 BCC 而激光实验没有。样本随每个激光脉冲加热和冷却,使瞬态立方相有时间出现。而在传统的激光冲击实验中,样本经历的是单次剧烈的加热事件。

卡内基科学研究所的矿物物理学家 Sally June Tracy 表示,由于六方相和立方相可以在如此相似的条件下形成,它们可能同时存在于内核中。她说,内核中的微小变化——例如少量的额外镍和其他轻元素——可能会使平衡向立方相偏移。事实上,Merkel 的团队随后开始使用 X 射线激光测试这些合金。尽管这项工作尚未发表,但他说他的团队发现,含有镍和硅的铁倾向于稳定在立方形式。

Merkel补充道,HotCores对立方铁的发现具有一种讽刺意味。该团队在资助申请书的前几行中明确写道,地核中的铁是六方结构的。但现在,地球核心地带究竟存在什么再次变得不确定了。“地核中正在发生什么?”Merkel说,“我不知道。”

科学共同体

被解雇的生物学家在诽谤诉讼中获赔 600万美元

陪审团做出有利于大卫·萨巴蒂尼(David Sabatini)的裁决,驳回了原告关于性骚扰和报复的指控 PHIE JACOBS

生物学家大卫·萨巴蒂尼在 5 年前因一项调查发现其违反了性骚扰政策而导致显赫的职业生涯崩塌。

上周,马萨诸塞州的一个陪审团在萨巴蒂尼起诉前同事、怀特海德生物医学研究所(Whitehead Institute for Biomedical Research)前研究员克里斯汀·诺斯(Kristin Knouse)的诽谤案中,裁定诺斯需向其支付 600万美元(外加利息)的损害赔偿金,这使他获得了一次重大胜利。诺斯指控他对其进行性骚扰,这导致一家研究机构解雇了萨巴蒂尼,并促使他从怀特海德研究所以及他担任终身教职的马萨诸塞理工学院(MIT)辞职。

萨巴蒂尼告诉《Science》,在 16 October 裁决之前的几个小时是“我人生中最紧张的时刻”。对他而言,陪审团的决定代表了“一次明确的洗刷”,带给他“巨大的解脱感”。陪审团还驳回了诺斯关于性骚扰和报复的反诉。

这一结果令一些法律专家感到意外,部分原因是此前两名法官已经驳回了萨巴蒂尼针对怀特海德研究所及其所长露丝·莱曼(Ruth Lehmann)提出的指控,甚至驳回了他针对诺斯提出的一些指控。在调查了萨巴蒂尼的行为后,怀特海德研究所在 2021, 得出结论,认为他违反了该研究所关于合意关系的政策及其反骚扰政策。萨巴蒂尼在担任怀特海德研究所副所长期间结识了诺斯,而诺斯当时是哈佛大学和马萨诸塞理工学院的医学博士-哲学博士(M.D.-Ph.D.)学生,萨巴蒂尼是她的指导教师之一,并担任其论文委员会成员。在诺斯作为研究员加入怀特海德研究所并建立自己的实验室之前,两人开始了性关系。

尽管诺斯表示她是被当时担任怀特海德研究员计划(Whitehead Fellows Program)主任的萨巴蒂尼强迫进入这段关系的,但萨巴蒂尼坚称这是合意的。他主张,诺斯是在他为了追求另一个女人而与她分手后才提出骚扰指控的。萨福克县(Suffolk County)的陪审团现在做出了有利于他的裁决,认定诺斯诽谤了萨巴蒂尼并干扰了他的工作能力。

“这是一个相当重大的认定,”专门处理性骚扰案件的律师安·奥利瓦里乌斯(Ann Olivarius)表示,“显然,陪审团在很大程度上完全站在了他的这一边。”奥利瓦里乌斯对陪审团授予萨巴蒂尼如此巨额的损害赔偿金也感到惊讶。“这非常罕见。这是一个极其突出的案例。”

尽管萨巴蒂尼及其支持者将其视为洗清冤屈,但该民事诉讼的裁决对怀特海德研究所调查的结论没有直接影响。一些人,包括亿万富翁比尔·阿克曼(Bill Ackman)——他利用其庞大的社交媒体平台为萨巴蒂尼辩护并资助其近期的研究——呼吁该研究所重新考虑其调查结果,并要求莱曼辞职。

诺斯的律师艾伦·祖克(Ellen Zucker)告诉《Science》,她的当事人打算对该决定提出上诉。“这一裁决令人深感失望,”她说,并指出其他几名女性在法庭上作证,讲述了与萨巴蒂尼之间“令人担忧的互动”。祖克认为,要求一名职业生涯早期的科学家支付超过 600万美元 的赔偿金,“充分证明陪审团不具备在本案中做出适当决定的能力”。

萨巴蒂尼因研究调节细胞生长和代谢且在癌症等疾病中发生故障的分子信号通路而声名鹊起。在怀特海德研究所,他获得了霍华德·休斯医学研究所(HHMI)研究员这一显赫职位。2021 年,在一次员工调查发现萨巴蒂尼实验室存在问题后,怀特海德研究所聘请了一家外部律师事务所进行调查。

除了发现萨巴蒂尼(Sabatini)与诺斯(Knouse)违反了研究所关于性关系的规定外,调查还得出结论,认为萨巴蒂尼营造了一个性化的实验室环境,并试图通过误导调查人员以及企图操纵受访者的证词来影响调查。作为其正式雇主,HHMI解雇了萨巴蒂尼,后者同时也放弃了在怀特海德(Whitehead)的职位和实验室。在三位高级官员建议撤销其终身教职后,萨巴蒂尼随后从麻省理工学院(MIT)辞职。

萨巴蒂尼的律师丽莎·阿罗伍德(Lisa Arrowood)表示,这位曾经风光无限的生物学家“在科学界成了彻头彻尾的弃儿”。此后,萨巴蒂尼一直努力重启其职业生涯。2023年,阿克曼(Ackman)和一名匿名捐赠者承诺出资共计$25 million以重启他的实验室。同年晚些时候,萨巴蒂尼在捷克科学院有机化学与生物化学研究所就职。该研究所最近在波士顿地区开设了一个分部,萨巴蒂尼目前在那里拥有实验室空间。

2024年,美国卫生与公众服务部(HHS)宣布,由于相关指控,该部门正寻求禁止其获得任何联邦研究资金。萨巴蒂尼确认,2025年9月,该机构确实禁止他领取美国国立卫生研究院(NIH)的资助,期限为1年。但根据萨巴蒂尼提供给《科学》(Science)的一封HHS电子邮件,该禁令在4月被提前终止。

萨巴蒂尼辩称,他与诺斯之间不存在权力失衡。阿罗伍德在谈到诺斯时说:“她有自己的实验室,有自己的资金,有自己的学生。”但奥利瓦里乌斯(Olivarius)认为,萨巴蒂尼对诺斯——一位处于职业生涯早期且年轻得多的同事——不持有权力地位的观点十分“荒谬”。“看看他是谁,再看看她是谁……这不是一段平等的关系。”

然而,麻省理工学院的计算机科学家雷吉娜·巴齐莱(Regina Barzilay)自称是萨巴蒂尼的朋友和同事,她表示最初的怀特海德调查“极其片面”,并且她对萨巴蒂尼赢得诉讼感到“欣喜若狂”。

但对于祖克(Zucker)来说,针对其客户的裁决象征着更广泛的文化问题:“在我看来,这次审判和陪审团的裁决是我们这个时代的悲哀标志,在这个时代,女性依然很难被相信,而让权势人物承担责任则更加困难。”

他的律师表示,萨巴蒂尼计划就此前针对怀特海德和莱曼(Lehmann)主张的被简易驳回申请提出上诉,这些主张包括诽谤,以及因对方采信诺斯而非他的陈述而构成的性别歧视。根据奥利瓦里乌斯的说法,他与诺斯可能都面临一场艰苦的战斗。“上诉总是很难获胜。” □

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持久的余震

2004年印尼在一次海底地震后遭遇的海啸导致170,000人死亡,并迫使超过50万人离开家园。一项新研究发现,在20年多之后,目睹了这场毁灭性灾难的人们可能会产生持久的健康影响,包括代谢失衡。在上个月发布于预印本服务器 bioRxiv 的一项研究中,研究人员追踪了3270人的甲状腺激素水平和其他健康指标,这些人员所属的家庭在灾难发生前就拥有基线数据。该团队发现,在受海啸影响最严重地区的人群中,甲状腺激素水平较低,且肥胖率更高、胆固醇更高,以及其他代谢健康状况不佳的指标。研究人员得出结论,由这场毁灭性灾难引起的压力——其中部分景象如图所示,为海啸发生2天后在班达亚齐的一座清真寺拍摄——可能永久性地改变了该激素调节生理功能的能力。——Sara Reardon

EYES ON THE BALL

一款在美国职业棒球大联盟中判定好球与坏球的“机器人裁判”本周在世界大赛首次亮相。它必须近乎完美

乔恩·科恩(JON COHEN),发自圣迭戈佩特科公园球场

10月 8 日上午 6 点,凯尔·韦特(Kyle Wait)和泰勒·丹比(Tyler Danby)将装满设备的 Pelican 运输箱和行李袋拖进了圣迭戈教徒队的主场。在前一天晚上,该队在这里输掉了一场令人心碎的比赛,使 47,712 名欢呼的球迷陷入沉默,教徒队也因此被淘汰出季后赛。

除了 2 打被称为“珍珠”的崭新棒球外,这两个男人没有带任何棒球装备进入依然昏暗的球场。但他们携带的高速摄像机、三脚架、激光器、直尺、铅垂线、雷达,以及一台定制的活塞动力发球炮,与每一个比赛中的关键问题都息息相关:一次投球是否在好球区内(以恰好正确的高度和深度穿过本垒板),还是脱离了该区域——即坏球。

美国职业棒球大联盟在 2025 年的春季训练期间测试了其自动好坏球挑战系统。

韦特和丹比都就职于华盛顿州立大学(WSU)由劳埃德·史密斯(Lloyd Smith)运行的体育科学实验室。他们担心球场的昏暗(大多数灯塔都关闭了),以及清理人员使用高压清洗机产生的带有啤酒味的雾气。应美国职业棒球大联盟的邀请,他们即将对今年推出的一项技术进行“地面真值”校验,这项技术代表了 MLB 123 年历史上最大的变革之一:自动好坏球(ABS)挑战系统,更常被称为“机器人裁判”。而他们的摄像机每台成本超过 $100,000,需要充足的光线且极其忌讳潮湿。

在经过一连串的电子邮件和电话沟通后,体育场灯光开始亮起。清洁工撤离。工作开始了。

在接下来的 3 小时里,两人拍摄了 100 个以约 90 英里时速穿过本垒板的炮击“珍珠”,他们将把这些图像带回 WSU 进行分析,以校准该球场基于摄像机的 ABS 系统。(《科学》杂志的风格是使用公制单位,但棒球运动显然不这么做。)“我热爱做这个,”韦特说道,他曾是一名野生动物生态学家,曾使用摄像机追踪食肉动物,并担任地面真值专家为 MLB 的 30 个体育场进行校验已有 7 年时间。“完善我们的方法就是一场持久战,”丹比说。

棒球的核心对抗发生在投手和击球手之间,但在这一戏剧中还有另一个重要角色——本垒板裁判,他必须在瞬间决定一次未被击中的投球是好球还是坏球。在过去,球员和经理在官方层面上无法对裁判的决定提出挑战。但这并没有阻止成年人在不同意判罚时咒骂、剧烈地挥动手臂,并像被宠坏的孩子一样表现,甚至冒着被驱逐出场的风险。鉴于三次好球意味着击球手出局,而四次坏球则让他们获得保送上垒,因此判罚的利害关系极高。

即使是裁判也知道判罚经常出错——在 2022 年的一场比赛中就出现了 19 次误判,而一名明星强击手因判罚错误而大发雷霆,使这场比赛格外令人难忘。因此,MLB 采用了由 Hawk-Eye Innovations 制造的 ABS 系统,该系统利用球场周围的五台摄像机来核查裁判的判罚。对于一个年营收 120 亿美元 billion 的行业,比赛结果、职业生涯以及数十亿赌注都取决于投球命运,该系统必须近乎完美。“人们会问:‘我们知道你们用 Hawk-Eye 来给裁判打分,但谁给 Hawk-Eye 打分?’”MLB 的棒球科学家、电气工程师克莱·纳纳利(Clay Nunnally)说,“WSU 给 Hawk-Eye 打分。”

借助美国职业棒球大联盟(MLB)的ABS系统,投手、捕手或击球手现在可以通过在2秒内轻敲头盔或球帽顶部,对裁判关于好球或坏球的判定提出挑战。几秒钟后,投球的轨迹会以慢动作形式出现在体育场的巨型屏幕上,显示棒球在经过本垒板中点时的精确位置(见第376页图表)。球队在比赛开始时仅有两次挑战机会,只有在判定被推翻的情况下,挑战机会才会保留。

今年MLB常规赛出现了10,557次好球或坏球挑战,而修正后的判定显著改变了比赛进程。三周前,一场加时赛季后赛在一次ABS申诉中结束,该申诉将一次判定为坏球的球变成了第三次好球(三振)。当判定被推翻时,球迷有时会陷入疯狂。但“机器人裁判”平息了场上的情绪:因好坏球争议而被驱逐的人数从上赛季的110人骤降至11, 因为数字证据给争论留下的空间更小。

追踪一个在不到60英尺的距离内、速度并不比高速公路上的汽车快多少的球,对于当今的技术来说似乎是一项简单的任务。但由于赌注极高,哪怕是几分之一个英寸的精度也至关重要。两种由雷达工程师和计算机科学家分别为不同运动开发的ABS方案曾竞争大联盟的订单,最终Hawk-Eye险胜其竞争对手。而且,令人惊讶的变量可能会改变每个系统的准确性。“追踪球并确定其位置并非易事,”史密斯说,“有很多因素在起作用。”

在1903, MLB成立之初,好球区是一个三维概念。如果棒球在球员膝盖以上、肩膀以下跨过本垒板的任何部分,即被视为进入好球区。然而,对于今年的Hawk-Eye ABS系统,好球区是本垒板中心的一个二维平面,并根据每位球员的身高进行调整。MLB在赛季开始时测量每位球员不穿鞋的身高。测量通过手动(使用身高计或滑动墙尺)和激光两种方式完成。测量时间定在10 a.m.到12 p.m.之间,以避免一天之中发生的脊柱压缩。

ABS系统不仅仅是在球经过本垒时捕捉它:它们还追踪球在飞向本垒板的半秒旅程中的初始位置、速度和加速度,从而计算其向好球区的轨迹。退休粒子物理学家艾伦·内森(Alan Nathan)表示:“通过使用完整轨迹而非单个点,可以提高测量的整体精度。”内森是史密斯的合作者,并维护着一个名为“棒球物理学”的网站。

投球追踪技术在20年前首次进入MLB球场,但最初仅是为了帮助教练和球员提高投球和击球水平。在过去的5年里,它一直被用作MLB小联盟的ABS系统。“在将任何东西引入大联盟之前,我们会对其进行相当充分的测试,”前MLB投手、现任组织副总裁乔·马丁内斯(Joe Martinez)说道。

早期的双摄像头ABS系统PITCHf / x在2006年至15, 间被用于小联盟,该系统声称精度可达半英寸,并让电视观众习惯于观察球是否真正处于好球区。但随后,来自丹麦的电气工程师弗雷德里克·图森(Fredrik Tuxen)提供了一项更精确的技术,而他在成长过程中对棒球一窍不通。

图森曾帮助军方开发用于追踪导弹的多普勒雷达。高尔夫练习场的业主找到他,询问他是否能创建一种多普勒设备来测量球的距离。作为一名忠实的高尔夫球手,图森早就知道这是可行的:10年前,当他在美国陆军尤马试验场完成导弹探测雷达测试后,曾在那里挥杆。他说:“在2小时后,我成功追踪到了一个高尔夫球,但问题是我用的是一台$2 million雷达。”

在可以通过敲击头部来挑战裁判对“好球”或“坏球”判定的人员中,投手的成功率最低。

这促使 Tuxen 在 2003 年共同创立了一家名为 Trackman 的公司,该公司开发了一种廉价得多的雷达,它可以装进一个大型手提箱,但依然能够追踪高尔夫球。销售额随即激增。“人们立刻说:‘嘿,伙计们,你们得把这个引入棒球,他们对数据简直痴迷,’”他回忆道。

Trackman 系统发出大约 24,000 个无线电波脉冲

裁判对好球的看法与摄像机的看法不同。

捕手在挑战中的成功率最高。

在区域内

ABS 好球被定义为:在球员调整的高度范围内,且在 17" 宽度之内,穿过本垒板中点的一球。

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裁判的裁判

美国职业棒球大联盟(Major League Baseball)本赛季引入的基于摄像头的自动球好坏判定(ABS)挑战系统,允许投手、捕手或击球手对裁判的投球判定提出质疑。

在投球短暂的飞行过程中,接收器捕捉球的反射信号,从而揭示其速度、位置,并且通过追踪球的缝线来确定其旋转速度。旋转产生的空气动力学力量(即马格努斯效应)可以通过使球偏离直线路径来欺骗击球手。许多球员和教练起初并未立即意识到这台机器的价值。Tuxen 表示:“多年来,球员们一直凭眼睛观察并讨论‘球质’——比如‘这是一个很阴险的球’之类的话——但对我这个工程师来说,这没有意义。我需要数据。”

到 2010 年,Trackman 提供了这些数据,将科学引入了投球这项艺术。例如,它显示一名 MLB 投手的平均曲球旋转速度为 2450 转 / 分钟 (rpm),并揭示了其翻滚或扭转的程度。投手们首次了解到,旋转速度超过 2600 rpm 的曲球更有可能诱使击球手挥棒落空——即判定为好球。

Trackman 最初为 MLB 的转播提供娱乐功能,用于区分投球类型(肉眼很难分辨切球和滑球)以及飞行轨迹和投球位置。为了改进 Trackman,Tuxen 聘请了 Smith 的团队来进行地面真值验证。

---

观点

由 Hawk-Eye Innovations 设计的 ABS 系统依赖于球场周围的五台高速摄像机。由于投球速度可超过 100 英里 / 小时,摄像机可能无法捕捉到棒球穿过本垒板中心点的确切瞬间,因此 Hawk-Eye 在判定投球是好球还是坏球的计算公式中加入了球的轨迹。

随后,美国职业棒球大联盟(MLB)决定使用 ABS 系统来评估裁判。“这就是我参与进来的时候,”史密斯(Smith)说道,“如果你打算用这个来评估人员,特别是如果涉及工会,你必须有一个独立的系统来证明这确实有效。”

图克森(Tuxen)很高兴地看到“机器人裁判”在这项运动中获得认可。“当你面对像棒球这样一项拥有深厚文化底蕴的古老运动,包括拥有裁判这一传统时,这很有趣,”图克森说,“现在现代技术与之相遇。你该如何架起这座桥梁?”

许多从事 ABS 系统工作的人本身就打棒球,但史密斯除外。“我可能会被投票选为最不像运动员的人,”他说。他是凭借在复合材料方面的专业知识进入这个领域的。通过与终身业余球员内森(Nathan)合作,他开始研究不同种类球棒(木制、金属和复合材料)的性能。这项工作涉及将棒球发射向静止的球棒,史密斯因此深深着迷。“我算是偶然进入这个领域的,但我发现这项研究非常有趣,而且谁不喜欢一份制造大炮的职业呢?”他说。

MLB 仅允许使用木制球棒,但大学和其他联赛允许使用其他材料。那个市场规模很大,来自球棒研究的收入让史密斯能够创建 WSU 体育实验室,该实验室拥有近 20 名员工。他们共同在从《体育工程》(Sports Engineering)到《复合材料结构》(Composite Structures)等期刊上发表了 50 多篇关于棒球和垒球的论文。有 20 多名研究生在此完成了论文,研究对象涵盖板球拍、冰球杆、羽毛球阻力、跆拳道,以及棒球中最奇特的投球——指球(knuckleball)的空气动力学。

当史密斯开始评估 Trackman 时,他的团队很快发现一些细微因素会影响雷达结果。例如,满场观众的重量会导致体育场下沉。“雷达的方向可能会改变 100 分之一度,但这在本垒板处会转化为几英寸的偏差,而几英寸在棒球中至关重要,”图克森说。

为了提高精度,Trackman 在其系统中增加了一台摄像机,用光学数据补充雷达数据。2015 年,MLB 在推出自有数据分析平台 Statcast 的同时,将 NIH 安装在所有 30 个球场中。 NIH 的数据帮助球队评估未来的球员,一些职业投手还购买了设备来磨练他们的“球路”(stuff)。韩国和日本的职业棒球队伍也开始将该雷达系统用于分析。

然而,直到 2019 年,MLB 才将 NIH 作为机器人裁判进行测试,次年,它切换到了完全依赖摄像机追踪球的 -。MLB 没有直接就这一决定发表评论,但 - 的精度相当,可能更便宜,且能提供更多信息。图克森承认,在当时,“它要先进得多”。

  • 是一家总部位于英国的公司,由计算机科学家保罗·霍金斯(Paul Hawkins)于 2001 年创立,最初旨在判定他最热爱的板球运动中的困难判罚。10 年后被索尼(Sony)收购,- 现在被用于约 20 项运动,包括网球、足球、美式足球和橄榄球。对于棒球,- 最初依赖 10 台摄像机,但随后增加了第 11 台以检测球的旋转,之后又增加了一台,仅仅是因为计算机能够处理其数据。部分摄像机追踪球员的移动,但有五台专注于球,以每秒 300 帧的速度拍摄其飞行轨迹。“在光学追踪方面,我们现在已经达到了能够测量球缝实际方向的程度,”- 的棒球技术经理马修·盖顿(Matthew Gaydon)说道。

即便如此高的帧率,仍可能无法捕捉到球进入或错过美国职业棒球大联盟(MLB)目前使用的二维好球区的那一刻。“在两次原始测量之间,球大约移动了5英寸,我们必须运气很好才能在好球区正对着本垒板中心平面处获得一次实际测量,”纳纳利(Nunnally)说道。因此,与Trackman一样,Hawk-Eye通过计算轨迹并将其外推至整个好球区。

通过综合分析华盛顿州立大学(WSU)使用Trackman和Hawk-Eye对3000次测试投球进行的评估数据,MLB确定这两个系统的ABS中位数“误差”目前均为0.17英寸。“尽管我们称之为‘误差’,但它更多是对不确定性的衡量,”纳纳利说道。

许多因素都会降低Hawk-Eye的性能,MLB今年在比赛期间不得不八次暂停其ABS系统。由于剧烈的高温、球场下方地面的偏移,或者因为雨、雾或海雾而在比赛期间清洗镜头,Hawk-Eye的摄像机可能会出现对齐偏差。这就是为什么WSU的团队来到佩特科球场(Petco Park),以评估Hawk-Eye的五台ABS摄像机——其中四台安装在好球区后方最高层看台(nosebleed section)上方的横梁上,一台在外野——的耐用情况。

在佩特科球场的一次地面真值测试中,泰勒·丹比(Tyler Danby)用投球机向本垒板发射一颗快球。

测试人员使用了两台自己的摄像机,其每秒2500帧的运行速度远快于ABS摄像机。在利用水平仪、激光仪和铅垂线在本垒板处精确计算出三维好球区的高度、宽度和深度后,韦特(Wait)和丹比记录了投球机在投手丘上发射的100次投球,每次投球都伴随着一声巨响和一团冷凝雾,这是由于压缩空气膨胀并冷却所致。在亚特兰大的Hawk-Eye控制室里,技术人员同步运行佩特科球场的ABS摄像机。如有必要,技术人员可以远程调整焦距,以应对云层或太阳引起的光线变化,他们在本赛季MLB的所有24 30场比赛中都这样做了。

地面真值测试的目标是测试系统测量位置、速度和旋转的准确度。丹比调整投球机爪心中的每个球的位置,以便摄像机能够追踪球上的缝线和印刷文字,包括被两颗星包围的“OFFICIAL”字样。“为了测量旋转率,我们追踪表面标记,”韦特解释道。

WSU团队将计算其坐标与Hawk-Eye摄像机记录的坐标之间的“偏移量”,但这种学术性的球位评估速度远慢于ABS系统在实时比赛中的速度。“疯狂的是,球刚投出,他们就立刻知道了[好球区位置],”韦特说。“而我们这样做,我得在下周才能告诉你答案。”

随后,Hawk-Eye将调整其摄像机以修正不精确之处。

盖顿(Gaydon)认为,自动化裁判革命才刚刚开始。他预计Hawk-Eye技术将普及到高中比赛甚至少棒联盟(Little League)赛事中,由固定位置的智能手机提供摄像功能。“我迫不及待想看到那样的一天:一个在9岁孩子身上倾注了所有心血的家长开始与可怜的裁判争论,而裁判说:‘判定不是我做的,是上面那台摄像机做的,’”盖顿说道。

除了让裁判的工作减少争议外,ABS系统还给他们带来了一些令人振奋的消息。MLB将人工投球判定与自动判定进行对比显示,本赛季人工裁判的正确率达到了93.5%。前MLB投手马丁内斯(Martinez)对此并不感到惊讶。“每个人,现在比以往任何时候都更能体会裁判在后方所做的工作。” □

前FBI反情报特工谭道(Tam Dao)现在在莱斯大学从事研究安全工作。378

煽动者

一名 FBI 特工促使美国国立卫生研究院(NIH)开展针对美国校园外国干预的行动。现在,他正在研究该问题的严重程度 JEFFREY MERVIS

在过去的十年里,美国国立卫生研究院(NIH)一直在收集数百名在美科学家的信息, NIH 认为这些人试图非法帮助其原籍国,其中最常见的是中国。但一直不清楚是什么触发了 NIH 对这些科学家的激进追捕——其中许多人最终失去了工作甚至入狱——以及为什么这种追捕比其他联邦机构的努力要广泛得多。

谜底揭晓。《科学》杂志获悉,一名从学术心理学家转行为 FBI 反情报特别特工的 Tam Dao 为 NIH 的这场行动奠定了基础。“我领导了启动这一切的调查,”Dao 表示,在美国与中国竞争全球科学领导地位之际,他首次承认了自己起到的关键作用。

仍然是关于研究安全辩论中的一个重要角色。现在,作为莱斯大学校园安全与研究安全负责人,他将探讨一个在 NIH 贸然行动之前本该被提出的问题:外国政府尝试在大学窃取研究的频率有多高?

“Tam 将[这个问题]引起了我们的注意,”前 校外研究项目负责人 Michael Lauer 表示。他提到从 2014 年开始的几次会议,在会上 告诉 高级官员,他认为 MD Anderson 癌症中心的科学家们违反了 NIH 同行评审过程的保密协议,以造福中国机构的同事。“他拥有他们的电子邮件、短信副本以及电脑,而这些显然是我们无法接触到的,”Lauer 回忆道。

对 MD Anderson 的调查导致三名亚裔科学家在 2019 年被解雇,这是 NIH 在 2012 年至 23 年期间在 FBI 休斯顿分局工作 11 年中所处理的数百起反情报案件之一。他的努力是美国政府一项名为“中国计划”的更广泛行动的一部分,该计划始于 2018 年唐纳德·特朗普总统的第一任期,旨在根除间谍活动。并且他让 NIH 相信,这是一个需要解决的严重问题。

在 NIH 收集并分享的信息的激励下,Lauer 组建了自己的团队,以挖掘更多关于可疑行为的信息,包括未能披露外国关系。这导致数百所美国大学收到了 Lauer 的信函,要求他们调查一名或多名持有 资助的教职员工并采取适当行动。这项工作在接下来的几年中不断扩大,截至 6 月, NIH 表示已发现 238 起未披露隶属关系的案例,其中包括 197 起未报告的资助支持。结果,122 名科学家失去了工作,216 人被禁止担任同行评审员。

在 NIH 继续调查的同时,FBI 的上级机构美国司法部(DOJ)在当时的总统乔·拜登领导下,于 2022 年结束了“中国计划”,因为该部门承认许多人认为该计划不公正地针对了华裔科学家。而 对其方法及其影响的看法则较为复杂。

“我整个[学术]生涯都在开发不会过度诊断或不对亚裔美国人产生偏见的心理健康量表,”他说。“因此,任何关于针对亚裔美国人的指控都触及了我的核心。”

他同意批评者的观点,即“中国计划”损害了许多无辜科学家的名誉,并“阻碍了优秀人才来到美国”。但他也认为,它“通过阻止坏人来到这里……并让国家更安全,对国家的帮助大于伤害”。并且他强烈捍卫政府的策略。

“我很确定外界存在一些种族主义者,他们会将[亚裔]作为目标,”他说。“但 FBI 关注的是个人的行为而非种族,且该行为必须提供我们所谓的‘合理的、可阐明的实事’来支持案件。”

DAO 的个人经历使他成为一个既不像候选人、却又完美契合的人选,去影响政府关于研究安全的政策。他于 1975 年 4 月 5 日出生在当时的西贡,在 4 月 30 日该市被北越军队占领前几天,他与家人被撤离。“我们被告知在特定的时间前往特定的地点,”Dao 回忆道,这是他从父亲那里得知的情况,其父曾是美国政府的翻译。

的家人暂时安置在阿肯色州查菲堡(Fort Chaffee)的一个安置中心,最终定居在休斯顿,在那里他们为了维持生计而苦苦挣扎。他的父母从事最低工资的工作,在暑假期间,他和三个兄弟只能自谋生路。“在今天,这会被认为是虐待儿童,” 说。但他的父母“别无选择”。

他们也将教育放在首位。追随两个哥哥的脚步, NIH 从德克萨斯大学奥斯汀分校(UT Austin)毕业。在从事了一份薪水丰厚但缺乏成就感的房地产管理工作 2 年后,想要为社会做出更大贡献的愿望促使他重返校园,并获得了佛罗里达州立大学的咨询心理学博士学位。2009 年,他加入休斯顿大学教职员工队伍,专门从事人格评估研究。

说,他的系在仅 3 年后就愿意支持他申请终身教职,但他觉得是时候表达他对“这个国家为我的家庭所做的一切”的感激之情了。他申请了 FBI 的工作,尽管他缺乏执法训练——“我甚至不知道怎么开枪”——且已经超过了新特工 37 岁的年龄限制。他获得了年龄豁免,挺过了艰苦的新兵训练营,并于 2012 年被分配到休斯顿 FBI 办公室。几年后,他转入反情报部门,调查在美学术科学家是否可能在帮助外国实体非法获取由美国政府资助的研究成果。

其中一个他最早处理的反情报案件涉及德克萨斯大学系统的 MD 安德森癌症中心。但当 将他的调查结果呈交给时任 NIH 院长 Francis Collins、其首席副院长 Lawrence Tabak 以及 Lauer 时,“我们都相当怀疑是否存在任何问题,”Lauer 回忆道。 NIH 说:“他们说我不具备可信度,并且受 NIH 资助的科学家经过培训,不会做那些事情。”

这种怀疑的一个主要原因是 Lauer 所称的两个机构之间的“文化差距”。“在 FBI 工作的人……来自非常不同的背景,对于世界如何运作有着不同的看法,”

任何关于针对亚裔美国人的指控都触及了我的核心。

Tam Dao,莱斯大学

他解释道。“而且我们不习惯与他们打交道。”

Dao希望利用科学的通用语言——证据——来弥合这一差距。他获得了许可,将他和其他FBI特工收集的信息分享给NIH——Dao表示,这种不寻常的做法需要与他的上司进行数月微妙的谈判。

Dao开展的关于心理健康评估的研究也让他与NIH官员之间建立了一些共识。“他将各种现代统计技术应用于一些问题,而这些问题与我在研究心血管疾病时使用的统计技术非常相似,”Lauer回忆道,他在2007年加入NIH之前曾在克利夫兰诊所工作。“所以这之间有了联系。而且他也是个非常友善的人。”

一旦NIH领导层认同了Dao的结论,Collins就向大约10,000家获得NIH资助的机构发出了一封信。Dao协助起草了这封2018年8月的重磅信函,信中警告称,“NIH意识到,一些外国实体已经启动了系统性计划,旨在影响NIH的研究人员和同行评审员,并利用NIH资助研究活动长期以来秉持的信任、公平和卓越的传统。”

随后,Lauer发出的密集信函促使各大学匆忙调查其教职员工是否参与了NIH所定义的“外国干预”。这一短语涵盖了违反同行评审规则,或受资助者未披露与外国机构关系的违规行为。但许多大学管理人员抱怨说,他们无法获取NIH(通过Dao)已经掌握的关于其相关案例的信息。Dao表示,这种信息不对称导致人们认为亚裔科学家受到了不公正的针对。他再次决定,目前需要的是更高的透明度。

“传统上,FBI会进行自己的调查 [而不涉及相关机构],”Dao解释道。“但当你这样做时,就有产生偏见的风险。我不喜欢那种方法。所以我开始向他们提供机密资料。我会说,‘资料在这里。由你们决定是否出了问题。’”Dao估计,在他担任FBI特工期间,他为300多所大学和医学中心举行了此类简报会。

他认为,与机构分享FBI信息提高了校园内的研究安全性。他说,其中一个重要因素是引入具有专业知识的教职员工,由他们来判定如果发生了违规行为,是否会对国家安全构成威胁。Dao表示,他的FBI同事并不具备此类专业知识。

“大多数特工试图保护他们甚至不理解的东西,”Dao解释道。“例如,量子技术的哪些方面构成了国家安全风险?大多数FBI特工对此毫无头绪。就此而言,我也一样。”

对于两党许多政治人物来说,MD Anderson案例就是充分的证明,证明学术机构在应对感知到的威胁方面做得不够。美国司法部(DOJ)不断发布新闻稿,吹捧对个人提起起诉或与机构就涉及所谓“恶意外国影响”的案件达成和解,这表明问题规模巨大且在不断扩大。

但许多涉及学术人员的案件后来被撤销,或者以政府败诉告终。

Dao目前由美国国家科学基金会(NSF)上个月资助的项目,是量化该问题的首次严谨尝试。这是NSF新设立的“研究安全研究计划”的一部分,该计划由一项2022年的法律授权,赋予该机构更多责任,以提高美国大学和学术医学中心的研究安全性。

Dao及其团队希望调查多达1600名教职员工,将其分为STEM(科学、技术、工程和数学)或非STEM领域,并根据其所在机构每年的研究经费是否超过$50 million进行划分。Dao表示,这些区分可能至关重要。“如果非STEM教职员工中的比例要高得多怎么办?”他问道,“或者如果我们发现这个问题在大多数顶尖机构中很少见怎么办?”

该研究将采用一个关于外国影响的定义,涵盖外国政府四类不当行为:提供激励或奖励、要求任何合作必须保密、强迫科学家参与,以及直接盗窃知识产权。Dao表示,该调查方法可以在不将答案与个人受访者关联的情况下,收集有关任何可疑行为的类型和频率的准确信息。然而,他承认,“中国计划”带来的寒蝉效应可能会使教职员工不愿报告任何接触,更不用说任何失误了。

Dao希望在未来几个月内开展的这项调查结果能够解决他认为的当前关于外国影响的政治辩论中的两个缺陷。一是执法机构的一种固有偏见,即因为他们看到了太多可能违法的行为案例,从而夸大了问题。二是科学家不愿考虑其同行可能做出此类不端行为。

Dao承诺将避免这两种倾向。“了解我的人都知道我是由数据驱动的,”他说。

Lauer则信任Dao能够把握好这个微妙的平衡,并为美国校园受外国影响的情况建立一个基准。“Tam是一个能力极其出色的人,而且他倾向于定量分析,”Lauer说,“所以我认为他是尝试回答这个问题的显然合适人选。”

评论

位于加拿大努纳武特地区巴芬岛的巴恩斯冰帽(Barnes Ice Cap)是大陆冰川的最后残余,自 1960 年以来一直在退缩。

观点

冰川学

下一次冰河时代是否已经到来并结束?

大陆冰川的最后残余表明,全球变暖可能已经阻碍了下一次冰期

Shaun A. Marcott

在过去的 200 万 年里,地球就像节拍器一样,在由其绕太阳运行的行星轨道驱动的可预测“节拍”上经历着冰河时代 (1)。然而,未来的 anthropogenic 温室气体排放可能会给这一循环画上决定性的句号,使下一次冰河时代推迟数十万年 (2)。在本期第 455 页,Young 等人 (3) 报告了加拿大东北部的巴恩斯冰帽在过去 4000 年中应对自然和 anthropogenic 气候变化的历史。该冰帽是劳伦泰德冰盖的最后残余,劳伦泰德冰盖是一座巨大的大陆冰川,在冰期巅峰时曾覆盖了北美近 30% 的面积。研究表明,该冰川在 2000 年前开始生长,但由于工业化前的全球变暖,在 1960 年开始失去冰量,这可能预示着下一次冰河时代的终结。

劳伦泰德冰盖一直随着每个冰河时代循环同步生长和萎缩 (4)。在上次冰盛期巅峰 [约 20,000 年前 (5)],该冰盖覆盖了加拿大大部分地区和美国北部部分地区。相比之下,在目前的间冰期(一个全球平均气温较高的地质纪元)期间,它已基本消失。Young 等人结合使用了多种地质测年技术,以确定巴恩斯冰帽在过去 4000 年中的前进和后退时间。地表暴露测年法是在高山地形中常用的一种方法 (6),用于确定岩石表面暴露在大气和宇宙辐射中的持续时间。裸露的岩石与宇宙射线相互作用,以已知速率稳定地积累稀有同位素,例如铍-10 ($^{10}$ Be)。Young 等人测量了由后退冰川新暴露的基岩表面,以及位于广泛的冰碛网络(由未固结碎片组成的独特脊线)之上的巨石表面的 ${}^{10}$ Be 同位素。所获得的 ${}^{10}$ Be 年龄中,近一半包含从先前宇宙射线暴露中继承的同位素,这在极地或高纬度环境中是一个常见的复杂问题,因为在这些环境中,冰川底部与床岩冻结且侵蚀速度极慢 (7)。Young 等人使用了第二种年代学技术,测量此前被冰封在低侵蚀冰层下方并得以保存的植被中的放射性碳-14 (${}^{14}$ C) 同位素。被冰川覆盖的枯死植被不再吸收 ${}^{14}$ C,从而为冰川覆盖这些物质的时间提供了精确的时间戳。

通过将测得的日期与该地区的先前研究 [例如 (8)] 相结合,Young 等人发现巴恩斯冰帽在约 3600 年前达到最小规模,然后在 2000 年前左右开始重新生长。冰川的前进标志着由夏季入射太阳辐射量减少导致的区域冷却所驱动的下一次冰期的开始 (9)。到 1950 年代末,巴恩斯冰帽达到了其历史最高位置。然而,该冰川的质量平衡在 1960 年转为负值 (10),冰帽开始了其历史性的边缘后退。这次后退标志着遵循常规冰河时代循环的下一次冰期的终结。

Young 等人的研究为冰盖如何响应气候变化提供了一个重要的基准,可能为先前冰期的开始提供信息 (11)。识别冰期的开始具有挑战性,因为在冰河时代开始时的初始冰体通常太小,无法用传统方法检测到 (12),且很难精准定位大规模冰盖的确切成核位置。Young 等人新获取的时间序列数据提供了一种确定冰期开始的精确时间和速率的方法,展示了冰川对夏季温度变化的响应速度。作者认为,一系列气候反馈(例如海冰的变化),以及逐渐降低的温度,可能有助于加速 2000 年前残余的劳伦泰德冰盖(Laurentide Ice Sheet)的观测到的重新生长。这与之前的研究一致,即认为夏季入射太阳辐射量的变化是过去冰期的一个关键初始驱动因素 (13)。它还强调,其他气候效应,如来自积雪和冰盖的反照率(地表反射的太阳辐射量)变化,在启动冰期开始方面同样重要 (14)。

是否还会发生另一个冰河时代?通常认为在下一个预测周期内不太可能发生下一次冰期开始,但最终跳过多少个冰期循环,取决于人类的选择并与未来的碳排放挂钩 (2)。人类现在已成为地质代理人,能够挫败数百万年的自然冰期循环,并在未来的数十万年里抵消地球的气候。在过去 200 万 年的地质历史背景下,未来冰期循环的缺失将产生深远影响,并将波及与其他冰河时代共同演化的其他生物和物理系统 (15)。随着冰河时代的钟摆停止摆动,Young 等人的研究引发了人们对一个无冰世界意味着什么的深思。

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参考文献与注释

1. J. D. Hays, J. Imbrie, N. J. Shackleton, Science 194, 1121 (1976).

2. D. Archer, A. Ganopolski, Geochem. Geophys. Geosyst. 6, Q05000 (2005).

3. N. E. Young et al., Science 394, 455 (2026).

4. A. S. Dyke et al., Quat. Sci. Rev. 21, 9 (2002).

5. P.U. Clark et al., Science 325, 710 (2009).

6. K. Nishiizumi et al., J. Geophys. Res. 94, 17907 (1989).

7. P.T. Davis, J. P. Briner, R. D. Coulthard, R. W. Finkel, G. H. Miller, Quat. Res. 65, 156 (2006).

8. G.H. Miller et al., Clim. Past 19, 2341 (2023).

9. B. S. Lecavalier et al., Proc. Natl. Acad. Sci. U.S.A. 114, 5952 (2017).

10. O.H. Loken, R. B. Sagar, Int. Assoc. Sci. Hydrol. Publ. 79, 282 (1967).

11. J. D. Ives, J. T. Andrews, R. G. Barry, Naturwissenschaften 62, 118 (1975).

12. A. C. Mix, W. F. Ruddiman, Quat. Res. 21, 1 (1984).

13. M. Milankovitch, Kanon Der Erdbestrahlung Und Seine Andwendung Auf Das Eiszeitenproblem (Royal Serbian Academy, 1941).

14. W.F.Budd, I.N.Smith, Geogr. Phys. Quat. 41, 279 (1987).

15. K. D. Burke et al., Proc. Natl. Acad. Sci. U.S.A. 115, 13288 (2018).

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致谢

作者感谢美国国家科学基金会和威斯康星大学麦迪逊分校的支持。

10.1126 / science.aem3295

代谢

将葡萄糖代谢置于电子控制之下

一种电子设备可控制调节小鼠血糖浓度的氧化还原机制

W. E. Bentley $^{1}$ 和 G. F. Payne $^{1}$

电极一直是生物学发现和疾病治疗的重要工具。在生物电理论被接受的几十年前,路易吉·伽伐尼(Luigi Galvani)和亚历山德罗·伏打(Alessandro Volta)就发现了“动物电”;而在 DNA 结构和遗传密码被破解之前,艾伦·霍奇金(Alan Hodgkin)和安德鲁·赫胥黎(Andrew Huxley)研究了动作电位如何在细胞中传播电信号。如今,电测量被常规用于评估心血管健康(例如心电图)和大脑活动(例如脑电图)。电极还使经过简单培训的人员能够使用公开可用的除颤器进行救命干预。在所有这些例子中,电极影响的是动物体内基于离子的电过程。在本期第 400 页,Maity 等人 (1) 报道了一种植入式电极,它通过一种完全不同的、基于还原-氧化(氧化还原)反应的机制与生物体对接。他们将这种方法在小鼠身上进行了测试,目标是治疗 2 型糖尿病——这是一种影响全球数百万人的衰弱性疾病。

氧化还原反应在生物学中无处不在。它们可以独立发生,例如产生活性氧的反应,也可以在细胞中组装成空间有序的通路,例如线粒体中的呼吸电子传递链。氧化还原反应还嵌入在平衡复杂分子产生与降解(分别为合成代谢和分解代谢)的代谢网络中。除代谢外,氧化还原过程还参与调节和蛋白质相互作用网络,将环境、社会和生活方式的暴露转化为生物反应 $(2-5)$。例如,电极可以提供作用于氧化还原响应转录因子的信号,从而影响基因表达 $(6)$,这一概念被称为“电遗传学” $(7, 8)$。Maity 等人使用了一种在代谢水平上与身体生物过程相互作用的电极:它通过电化学方式氧化葡萄糖。这种方法有望成为治疗 2 型糖尿病和肥胖症的一种无药干预手段。

电极如何影响生物氧化还原机制,与它如何监测或影响离子的移动有着本质的区别。氧化还原网络中的带电粒子是通过电子传递反应流动的电子。这为使用电极影响氧化还原生物学带来了若干挑战 (9)。由于它们针对的是局部反应,基于氧化还原的干预通常比依赖于皮肤表面电极产生电场的基于离子的干预更具侵入性。在 Maity 等人的研究中,实现电化学葡萄糖氧化的电极被皮下植入小鼠体内。氧化还原反应通常还需要大量的激活能,生物体通过使用酶(触发特定分子反应的蛋白质)来克服这一问题。为了应对这一挑战,Maity 等人开发了一种非生物的

石墨毡基质,并以铂装饰的金纳米团簇作为电催化剂,以促进葡萄糖的选择性电化学氧化。植入式电极同样容易受到损伤,这会缩短其有效寿命。为了在数天甚至数周内保持电极性能,Maity 等人将其封装在由纤维素、海藻酸盐和白蛋白组成的 3 层保护结构中。由于葡萄糖氧化发生在电极表面,氧化速率与电极的表面积成正比,而从血液中清除多余葡萄糖的需求则与动物的体积成正比。Maity 等人在其小鼠研究中使用了 0.5-cm $^{2}$ 的电极来控制血糖浓度。为了确保电化学刺激在产生益处的同时足够无害,该干预措施采用了低电压(<1 V)。这足以产生葡萄糖酸(葡萄糖氧化的产物),后者由肾脏清除,并促进代谢从基于葡萄糖转向基于脂肪。

Maity 等人将这些电化学能力集成到一个无线电催化闭环健康优化设备中,并将其与市售的连续葡萄糖监测系统耦合。该装置将生物信息(葡萄糖浓度)转换为电信号。该信号通过标准电子技术进行分析,以产生用于引导电极干预(氧化葡萄糖)的电响应。

将该方法扩大到人体干预的尝试需要考虑如何适应更大的血容量,并确保在不同的免疫和代谢环境中保持稳定性。一种能够自动检测并纠正过高葡萄糖浓度的植入式电子设备(就像植入式除颤器检测并纠正危及生命的心律失常一样),可能比目前检测葡萄糖水平并释放胰岛素治疗糖尿病的设备具有优势。这些优势包括实现无需人工干预且无需药物(而非激素介导)运行的可能性。此类设备的电子特性还将便于与智能手机通信以进行健康监测和独立于人类的学习,从而实现个性化的糖尿病管理。现有的生物电子设备提供了进入神经和神经肌肉系统的显著途径。基于氧化还原的生物电子版本可以触及其他生理系统,例如免疫系统、内分泌系统和胃肠道,这些系统并不那么依赖于基于离子的电调节,但深受氧化还原网络的影响。因此,未来的电子干预设备可能有助于管理除糖尿病以外的其他疾病,调节人体与微生物组的相互作用,或在压力条件下维持氧化还原稳态,以及许多其他应用。

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参考文献与注释

1. D. Maity, P. Guha Ray, P. Buchmann, G. Charpin-El-Hamri, M. Fussenegger, Science 394, eady8560 (2026).

2. D. P. Jones, H. Sies, Antioxid. Redox Signal. 23, 734 (2015).

3. H. Sies, R. J. Mailloux, U. Jakob, Nat. Rev. Mol. Cell Biol. 25, 701 (2024).

4. H. Sies, D. P. Jones, Nat. Rev. Mol. Cell Biol. 21, 363 (2020).

5. D. P. Jones, Free Radic. Biol. Med. 217, 179 (2024).

6. W. Weber et al., Nucleic Acids Res. 37, e33 (2009).

7. T. Tschirhart et al., Nat. Commun. 8, 14030 (2017).

8. J. M. Lawrence et al., Sci. Adv. 8, eabm5091 (2022).

9. E. Kim et al., Adv. Sci. 12, e10184 (2025).

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致谢

作者感谢国防威胁削减局(grant HDTRA1–19–0021)、戈登和贝蒂·摩尔基金会(grant GBMF11395)以及美国国家科学基金会(grant 2607564)的支持。

10.1126 / science.aem0762

细胞生物学

两幕细胞死亡芭蕾

两种使线粒体通透化的蛋白质通过不同的机制促进细胞死亡

Cristina Muñoz-Pinedo $^{1}$ 和 Seamus J. Martin $^{2}$

复杂的多细胞生物由于衰老、感染和损伤等多种原因,需要不断地更换细胞。在许多情况下,细胞死亡是对压力的一种响应,通过一个被称为细胞凋亡(apoptosis)的调节过程来实现 (1)。细胞凋亡的一条关键途径涉及两种相关的蛋白质:Bcl-2相关X蛋白 (BAX) 和 Bcl-2同源拮抗杀手蛋白 (BAK),它们在线粒体中形成孔道 (2, 3)。这会将细胞色素 c 释放到细胞质中,从而触发协调细胞凋亡的半胱天冬酶(caspase)蛋白酶的激活 (4)。BAX-BAK 孔道还可能导致线粒体 DNA (mtDNA) 延迟释放到细胞质中,并产生 I 型干扰素 (IFNs),这是一种经典的抗病毒免疫反应 (5, 6)。在本期第 401 页,Yang 等人 (7) 报道了两种不同的 BAX-BAK 复合物——一种用于释放细胞色素 c,从而促进免疫静默的半胱天冬酶依赖性细胞凋亡;另一种则促进 mtDNA 释放、非半胱天冬酶依赖性细胞死亡以及 IFN 产生,以刺激炎症。

细胞凋亡的一个总体目标是外科手术式地移除

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线粒体上的双重作用

为了应对细胞压力,不同的 BAX-BAK 复合物会组装,以促进触发不同细胞死亡途径的因子的释放。复合物 1 是免疫沉默的,而复合物 2 则会激活强烈的免疫反应。

ANT1,腺嘌呤核苷酸转运蛋白 1;BAK,Bcl-2 同源拮抗杀手蛋白;BAX,Bcl-2 相关 X 蛋白;cGAS,环 GMP-AMP 合成酶;IFN α / β,干扰素 α 和 β;PHB1,2,禁止蛋白 1 和 2;STING,干扰素基因刺激因子;VDAC1,2,3,电压依赖性通道 1, 2 和 3。

细胞,且避免炎症 (1, 8)。这在很大程度上得益于吞噬细胞在质膜完整性丧失之前,能够迅速识别并清除凋亡细胞,从而防止促炎分子从死亡细胞中释放 (1, 9)。基于这些原因,细胞凋亡通常在免疫学上是沉默的。此外,由 caspase 介导的蛋白质失活进一步增强了这一效果,这些蛋白质在促进免疫反应中起关键作用,例如环 GMP-AMP 合成酶 (cGAS)、干扰素调节因子 3 (IRF3) 和白细胞介素-33 (IL-33) (1, 10)。因此,当凋亡相关的 caspase 活性被抑制时——无论是通过药物还是由病原体编码的 BAX 抑制剂——这可以将原本免疫沉默的细胞死亡事件转化为促炎事件 (1, 5, 6, 8)。

包括 DNA 损伤、蛋白质错误折叠和病毒感染在内的多种形式的细胞压力,会促进 BAX 和 BAK 的激活,从而导致线粒体细胞色素 c 的释放,并形成凋亡蛋白酶激活因子 1 (APAF1)--9 凋亡小体——这是一个激活下游“执行者”-3 和 -7 的蛋白质复合物 (4)。这导致通过 介导的数百种蛋白质的蛋白水解来实现受控的细胞拆除,产生经典的凋亡表型 (1, 11)。由于 BAX-BAK 介导的线粒体通透化对细胞命运至关重要,这一过程的复杂细节已被深入研究 (2, 3, 12, 13, 14)。因此,目前已明确,由细胞压力启动的一种或多种 BH3-only 蛋白(带有 Bcl-2 同源结构域 3 的蛋白)的激活会动员 BAX 和 / 或 BAK,导致它们在线粒体外膜内逐渐寡聚化,形成允许细胞色素 c 外流的孔道或通道。BAX-BAK 孔随后可以合并形成大孔,这些大孔被认为与 mtDNA 的释放有关,但其具体发生机制一直是争论的话题 (12, 13, 14)。BAX-BAK 依赖性的 mtDNA 释放具有重要影响,因为这可以激活 cGAS-干扰素基因刺激因子 (STING) 通路以触发抗病毒 IFN 的产生,但这通常被 BAX 介导的 cGAS 和 IRF3 蛋白水解所抵消 (10)。然而,在缺乏 APAF1 或 BAX 活性被抑制的细胞中,mtDNA 驱动的 IFN 产生会被释放 (5, 6)。

先前的研究提出,与凋亡相关的 mtDNA 释放源于 BAX-BAK 大孔驱动的线粒体内膜通过外膜的疝出,最终导致内膜破裂并通过此类疝出释放 mtDNA (12, 13)。然而,Yang 等人提供了证据,证明线粒体中形成了两种截然不同的 BAX-BAK 复合物:复合物 I,其分子量较低(~160 kDa)并促进细胞色素 c 的释放;以及复合物 II,其分子量较高(~600 kDa)——由 BAX、BAK、电压依赖性阴离子选择性通道蛋白 1 至 3 (VDAC1, VDAC2 和 VDAC3)、腺嘌呤核苷酸转运蛋白 1 (ANT1) 以及 prohibitins 1 和 2 (PHB1 和 PHB2) 组成——且对于 的释放和 cGAS-STING 通路的激活至关重要。出人意料的是,研究表明,在凋亡小体介导的 caspase 激活受到抑制的情况下,复合物 II 是细胞死亡(作者称之为 baciptosis)所必需的(见图)。

Yang 等人证明,缺乏复合物 II(缺失 VDAC1, VDAC2 或 PHB2)的哺乳动物细胞仍然可以释放细胞色素 c 并经历 BAX-BAK 依赖性的线粒体疝出,但其 释放和 IFN 产生显著减弱。目前尚不清楚复合物 II 正确促进 释放的具体机制,尽管有证据表明,BH3-only 蛋白可以诱导该复合物内 VDAC 通道的构象重塑,从而导致钙离子流入和 BAX 流出。出乎意料的是,作者观察到 的释放是 caspase 非依赖性细胞死亡所必需的。在下游 激活受抑制的情况下,缺失 VDAC1 或 VDAC2 的细胞表现出 BAX-BAK 依赖性的细胞色素 c 流出,但没有 释放,并且能够生存数日。在存在复合物 II 的条件下,消除 同样减轻了 BAX 非依赖性细胞死亡。该研究结果挑战了主流观点,即 非依赖性细胞死亡是线粒体外膜通透化和细胞色素 c 释放导致线粒体功能障碍的被动结果。然而,胞质 如何引发 非依赖性细胞死亡仍有待确定,尽管胞质 DNA 传感器 cGAS、Z-DNA 结合蛋白 1 (ZBP1) 和干扰素诱导蛋白 16 (IFI16) 似乎并未参与其中。

Yang 等人的研究表明,BAX-BAK 的激活可导致两种截然不同的细胞死亡模式,每种模式由不同的 BAX-BAK 复合物引导:一种促进由细胞色素 c 启动的 BAX 激活从而导致凋亡;另一种促进由 BAX 启动的未知胞质效应因子(或多个效应因子)的激活,从而导致 非依赖性细胞死亡。值得注意的是,前一种死亡模式在免疫学上是沉默的,而后者则伴随着强烈的抗病毒免疫反应 (5–7)。由复合物 II 介导的细胞死亡途径可能是作为一种备份演化而来的,用以对抗携带 抑制剂以抑制凋亡小体死亡途径的病毒和其他病原体。这种情况将需要启动强烈的炎症反应(凋亡通常会减轻这种反应 (1, 8)),以及一条独立于 运行的故障安全细胞死亡途径。因此,组装复合物 II 以驱动 释放可以被视为一种效应因子触发的免疫形式,它是响应于病原体活动(即 抑制)的检测而启动的,而非响应于病原体相关分子模式的检测,而后者是高等生物中主要的免疫形式 (15)。此外,在某些细胞类型(如神经元和心肌细胞)或某些癌症中,APAF1 的表达在表观遗传上被沉默,在这种情况下,由复合物 II 启动的 BAX 非依赖性细胞死亡可能也发挥作用。

目前研究尚未解决的问题包括:在细胞质中检测到 mtDNA 时启动细胞死亡的核酸传感器的身份。此外,复合物 II 如何促进 mtDNA 外流,以及它是否被 caspase 抑制,仍有待阐明。Yang 等人确定的线粒体通透化机制,为 BAX-BAK 细胞死亡芭蕾的下一步研究搭建了一个令人兴奋的舞台。□

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参考文献与注释

1. S. J. Martin, C. M. Henry, S. P. Cullen, Mol. Cell 46, 387 (2012).

2. H. L. Glover, A. Schreiner, G. Dewson, S. W. G. Tait, Nat. Cell Biol. 26, 1434 (2024).

3. P. E. Czabotar, A. J. Garcia-Saez, Nat. Rev. Mol. Biol. 24, 732 (2023).

4. X. Jiang, X. Wang, Annu. Rev. Biochem. 73, 87 (2004).

5. M.J. White et al., 159, 1549 (2014).

6. A. Rongvaux et al., 159, 1563 (2014).

7. S. Yang et al., Science 394, eaea2181 (2026).

8. M. Beltrán-Visiedo et al., Nat. Rev. Mol. Biol. 26, 884 (2025).

9. I. K. H. Poon, K. S. Ravichandran, Annu. Rev. Pharmacol. Toxicol. 64, 339 (2024).

10. X. Ning et al., Mol. 74, 19 (2019).

11. R. C. Taylor, S. P. Cullen, S. J. Martin, Nat. Rev. Mol. Biol. 9, 231 (2008).

12. K. McArthur et al., Science 359, eaao6047 (2018).

13. J. S. Riley et al., EMBO J. 37, EMBJ201899238 (2018).

14. K. Cosentino et al., Mol. 82, 933 (2022).

15. B. C. Remick, M. M. Gaidt, R. E. Vance, Annu. Rev. Immunol. 41, 453 (2023).

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致谢

S.J.M. 感谢欧洲研究委员会高级资助计划(DESTRESS, AdG 101020534)的支持。

10.1126 / science.aem1247

$^{1}$ 西班牙巴塞罗那,贝尔维奇生物医学研究所 (IDIBELL)。$^{2}$ 爱尔兰都柏林,三一学院,遗传学斯默菲特研究所,遗传学系,分子细胞生物学实验室。电子邮箱:martinsj@tcd.ie

鸟类大脑的认知能力

秃鸦的决策速度快于猴类和人类

Michael Colombo 和 Oriane Poutrain-Sorel

鸟类曾被认为主要是依靠本能和简单学习的生物,但现在它们展现出的认知能力正显示出能够与灵长类动物相媲美,有时甚至超越后者的潜力。即使是鸽子——这种通常不被认为具有高认知能力的动物——也能区分癌细胞和健康细胞的图像,表征“相同”和“不同”的概念,进行数值辨别,并能以类似于人类阅读某些方面的方式区分单词和非单词。鸦科动物(乌鸦、渡鸦、丛林蓝鸦和秃鼻鸦)展现出更为令人印象深刻的能力,例如自我识别、工具使用、问题解决、情景记忆、心智理论以及对未来事件的规划,其水平往往超过灵长类动物的类似能力。在本期第 445 页中,Schmidbauer 和 Nieder (1) 报道称,秃鸦能够做出极快速且准确的决策。

这些发现增加了人们对鸟类心智能力的日益认可。

拥有相同的运作原理缩小了鸟类与灵长类动物之间的认知差距,但这不能完全解释鸟类的高水平认知和快速决策能力。另一种解释是,尽管鸟类大脑体积小,但其神经元数量不成比例地多。恒河猴的大脑比渡鸦(另一种具有惊人认知能力的鸦科动物)的大脑大 8 倍,但其神经元数量仅为后者的 3 倍(63 亿美元 versus 22 亿美元)。这种差异的根源在于神经元的大小:鸟类大脑的神经元比灵长类大脑的神经元更小,因此在相同体积的组织中可以容纳更多神经元(见图)(6)。

然而,如果恒河猴大脑的神经元数量是渡鸦大脑的 3 倍,难道这不应该仍然赋予其认知

Schmidbauer 和 Nieder 训练秃鸦报告计算机屏幕上出现的随机点是向上还是向下移动,或者向左还是向右移动。一旦点开始移动,乌鸦通过啄击目标来报告其方向:对于上下移动的点,目标出现在点之上或之下;对于左右移动的点,目标出现在点的两侧。乌鸦做出决策并做出反应大约需要 235 ms,这一速度是执行类似任务的恒河猴 (2) 和人类 (3) 的两倍。此外,乌鸦决策的准确率依然很高。Schmidbauer 和 Nieder 还测量了乌鸦在尾侧 nidopallium(nidopallium caudolaterale)的神经元活动,该脑区在功能上等同于灵长类动物的前额叶皮层。他们注意到,方向选择性神经元在移动点刺激出现后约 70 ms 被激活,并在鸟类做出反应前约 170 ms 被激活。

哪些因素解释了乌鸦的极速决策及其惊人的认知能力?研究人员通常将灵长类动物的认知表现归因于—。

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以小博大

尽管鸟类的脑容量远小于哺乳动物,但它们却展现出极高的认知能力。鸟类不具备分层的大脑组织结构,而是拥有排列成簇的更小神经元。高神经元密度和较短的神经元间距支撑了快速的信息处理和决策。

寒鸦

Corvus corone

猕猴

Macaca mulatta

这对应于一个拥有数十亿个神经元的大脑,以及一个通过跨越 6 个皮层层的循环(重复)神经回路处理信息的皮层。然而,鸟类的大脑要小得多,且没有皮层,这似乎表明它们的计算能力要低得多。那么,它们的认知能力和决策速度如何能与灵长类动物相当甚至更高呢?部分答案在于它们的大脑架构。与灵长类动物皮层的分层组织不同,鸟类外套层(包含尾侧 nidopallium caudolaterale)——一个与灵长类皮层大致类似的区域——其神经元呈簇状排列 (4)。尽管存在这种差异,灵长类大脑的重复神经回路在鸟类大脑中同样存在,其处理感官信息的径向组织纤维与将信息在不同大脑区域之间关联的切向运行纤维相连接 (5)。无论大脑的整体架构如何,功能能力都源自这种回路。因此,鸟类大脑处理信息的方式与灵长类大脑相似。

这对猕猴来说是优势吗?不一定。与灵长类皮层中脑神经元的比例相比,鸟类外套层中的神经元比例更高 (6, 7)。例如,猕猴大约有 17 亿美元 个皮层神经元,而渡鸦有 12 亿美元 个外套层神经元 (6)。这使得渡鸦与猕猴处于几乎相同的认知水平。当比较重点转向最参与认知的皮层或外套层子区域(如灵长类动物的前额叶皮层和鸟类大脑的 nidopallium 和 mesopallium)的神经元数量时,这种差异进一步缩小。例如,在这些参与认知的专门区域中,秃鸦(一种比渡鸦小的鸦科鸟类)与黑猩猩拥有相同数量的神经元——大约 6 亿 个 (7)。

鸟类大脑中密集排列的神经元不仅使大脑结构紧凑,还使其运行迅速。更高的神经元密度导致神经元之间的距离更短,从而缩短了传导时间并提高了信息处理速度 (6, 7)。这些效应很可能解释了 Schmidbauer 和 Nieder 的研究中寒鸦所做出的超快速决策。结合其他关于鸟类卓越认知能力的最新证据,这些发现促使人们重新思考浓缩在小型鸟类大脑中的强大能力。 □

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参考文献与注释

1. P. Schmidbauer, A. Nieder, Science 394, 445 (2026).

2. T. Hanks et al., eLife 3, e02260 (2014).

3. J. Palmer et al., J. Vis. 5, 376 (2005).

4. H.J. Karten, Ann. N. Y. Acad. Sci. 167, 164 (1969).

5. M. Stacho et al., Science 369, eabc5534 (2020).

6. S. Olkowicz et al., Proc. Natl. Acad. Sci. USA 113, 7255 (2016).

7. F. Ströckens et al., J. Comp. Neurol. 530, 1588 (2022).

10.1126 / science.aem0341

BOOKS ET AL.

反思

显微镜与隐喻

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科学告诉我们如何拯救地球——而诗歌帮助我们理解为何应当如此

Phillip Levin $^{1}$ 和 David Hassler $^{2}$

2017年1月,随着即将就任的特朗普政府从白宫网站删除气候变化信息,并对联邦科学家的沟通施加新限制,诗人简·希尔希菲尔德(Jane Hirshfield)做出的回应并非一篇论文或一场抗议演说,而是一首诗。三个月后,这首名为《在第五天》(On the Fifth Day)的诗以整页广告的形式出现在《华盛顿邮报》上,而一周后,希尔希菲尔德在国家广场举行的“科学大游行”期间朗诵了这首诗 (1)。

这首诗并没有提供关于气候变化或生物多样性丧失的新证据。科学已经完成了这项工作。相反,它提醒人们为什么这些证据至关重要。在仅凭科学事实似乎不足以产生影响的时刻,它为悲伤、责任、希望和惊叹地赋予了声音。正如希尔希菲尔德经常所说,显微镜和隐喻都是探索的工具。

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诗歌阐明证据为何重要

诗歌与科学之间的关系通常被界定为一种沟通关系:诗歌和其他艺术形式可以帮助向更广泛的受众解释科学。虽然这确实没错,但这低估了两者在对话中各自能带来的独特贡献。

科学帮助我们理解正在发生什么,为什么会发生,以及哪些干预措施最有可能产生影响。诗歌则可以应对另一种挑战:通过激活情感、想象力、身份认同、记忆和价值观,帮助人们产生足够的关注从而参与其中——而这些特质往往决定了科学是否能产生个人层面的意义 (2, 3)。

诗歌不仅仅是传播科学的一种方式,它还能帮助创造使此类知识变得有意义的情感和文化条件。简单来说,科学可以帮助我们询问“我该做什么?”以及“我如何知道它是否奏效?”,而诗歌和其他艺术形式则可以帮助我们询问“我为什么要关心?”

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为自然保护培养连接感

越来越多的研究支持诗歌及其他艺术形式与保护科学(尤其是自然保护科学)之间的互补关系。参加有意将艺术与科学相结合的项目的人员报告称,他们在学习更多关于生物多样性知识的同时,表达了参与保护相关活动更强的意愿 (4)。基于艺术的保护教育在纠正关于受威胁物种的误解的同时,也提高了人们的理解程度 (5)。更广泛地,研究表明,艺术体验能够培养共情心、好奇心和情感连接,使科学信息更具记忆点且更相关 [例如 (6)]。对环境艺术的综述同样表明,审美体验可以加强与自然的联系,并增加从事亲环境行为的意向 (7)。

这一切并非暗示诗歌或其他艺术形式可以取代保护科学。相反,证据指向一种高效的互补性:艺术可以增强参与的动力,而科学则提供证据,帮助将这种动力引导至有效的行动中。这种关系呼应了更广泛的研究成果,即自然保护不仅依赖于生态知识,还依赖于人类的价值观、经验和关系。

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诗歌拓展了知识的定义

保护决策很少仅基于生态信息。它们还受到历史、文化、身份、记忆和生活经验的影响。这些形式的知识很难在地图、模型或期刊文章中捕捉,但它们能强烈影响保护工作的成败。艺术实践——包括讲故事、诗歌、摄影、表演和其他创意方法——提供了让生活经验、文化记忆和基于地域的知识可见的方式,而无需要求它们符合科学惯例 (8)。

科学认知与艺术认知之间的界限是可渗透的。科学家越来越多地利用诗歌和其他创意形式来探索其工作中传统科学写作无法捕捉的维度:悲伤、惊奇、不确定性、依恋和敬畏。此类工作并非取代科学探究,而是揭示了进行科学探究的人类经验。

为此,当我(Levin)在 2024 年开始与数百名同事共同开展《自然记录》(The Nature Record)——美国首次关于自然的科学评估 (9) ——时,我的合著者(Hassler)与诗人 Luisa A. Igloria 和 Aileen Cassinetto共同开发了一部配套的诗集,题为《我们时代的自然:关于美国土地、水域、野生动物及其他自然奇观的诗篇》(The Nature of Our Times: Poems on America's Lands, Waters, Wildlife, and Other Natural Wonders)(10)。该诗集汇集了来自艺术、生态学、学术界和原住民社区的声音,包括海洋生态学家 Maya Zeff,她的诗作《我翻译大海》用抒情的方式捕捉了定义海洋生态系统的互利共生关系;以及野生动物生态学家 Lara Volski,她的诗作《君主熊》深刻地描述了人类与动物之间相互影响的关系(见侧栏)。Zeff 和 Volski 的作品说明了科学观察和诗意关注如何产生于对自然世界的相同持续关注,并对其做出贡献。

多种认知方式的重要性在与原住民和当地社区的工作中尤为明显。在这里,基于艺术的方法有助于记录与海洋的文化联系,阐明嵌入在景观中的历史,并为多种形式的知识为保护规划提供信息创造空间 (11)。

2020 年,安尼希纳贝(Anishinaabe)诗人、学者兼环境活动家 Kimberly Blaeser 创立了 In-Na-Po——原住民国家诗人(Indigenous Nations Poets),这是一个致力于指导新兴作家、培育原住民诗歌实践并提高原住民作家可见度的全国性原住民诗歌社区 (12)。Blaeser 和 In-Na-Po 与其他组织开展合作,将诗歌、原住民知识、语言、社区以及与自然世界的关系联系起来。他们在 2023 年于威斯康星州多尔县(Door County)举行的指导静修活动产生了《为破碎星球而作的诗》(Poems for a Tattered Planet),这是一系列与 Overpass Light Brigade 合作创作的诗歌电影 (13)。此类合作并非与科学证据竞争,而是能丰富保护工作可利用的知识,有助于更全面地理解保护工作试图维持的生态和社会系统。

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科学助力直接行动

仅有动力是不够的。保护自然的历史充满了出于好意但最终失败的行动,因为这些行动基于不完整的认知或无效的干预。科学为决定在何处采取行动、哪些行动最有可能成功、如何评估权衡以及是否真正实现了预期结果提供了基于证据的基础。如果说诗歌能帮助激发公众保护自然的意愿,那么科学则能确保这种努力被引导至有利于生物多样性的行动上,而不仅仅是让我们觉得自己在做一些有用的事情。

因此,两者的关系是互惠的,而非等级制的。没有科学的艺术可能会激发无效的行动;而没有艺术的科学往往难以激发任何行动。两者单独存在都是不充分的。

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下一个前沿

尽管人们对艺术与科学协作的兴趣日益浓厚,但关于其长期保护效果的严谨证据仍然有限。近期的大量文献由概念框架、综合论文、项目描述以及对新兴实践的反思组成,而非对保护结果的评估 [例如,(14)]。尽管如此,这项工作为艺术家确定了极具前景的新角色——他们不仅是科学发现的传播者,更是能够帮助塑造研究问题、揭示被忽视的视角并催化新问题解决方法协作伙伴。

接下来的一个重要步骤是测试从艺术体验到动力,从动力到基于证据的决策,并最终到人类行为和生物多样性产生持久变化的完整路径。比较研究和纵向研究对于确定哪些艺术方法对不同受众和保护情境最有效,以及在何种条件下艺术与科学的协作能产生超越传统保护传播或单一参与所能实现的结果 $(7, 14)$ 将至关重要。

正是在这个新兴领域中,肯特州立大学的威克诗歌中心(Wick Poetry Center)将于 2026 年 11 月召开首届“科学诗人集会”(Poets for Science Gathering)(15)。此次集会将汇集诗人、科学家、教育工作者、临床医生、学生、环境倡导者、政策制定者、艺术家以及公众,共同探索科学与诗歌的交汇点。

这次会议将庆祝艺术与科学的协作,但也将对其提出挑战。一首诗(或在其他情境下的行为艺术、视觉艺术或故事)何时能不仅改变一个人的感受,而且改变其行为?哪些协作能产生持久的影响?针对谁?在什么情况下?而这些改变最终能否与更健康的生态系统和更具韧性的社区联系起来?

科学揭示了自然界如何运作以及它如何变化。诗歌提醒我们为什么这个世界至关重要。自然保护需要这两者的工具——显微镜和隐喻。理解它们如何协同工作,可能会成为该领域最重要的课题之一。

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参考文献与注释

1. J. Hirshfield, "On the Fifth Day," The Washington Post, 14 April 2017.

2. D. J. Curtis, N. Reid, I. Reeve, S. A. P. I. EN. S. 7, 1655 (2014).

3. S. Dupont, J. Mar. Biol. Assoc. U.K. 97, 1211 (2017).

4. O. Opermanis, S. N. Kalnins, A. Aunins, J. Nat. Conserv. 28, 67 (2015).

5. M. Franquesa-Soler, L. Jorge-Sales, J. F. Aristizabal, P. Moreno-Casasola, J. C. Serio-Silva, PLOS ONE 15, e0228382 (2020).

6. P.-C. Wang, C.-Y. Yu, Sustainability 10, 1098 (2018).

7. A.-S. Tribot, D. Faget, T. Richard, T. Changeux, Biol. Conserv. 276, 109791 (2022).

8. R. E. Brennan, Ocean Coast. Manag. 162, 110 (2018).

9. The Nature Record; https: / naturerecord.org / .

10. L.A. Igloria, A. Cassinetto, D. Hassler, Eds., The Nature of Our Times: Poems on America's Lands, Waters, Wildlife, and Other Natural Wonders (Paloma Press, 2025).

11. M. Strand, N. Rivers, B. Snow, Front. Mar. Sci. 9, 886632 (2022).

12. Indigenous Nations Poets, About In-Na-Po; https: / www.indigenousnationspoets.org / about-us.

13. Indigenous Nations Poets, "Poems for a Tattered Planet" (2023); https: / www.indigenous-nationspoets.org / poems-for-a-tattered-planet.

14. I. Jarić et al., Front. Ecol. Environ. 23, e70012 (2025).

15. Poets for Science Gathering, Wick Poetry Center, Kent State University, 12 to 14 November 2026; https: / poetsforscience.org / gathering-2026 / .

10.1126 / science.aej4196

读者来信

编辑:Jennifer Sills

各团队在加拿大萨斯喀彻温省的里贾纳大学竞相搭建圆锥形帐篷(tipis)。这一年度活动反映了里贾纳大学与加拿大第一民族大学之间长期的合作伙伴关系。

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原住民高等教育需要支持

原住民知识体系对于应对保护挑战至关重要。原住民大学为原住民语言、知识体系和世界观的繁荣提供了空间。此类大学理应获得其国家政府可靠的支持。

从保护区的管理到环境治理,原住民的声音已经重塑了关于人类对地球责任的科学和政策讨论 (1, 2)。诸如加拿大第一民族大学、美国的部落学院与大学以及巴西的联邦原住民大学等机构,有助于振兴并维持那些引导了世世代代人类与环境关系的语言、文化和知识体系 (3–5)。这些由原住民领导的机构还通过培训能够衔接不同知识体系以解决复杂社会-生态交互作用的专家,来培养本地专业能力,从而加强研究、治理和本地管理能力 (3)。

尽管发挥着重要作用,但原住民大学仍然高度依赖于不稳定的政治支持。在巴西,联邦原住民大学的建立代表了对原住民领导的高等教育的一次历史性投资 (6),但在其他地方,相关机构仍在艰苦奋斗。厄瓜多尔的第一所跨文化大学——Amawtay Wasi 大学面临着剧烈的预算和人员削减,影响了其运行 (7)。在墨西哥,跨文化大学面临着长期的资源限制,以及由于政治干预而导致的有限的机构自主权 (8, 9)。玻利维亚的原住民大学 (UNIBOL) 也面临着治理、基础设施和预算方面的限制 (10),而尼加拉瓜的尼加拉瓜加勒比海岸自治区大学 (URACCAN) 则继续在历史性的边缘化、对原住民自主权的持续挑战以及资源有限的情况下运行 (11)。

作为来自美洲各机构的原住民及盟友学者,我们对新原住民大学的发展表示赞赏,并敦促各国政府超越象征性的承诺,投资于原住民领导的高等教育的长期稳定性、自主权和增长。在美国,1978 年的《部落控制学院与大学援助法》建立了一个联邦框架来支持部落学院与大学,这是一个支持语言振兴、文化保护和培训的原住民领导机构网络 (5)。同样,新西兰通过将年度拨款改为持续的法定资金机制,以提供更高的资金确定性,从而加强了对毛利人领导的 wānanga(传统学习场所)的长期支持 (12)。这些例子共同证明了长期的立法和资金承诺如何支持原住民领导的高等教育机构的稳定性、自主权和增长。美洲各国政府应建立长期资金机制,加强跨文化和原住民领导组织的机构自主权,并支持原住民的教育主权。

Bruno Eleres Soares $^{1,2}$ , Thaïs Bernos $^{3}$ , Rodrigo F. R. Carmo $^{4}$ , Lucas Colares $^{5}$ , Jaime Grimm $^{6}$ , Alessandra Higa $^{7}$ , Anna-Leah King $^{8}$ , Andrew M. Miller $^{9}$ , Robert Newman $^{10}$ , Andrea M. D. Ortiz $^{11}$ , Andrea Sterzuk $^{8}$ , Vincent Ziffle $^{12}$

$^{1}$ 加拿大萨斯喀彻温省里贾纳,里贾纳大学环境变化与社会研究所。$^{2}$ 巴西里约热内卢,里约热内卢联邦大学生态学研究生项目。$^{3}$ 美国佛蒙特州伯灵顿,佛蒙特大学鲁本斯坦环境与自然资源学院。$^{4}$ 巴西累西腓,伯南布哥联邦农村大学生物系。$^{5}$ 巴西贝伦,埃米利奥-戈埃尔迪帕拉博物馆动物学协调部门。$^{6}$ 加拿大不列颠哥伦比亚省维多利亚,维多利亚大学生物系。$^{7}$ 美国南达科他州凯尔,奥格拉拉拉科塔学院数学、科学与技术系。$^{8}$ 加拿大萨斯喀彻温省里贾纳,里贾纳大学教育学院。$^{9}$ 加拿大萨斯喀彻温省里贾纳,加拿大原住民大学原住民研究系。$^{10}$ 美国北达科他州格兰福克斯,北达科他大学生物系。$^{11}$ 智利孔塞普西翁,孔塞普西翁大学地理系。$^{12}$ 加拿大萨斯喀彻温省里贾纳,加拿大原住民大学原住民知识与科学系。电子邮件:soares.e.bruno@gmail.com

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参考文献与注释

1. S.J. Bruce, Conserv. Biol. 40, e70254 (2026).

2. E. S. Brondízio et al., Annu. Rev. Environ. Resour. 46, 481 (2021).

3. S. Brant, K. Williams, D. Longboat, Front. Educ. 11, 1702361 (2026).

4. K. Leonard, J. Comp. Int. Hig. Educ. 13, 90 (2021).

5. E. S. Huaman, B. Chiu, C. Billy, Educ. Pol. Anal. Archiv. 27, 101 (2019).

6. 共和国总统府,第 15.418 号法律,2026 年 5 月 28 日。成立联邦原住民大学 (Unind) (2026);https: / www.planalto.gov.br / ccivil\_03 / \_ato2023-2026 / 2026 / lei / I15418.htm。

7. R. Revelo, "Consejo de Educación Superior aprueba intervenir la Universidad Amawtay Wasi, centro educativo habla de denuncia falsa," Primicias (2026 年 7 月 13 日);https: / www.primicias.ec。

8. M. Lloyd, Intercult. Educ. 35, 402 (2024).

9. S. Schmelkes, Intercult. Educ. 20, 5 (2009).

10. M. M. Chundary, Rev. Educ. Sup. Soc. 36, 195.

11. J. Cupples, K. Glynn, Singap. J. Trop. Geo. 35, 56 (2014).

12. 新西兰教育部,教育报告:为 Wananga 提供更大的资金确定性 (2024 年 4 月 24 日);https: / web-assets.education.govt.nz / s3fs-public / 2026-02 / MARKED\~1.PDF。

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印度需要一项树木保护计划

印度拥有 2603 种已知树种,其中 650 种为特有种,469 种已被评估为受威胁物种 (1, 2)。2025 年 10 月,印度环境、森林和气候变化部启动了国家红皮书评估(National Red List Assessment),这是一项为期 5 年、耗资近 US1000万美元 的计划,旨在根据世界自然保护联盟 (IUCN) 红皮书标准对大约 11,000 个物种(包括 7000 种植物)进行评估 (3)。然而,识别风险并不等同于采取行动。印度应在大量评估投资的基础上,为被发现处于易危状态的物种制定一项保护计划。

其他国家已经为其受威胁树种建立了国家保护行动计划。例如,几内亚、加蓬、加纳和肯尼亚,这些国家的树木植物群数量都远少于印度 (1),但它们都实施并为有时限的框架拨付了预算,将优先保护物种分配给特定机构,用于种子库建设、栖息地保护或野外研究 (4–8)。几内亚的计划涵盖了 76 个受威胁物种。哥伦比亚作为全球树种资源第二丰富的国家,也有一项涵盖 701 个受威胁物种的计划 (8)。每项计划都将保护行动与红皮书数据直接挂钩,并包含正式的审查周期。

印度应建立一个类似的系统,时间点与已为国家红皮书(National Red Data Books)设定的 2030 年截止日期同步。现有的计划(如绿色印度计划和补偿造林基金)支持大规模植树,但并未为指定的受威胁物种指定资金或机构责任 (9)。每个被评估为受威胁的物种都应自动添加到常设行动清单中,而不是等待单独的政治批准。该计划应设定明确的保护目标,例如为一定比例的受威胁物种建立种子库备份。此外,该计划应包含一个与红皮书时间表同步的 5 年审查周期,以便物种评估与保护行动保持在同一进度上,而不是逐渐脱节。

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Anurag Dhyani

贾瓦哈拉尔·尼赫鲁热带植物园与研究所,印度喀拉拉邦蒂鲁瓦南塔普拉姆。电子邮箱:anuragdhyani@gmail.com

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参考文献与注释

1. 国际植物园保护联盟 (BGCI), "State of the world's trees" (BGCI, 2021).

2. M. Rivers, A. C. Newton, S. Oldfield, Plants People Planet 5, 466 (2023).

3. 印度政府环境、森林和气候变化部, “National Red List Assessment of Indian flora and fauna: Vision 2025–2030” (2025).

4. C. Couch, 几内亚国家标本馆, "Plan d'Action National de Conservation pour les Arbres Menacés de Guinée" (Royal Botanic Gardens, Kew, and Herbier National de Guinée, 2023); https: / www.herbierguinee.org / uploads / 2 / 6 / 3 / 0 / 26303479 / panc\_arbres\_menaces\_guinea\_v2b\_2023.pdf.

5. GaboTREE 项目, “Plans d’actions de conservation multi-espèces des espèces d’arbres les plus menacées du Gabon” (Fondation Franklinia, 2023); https: / www.tropicos.org / projectimages / Gabon / GaboTREE / PACarbres.pdf.

6. BGCI, IUCN SSC 保护规划专家组, 加纳 CSIR-林业研究所, "Planning conservation action for Ghana's threatened tree species" (BGCI, 2023); https: / www.bgci.org / wp / wp-content / uploads / 2023 / 03 / PCAGhanaMedRes.pdf.

7. Y. Harvey-Brown, K. Shaw, Eds., "Planning Conservation Action for Kenya's Threatened Trees" (BGCI, 2020).

8. C. Lopez-Gallego 等, "Plan de acción para la conservación de los árboles de Colombia" (2024).

9. 印度政府环境、森林和气候变化部, "Year-End Review 2025" (2025).

10.1126 / science.ael9835

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AI 生物安全必须涵盖农业

生物人工智能 (AI) 的进步已将生物安全推向公众辩论的中心,美国国会目前正在考虑《生物安全现代化与创新法案》(1)。然而,这场辩论与更广泛的生物安全讨论一样,仍然主要集中在人类健康上,而忽视了影响农作物和牲畜的病原体的重要性。美国及全球各国政府应通过降低蓄意病原体攻击的可能性,并降低目标受害的脆弱性,将保护农作物和牲畜列为优先事项。

农业病原体可能威胁粮食安全、经济和政治稳定。1970 年,南方玉米叶枯病摧毁了美国约 15% 的玉米作物,而巴拿马病则重创了全球香蕉生产,严重损害了多个国家的经济,并引发了整个中美洲的劳工罢工和政治动荡 (2–6)。现代农业中的遗传单一性、密集生产系统以及全球互联的供应链放大了这些风险。

农业病原体在滥用方面也呈现出独特的风险。许多重要的农业宿主-病原体系统已被详细表征,实验材料易于获取,且宿主特异性可以降低开发者的风险 (7–10)。与可传播的人类病原体不同,它们还可以使损害集中在特定的作物、牲畜种群或环境中,从而可能减少反噬。AI 可能会加剧农业产品在面对针对性攻击时的脆弱性。

因此,农业生物安全需要一套从预防到响应的连续防御体系。美国农业部已经呼吁将农场和食品系统视为国家安全资产 (11);这一努力值得强有力的支持和扩展。DNA 合成筛查应对高后果农业病原体进行与人类病原体同样严格的审查。AI 评估应明确测试与农业滥用相关的能力。

生物监测应扩大到涵盖农田、畜群、野生动物、媒介和贸易商品。政府还应加强农业专用诊断、兽用疫苗、抗病品种、检疫能力和快速响应渠道。分层防御可以在防止蓄意滥用的同时,保留合法的研究。

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Jonathan Feldman $^{1,2}$ , Tal Feldman $^{3}$ , Pardis C. Sabeti $^{2,4,5,6}$

$^{1}$ 美国佐治亚州亚特兰大,佐治亚理工学院计算学院。$^{2}$ 美国马萨诸塞州剑桥,麻省理工学院和哈佛大学博德研究所。$^{3}$ 美国康涅狄格州纽黑文,耶鲁法学院。$^{4}$ 美国马萨诸塞州剑桥,哈佛大学生物有机体与进化生物学系。$^{5}$ 美国马萨诸塞州波士顿,哈佛大学 T. H. Chan 公共卫生学院免疫学与传染病系。$^{6}$ 美国马里兰州切维切斯,霍华德·休斯医学研究所。电子邮件:pardis@broadinstitute.org

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参考文献与注释

1. 美国国会,参议院,《2026年生物安全现代化与创新法案》,S. 3741,第119届国会,第2次会议,2026年1月;2026年1月29日提交至参议院。

2. S. Marquardt, Am. Hist. Rev. 106, 49 (2001).

3. L.A. Tatum, Science 171, 1113 (1971).

4. P. Balint-Kurti, J. Pataky, Phytopathology 114, 2007 (2024).

5. R. C. Ploetz, Crop Prot. 73, 7 (2015).

6. R. Harding et al., Plant Biotechnol. J. 23, 3628 (2025).

7. T. Nobori, Cell Host Microbe 33, 1227 (2025).

8. M. Urban et al., Nucleic Acids Res. 50, D837 (2022).

9. C. Verdonk, KK Gagalova, S. Raffaele, MC Derbyshire, Comput. Struct. Biotechnol. J. 27, 2881 (2025).

10. A. W. Woodward, B. Bartel, Genetics 208, 1337 (2018).

11. 美国农业部,“国家农场安全行动计划”,技术报告(美国农业部,2025年7月)。

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竞争利益

P.C.S. 是与病原体诊断和疫苗相关的知识产权的发明人,也是 Delve Bio 和 Lyra Labs 的创始人及股东。

气候金融

缺乏物理韧性的财政纪律

改革可以将财政纪律与韧性投资转化为相互增强的力量,而非相互竞争的关系

Aayushi Mishra $^{1}$ , Advait Arun $^{2}$ , Evan Kodra $^{1}$ , Auroop R. Ganguly $^{1,3}$

随着极端天气的加剧,气候脆弱国家面临着两种威胁:债务违约和物理暴露。国际货币基金组织(IMF)和多边开发银行能够很好地管理第一种威胁,通过信用评级和贷款条款奖励财政纪律,但

并没有相应的机制来奖励韧性投资。如果灾难袭击一个准备不足的经济体,这种差距会随着时间的推移而加剧,且由此产生的借贷会挤出下一轮韧性投资——先前的研究将此建模为“气候-债务毁灭循环”。目前尚未记录的是,在一次灾难期间,该循环在单个国家内部是如何实时展开的。我们利用 2025 年 10 月袭击牙买加的梅丽莎飓风(Hurricane Melissa)对此进行了实证追踪,并提出了相关改革方案——将韧性纳入债务可持续性分析、扩大韧性与可持续性信托(RST)基金的规模,以及采用气候韧性债务条款(CRDCs)——这些方案可以将财政纪律与韧性投资转化为相互增强的力量,而非相互竞争的关系。

在 2013 年至 2024 年间,牙买加将其公共债务(即通过国际贷方贷款和在金融市场出售债券所欠的资金)从国内生产总值(GDP)的约 144% 降低到 2023 年的 72% (1),目标是在 2027–2028 财年(FY)降至 60%。这种债务削减是通过多年的纪律性支出限制、基本盈余和严格的财政规则实现的。牙买加是根据自身的财政责任框架自愿采用这些规则的,而非作为 IMF 的条件。维持这些规则还使借贷成本保持在较低水平,这给了政府进一步坚持该路线的理由。2025 年 9 月,标准普尔全球(S&P Global)上调了牙买加的主权债务评级,以表明对其财政轨迹的广泛机构信心。随后几周,梅丽莎飓风以 5 级风暴的形式袭击,造成估计 122 亿美元 billion 的总损失、损害和成本(约占 2024 年 GDP 的 56.7%)(2)。保险赔付仅覆盖了损失的一小部分,大部分恢复资金以新的主权借贷形式提供。在几周之内,债务削减所创造的艰苦赢得的财政空间再次面临压力。

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气候-债务毁灭循环

有许多可能的增强机制可以引发气候-债务毁灭循环,特别是对于气候对增长和财政能力产生的缓慢、慢性的影响 (3)。对于我们这里关注的由灾难驱动的急性循环,该循环经过三个增强机制:优先考虑偿债而非资本投资的机构压力、灾难风险融资与实际恢复成本之间的结构性差距,以及灾后借贷重新制造了最初阻碍韧性投资的财政约束。在这里,我们利用牙买加报告的公共财务和灾难损失数据(图 S1),追踪了 2025 年梅丽莎飓风袭击牙买加后数周内该循环的每一步。基于灾难风险评估与风险管理研究,以及机制设计,两个问题引导了此次追踪:第一,保险和巨灾债券等灾难风险工具捕捉实际损失的准确程度如何;第二,如何重新设计机构激励机制,使其在奖励建设韧性方面能像目前奖励偿还债务那样具有一致性。

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物理韧性投资不足

在 2024–2025 财年,牙买加拨出约 US\31.5 亿美元 billion 用于偿还债务(\~15.8% of GDP),这大约是其 US\5.1亿美元 公共资本支出总额(\~2.5% of GDP)的六倍 [见补充材料 (SM)]。这种财政结构导致沿海防御设施相对于物理风险而言建设不足,排水基础设施系统被推迟,且关键系统投资不足。

这种失衡在一定程度上反映了目前主权信用评级的评估方式。尽管一些信用评级机构已开始在补充报告中纳入气候风险,但这些因素在核心决策中仍处于边缘地位。主权信用评级的基本框架仍然基于一种狭隘且短期的流动性逻辑:评级机构优先考虑初级盈余的规模、债务与 GDP 比率的下降速度,以及一个国家执行财政规则的严格程度。这种相同的激励结构可能在牙买加之外广泛存在,特别是考虑到有证据表明气候脆弱性会实质性地影响主权信用评级 (3, 4)。尽管存在像绿色气候基金 (GCF) 这样的专项韧性基金,但其范围通常较窄,且相对于本文讨论的更广泛的物理韧性需求而言规模较小。它们也无法解决加剧“毁灭循环”的债务偿还压力或评级机构的激励机制。例如,牙买加首个 GCF 投资项目于 2026 年获得批准,金额为 \5000万美元,主要用于农业韧性项目(见 SM)。换句话说,虽然有韧性资金可用,但其规模可能过小,且与决定政府财政灵活性的主流系统脱节。

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结构性保护缺口

牙买加灾后融资缺口不能仅用投资不足来解释。即使是拥有强大韧性基础设施的国家,在面对极端事件时仍会面临残余损失,而巨灾债券和参数化保险等灾害风险融资工具正是为了解决这一问题而设计的 (5)。这两种工具均基于预定义的物理测量值(如风速、风暴路径和中心气压超标)而非评估的损失金额进行赔付,尽管资金流经不同的市场。在参数化保险中,牙买加直接从区域保险公司 [如加勒比巨灾风险保险基金 (CCRIF)] 购买保单,该机构计算

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保障缺口

对于飓风 Beryl 和 Melissa,巨灾债券(CAT bonds)以及通过加勒比巨灾风险保险 facility (CCRIF) 提供的参数化保险所覆盖的损失不足 3%。

| 飓风 Beryl(4 级,2024 年 7 月)< / > 飓风 Melissa(5 级,2025 年 10 月)< / > | 总损失< / > US10 亿美元 billion< / > US122 亿美元 billion< / >< / > 损失(占 GDP 的 %)< / > ~5%< / > ~57%< / >< / > 巨灾债券赔付< / > US0万美元< / > US1.5亿美元< / >< / > CCRIF + 其他赔付< / > ~US2700万美元< / > ~US9200万美元< / >< / > 覆盖率< / > ~3%< / > ~2%< / > |

一旦损失超过设定阈值,赔付金额将根据风暴的实测严重程度按比例增加(见 SM)。而巨灾债券则通过资本市场运作:例如,世界银行向外部投资者发行债券,如果风暴超过同类阈值,投资者将按照类似的滑动比例损失部分本金,而资金则流向牙买加。无论哪种方式,赔付都是快速且客观的,但它也与灾难的实际成本脱节。参数化工具的赔付额与灾难实际成本之间的差距被称为基准风险(basis risk)。

牙买加近期遭遇的两场风暴说明了其后果。飓风 Beryl(2024 年 7 月)造成的损失估计为 US10 亿美元 billion。然而,牙买加的世界银行巨灾债券没有支付任何款项,因为其测得的强度未达到债券的最低赔付阈值,且 CCRIF 仅覆盖了 US$26.600 万(损失的 2.7%)。相比之下, CCRIF 触发了所有条件,导致全额赔付 US1.5亿美元;当与 CCRIF 的其他援助相结合时,总覆盖金额达到 US2.42亿美元(损失的 2%)(见第一张表格)。

在这两种情况下,这些工具的执行完全符合规定,但对于主权国家而言,这导致了合同履行与财政充足性之间的差距:牙买加的灾难风险融资策略奏效了,工具按设计触发并赔付,但大部分损失仍未得到覆盖。目前的制度架构尚无机制来调和这两个框架 (6)。

扩大参数化覆盖范围会带来年度保费的经常性成本,无论是否发生风暴都必须支付。如果灾后能获得优惠贷款(条款比市场贷款更宽松),长期成本可能与保险保费成本相当。然而,参数化工具相比灾后借贷具有两个关键优势。赔付在登陆后 3 到 14 天内到账,世界银行巨灾债券的赔付在 10 天内得到确认,而牙买加等待国际货币基金组织(IMF)拨款批准则大约需要 3 个月(见 SM)。参数化赔付也不会增加主权债务规模。第二个优势至关重要,因为灾后借入的每一美元都会通过利息产生复利,并挤出未来的资本支出,而保险赔付则不会。

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之后增长的分解

相对于 之前的债务与 GDP 比率,根据标准债务比率会计法, GDP 之后的估计增长是由恢复借贷带来的分子效应和产出损失带来的分母效应共同驱动的。

阶段< / > 公共债务(占 GDP 的 %)< / >< / > 前基准< / > 60%< / >< / > 恢复借贷< / > +6.4 pp< / >< / > GDP 短缺(产出损失)< / > +2.1 pp< / >< / > 后峰值< / > 68.5%< / > |

pp,百分点。

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债务融资恢复

由于参数化工具覆盖的损失不足 2%,政府的恢复融资绝大部分来自新借款,约为 36 亿美元 billion(约占 Melissa 灾前 GDP 的 18%)。仅这一年的借款额就已超过了国际货币基金组织(IMF)债务可持续性框架将新兴市场主权国家视为风险标志的 GDP 流量融资阈值(约 15%),并接近适用于发达经济体的 20% 阈值(见 SM)。Melissa 灾后的新债务分布在 IMF、世界银行和三家区域开发银行,其条款大多未公开(见 SM)。

我们模拟了从优惠利率到接近市场定价的不同条款下的总名义债务(本金加利息):为 49 亿美元 billion 至 57 亿美元 billion(占 Melissa 灾前 GDP 的 24% 至 29%)。在优惠利率下,其净现值低于本金,因此贷款在财政上是一种实质性的让步。然而,限制牙买加的是年度现金支付额,而非其折现值,因为这些支出每年都会与资本预算产生竞争。在还款高峰期,仅新债务的偿还额就将接近或超过牙买加全年的资本预算(见 SM)。

这形成了一个恶性循环:灾后借款恰恰挤占了本可以减少损失的灾前投资。据预测,这种恢复性借款与灾难对产出的抑制效应相结合,将使牙买加的债务与 GDP 比率达到约 68.5% 的峰值,比牙买加在没有这场风暴时预计的约 60% 轨迹增加了 8.5 个百分点(见图表和第二张表格)。

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投资缺口的规模

利用灾害风险文献中的效益成本比,我们估计,每年 3.6亿美元 至 9亿美元(占 GDP 的 1.8% 至 4.5%)的灾前韧性投资本可以完全抵消上述新借款,具体取决于所采用的比率(见 SM)。这些数字无法说明哪些投资效果最好,也无法捕捉实施滞后;尽管如此,它们表明,牙买加所需的韧性投资与其实际能够投资之间的估计缺口是巨大的,且基于既有的效益成本比研究。IMF 2025 年的第四条磋商(一项针对国家经济的健康检查)发现,牙买加每年仅能支出 GDP 的 0.2

至 0.4%(4000万美元 至 8000万美元)用于适应性建设而不会对债务路径造成压力,这比抵消灾后借款所需的资金低 4 到 22 倍。

一旦考虑融资结构,这一缺口将显著缩小:在回报率变为负值之前,公共融资可覆盖约三分之一的总适应成本,其余部分预计由私人资本资助 (7)。如果我们将该比例应用于 3.6亿美元 至 9亿美元 的范围,这意味着政府每年资助的部分约为 1.2亿美元 至 3亿美元。这仍比 IMF 第四条磋商认为的财政可持续水平高出 1.5 到 7.5 倍,但比之前提到的 4 到 22 倍的缺口要小得多。在当前规则下,牙买加能够可持续负担的资金不足以改变其在 Melissa 灾后的轨迹,因为这些规则目前给韧性支出的留下的财政空间从一开始就太小了(见 SM)。

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这种架构使循环持续下去

这种循环之所以持续,是因为每个参与者都对其面临的激励机制做出理性反应,但其综合效果使得借款国和贷款方的处境都比采取协调方案时更糟糕。政府优先考虑偿还债务,因为信用评级信号会对市场准入和借贷成本产生实际影响。评级机构单方面改变这一现状的动力有限:物理韧性指标尚未标准化,其与主权违约概率之间的联系研究不足,且将其纳入将需要重构整个评级框架 (4, 8)。鉴于评级机构将主权风险框架视为可靠的输入项,改革主权风险框架更具可行性。

信用评级机构奖励其框架旨在衡量的内容。在“梅丽莎”飓风后的牙买加案例中,启动灾害风险融资工具、使用纪律严明的优惠贷款,以及通过其财政逃逸条款(在灾害的财政影响超过 GDP 的 1.5% 时触发;“梅丽莎”的影响约为 3.9%)暂时暂停自身的预算规则(见 SM),这些都是财务风险管理方面的实质性改进。但目前的框架未能捕捉到的是,导致危机最初发生的物理暴露程度是否发生了任何变化。像国际货币基金组织(IMF)的债务可持续性分析(DSA)等计划旨在解决主权债务困境。2024年8月的补充说明将气候风险引入了部分计划的 DSA 中,但实施过程仍未成为核心方法论的一部分 (8, 9)。

灾害风险融资工具是超越传统援助机制的真正创新,例如 CCRIF 旨在提供灾后快速流动性,但其局限性在于规模和设计匹配度:为投资者流动性设计的工具不一定适用于国家恢复。目前的架构导致了协调失败,每个机构都在其自身授权范围内理性运作,但集体结果却是全球最脆弱国家在韧性方面的长期投资不足,且只要债务约束与物理风险共存,同样的情况就会在各地重复出现。在这种情况下,仅靠主权财政努力无法弥补差距,因为只有当政府承担适应性支出的反应性部分(即灾难救援和恢复)时,适应性投资才能实现自偿,而私营部门则资助韧性基础设施和预警系统等前瞻性措施。在相关国家中,政府承担的部分平均约占总适应成本的三分之一 (7)。如果政府改为完全自行资助适应性建设,成本将超过节省的金额,而且即使在这种最理想的分摊情况下,也无法完全恢复像牙买加这样高暴露、高债务国家的债务可持续性 (7)。

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打破厄运循环

多层韧性框架——结合财政缓冲(灾难前预留的储备或预先安排的信贷额度)、参数化保险以及债务暂停条款等应急融资——在类似的加勒比经济体中已取得成效 (10)。然而,目前缺失的是构建这三层结构的制度激励。以下干预措施旨在填补这一空白,使财政纪律与韧性投资相互增强而非相互竞争,从而使借款方和贷款方共同受益。所有措施均针对多边机构,因为与评级机构相比,IMF、多边开发银行(MDBs)和主权债务市场对于能够大规模改变市场信号的协调改革更为开放。以下每项改革都强化了其中一层:将韧性纳入 IMF 的 DSA 中可构建将它们联系在一起的激励结构,扩大 RST 的规模可建立财政缓冲,重新校准参数化触发机制可强化保险层,而 CRDCs 则可构建应急融资。

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将物理韧性嵌入 IMF 的 DSA 中

考虑到国际货币基金组织(IMF)在主权稳定性方面的职责、与所有主要借款国的关系以及分析能力,其现有的债务可持续性分析(DSA)框架是将物理韧性在主权风险评估中如何衡量和奖励标准化的最可行路径。将气候风险整合到随机 DSA (9) 中的基础论据是将综合评估模型与债务动态相结合,以捕捉全球变暖如何影响增长、财政成本和主权财富。牙买加 2025 年的第四条磋商代表了朝着这个方向迈出的一步,其中一个气候模块预测了在较高适应性支出下的债务路径(见 SM),但该分析仅询问了该国在不影响债务路径的情况下能负担多少适应性支出。至关重要的是,它没有对反面情况进行建模:当适应性不足且随后发生灾难时,债务可持续性会发生什么?牙买加在“梅丽莎”飓风后的轨迹就代表了这种情况。

气候变暖可能会抑制增长,而增长放缓会削弱债务能力 (9)。除了 DSA 中的这个“缓慢”渠道外,一个“急性”渠道可能会发现,对韧性的投资不足会增加灾难发生的概率和财政严重程度,这需要一种补充方法,在这种方法中,灾前投资作为一种变量进入 DSA,从而改变灾难性损失情景的概率分布。如前所述,为反应性适应提供资金可以达到盈亏平衡,并降低稳定债务所需的基础余额 (7)。削减这项支出以给债务偿还腾出空间并不一定会省钱,反而会放弃政府原本可以获得的收益。这部分份额应受到保护,避免被挤出,而将其嵌入核心 DSA 方法论中可以实现这一点。

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扩大 RST 资金规模

IMF 于 2022 年设立的韧性与可持续性信托(RST)旨在提供优惠融资,应更明确地用于扩大高债务和气候脆弱国家的财政空间。

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牙买加公共债务与 GDP 的轨迹

历史路径显示,债务从 2013 年的 $\sim 144\%$ 下降到 2024 年底的 $\sim 65\%$。在“梅丽莎”飓风之后,债务率预计将达到峰值 $68.5\%$ ,比没有风暴的假设情况($\sim 60\%$)增加了 8.5 个百分点。

早期加勒比地区的试点项目取得了成效,例如巴巴多斯利用 资源偿还高成本债务,并将节省的资金转向关键的水资源和粮食安全 (11)。尽管扩大规模具有强有力的经济理由,但该工具目前的规模相对于财政约束的程度而言仍然不足:大规模气候融资对发达国家捐助者的财政成本在 GDP, 中占比很小,而且支持气候脆弱经济体符合出资国的集体经济利益,而不仅仅是发展义务 (12)。IMF 应当扩大这一方法,并将 RST 的拨款与公共资本支出的可衡量增长明确挂钩。在牙买加的案例中,这将直接解决由于债务偿还义务而导致的挤出机制。

将这一方法推广到大约 35 到 40 个与 IMF 有活跃关系的、高债务且气候脆弱的小岛屿发展中国家(SIDS),将需要总额在 US200 亿美元 billion 到 US300 亿美元 billion 规模的 RST 拨款;如果明确优先考虑气候脆弱的 SIDS,这些数值在当前的 RST 能力范围之内(见 SM)。这要求针对那些 的优惠条款和长期期限能够适配问题的国家进行定向部署,而不是让 IMF 成为每个面临气候风险的主权国家的首席债权人。当与财政缓冲、参数化工具和应急融资相结合时,与 RST 挂钩的承诺对 IMF 自身资源的负担较轻 (10)。

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气候韧性债务条款 (CRDCs)

CRDCs 允许借款人在灾难发生后的最多 2 年内递延本金和利息,从而在不增加新债务的情况下,将现有资金转向应急响应。73 个国家以及世界银行和美洲开发银行等主要多边开发银行(MDBs)已承诺实施 (13)。2026 年 4 月,惠誉评级(Fitch Ratings)修订了其主权评级标准,明确指出,在设计良好的暂停条款中,基于规则且有上限的付款递延无需被视为违约,前提是触发条件和保护措施已明确规定 (14);穆迪评级(Moody's Ratings)已参与讨论,但尚未发布相应的修订。债券持有者最初持抵触态度,但现在越来越多地将结构良好的 CRDCs 视为信用增强手段,因为付款的灵活性降低了无序违约的可能性。

应急债务工具已被提出数十年,但很少被采用。其中最著名的尝试是 GDP 挂钩债券,但存在三个问题:触发条件与政府可以影响的 GDP 数据挂钩、定价困难(见 SM),以及发行历史主要集中在陷入困境的债务重组期间。CRDCs 解决了这些问题:风暴触发条件无法被操纵,且标准化的开发银行模板为市场提供了早期工具所不具备的共同参考。像巴巴多斯这样的国家已将其作为预防措施采用,这是基于财政实力而非在危机期间采取的 $13$。CRDCs 是对参数化工具的补充而非替代:当风暴达到触发条件时,巨灾债券提供流动性,而 CRDC 则在宣布紧急状态后递延付款,无论风暴路径如何。

协调仍然是主要障碍,因为其价格本身很低。世界银行对其 CRDC 选项收取的费用仅为拨付余额的 0.05%,且条款的透明度和披露优势甚至可以抵消这一成本 $(13)$。更深层的挑战在于 CRDCs 的使用方式,因为大多数条款是在债务重组期间添加的,而不是在最初借款时就写入,这使得整个概念与财务困境挂钩,从而令那些最能从中受益的国家望而却步。如果牙买加的债务在梅丽莎(Melissa)风暴之前就包含标准 CRDC 条款,其债务偿还将自动暂停,但这种益处只有在暂停适用于该国所有债务时才成立,这意味着必须在包括双边贷款方、开发银行和私人债券市场在内的所有资金来源中统一条款语言。

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重新校准参数化触发机制设计与承保限额

参数化工具需要在两个方面进行重新校准。首先,触发机制的设计应向多参数指数方向发展,使其在成为保险问题的同时,也成为一个风险建模问题:将降雨累积量、风暴潮和风速纳入其中,并在更小、更局部化的网格单元而非大型区域网格上定义触发条件。这将有助于降低基准风险(basis risk),此前尽管贝丽尔(Beryl)造成了数十亿美元的损失,但牙买加的赔付额仍为零 (5)。参数化-补偿混合结构(hybrid parametric-indemnity structures)可以成为弥合合同履行与实际恢复之间差距的直接途径,在这种结构中,参数化触发机制启动即时流动性,而理赔调整过程则决定补充补偿部分(即基于实际核实损失的赔付)。这一点至关重要,因为传统的损失核实保险实际上无法独立提供给主权国家,因为以这种方式为整个国家的损失承保需要现场评估员,且耗时数月(而这正是最初创建参数化工具的原因)。混合结构将同时提供参数化触发的快速性和核实的准确性。

其次,应通过让多边开发银行(MDBs)以额外的风险资本或担保为这些工具提供支持,从而扩大承保限额,使风险池本身能够安全地支持更大规模的赔付。其运作方式是增加风险池能够覆盖的损失规模,而不是改变任何单个国家的保费设定方式。即使风险池的总容量增加,保费仍可根据一个国家的实际风险状况进行缩放。这一区别很重要,因为如果保费不再反映一个国家的实际风险敞口,那么继续投资于旨在降低风险的韧性措施就几乎没有理由了。多边开发银行的资本化通过扩大风险池的赔付能力,同时让每个国家的保费与其自身风险挂钩,从而避免了这一问题。

成本权衡仍然是一个关键点:虽然多参数触发机制提高了精算效率,但混合结构的单笔保单成本高于纯参数化结构,这种增加的成本需要与灾后可帮助避免的借贷成本进行权衡。对于资金最紧张的主权国家,通过联合国“损失与损害基金”等气候基金提供的优惠保费融资可以吸收这部分成本。这些改革将使灾害风险融资能够满足国家恢复需求,而不仅仅是专注于提供市场流动性。

牙买加从十多年艰苦赢得的财政纪律,到在短短几周内出现剧烈逆转,这是一个紧迫的信号,表明制度框架未能跟上气候变化的步伐。导致牙买加这一结果的制度条件是结构性的,只要信用评级在衡量财政纪律时而不考虑有助于维持该纪律的物理韧性,这种情况就会在任何地方再次出现。在物理风险加剧的情况下,改革主权韧性的衡量、融资和奖励方式,是使财政纪律具有实际意义的前提条件。$\square$

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参考文献与注释

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2. 牙买加规划研究所 (Planning Institute of Jamaica),《飓风 Melissa 的社会经济和环境影响评估》(与联合国拉美经委会 [UN ECLAC] 及牙买加政府共同准备的损失与损害评估,牙买加规划研究所,2026);https: / jis.gov.jm / total-loss-and-damage-from-hurricane-melissa-estimated-at-1-952-trillion / .

3. S.A. Zenios, Curr. Opin. Environ. Sustain. 67, 101414 (2024).

4. P. Klusak, M. Agarwala, M. Burke, M. Kraemer, K. Mohaddes, Manage. Sci. 69, 7468 (2023).

5. 金融稳定研究所 (Financial Stability Institute),国际保险监督员协会 (International Association of Insurance Supervisors),“不确定的水域:参数化保险能否帮助弥补自然灾害 [NatCat] 的保障缺口?”(FSI 政策实施洞察 No. 62,国际结算银行,2024);https: / www.iais.org / uploads / 2024 / 12 / FSI-IAIS-Insights-on-parametric-insurance.pdf.

6. D. J. Clarke, S. Dercon, Dull Disasters? How Planning Ahead Will Make a Difference (Oxford Univ. Press, 2016).

7. M. Calcaterra, A. Consiglio, V. Martorana, M. Tavoni, S. A. Zenios, “Sovereigns on thinning ice: Debt sustainability, climate impacts and adaptation,” Working paper 06 / 2025, Bruegel, 2025; https: / www.bruegel.org / working-paper / sovereigns-thinning-ice-debt-sustainability-climate-impacts-and-adaptation.

8. 国际货币基金组织 (International Monetary Fund), “Staff guidance note on the debt sustainability framework for low-income countries: Supplemental guidance on climate change” (IMF, 2024); https: / www.imf.org / en / publications / policy-papers / issues / 2024 / 08 / 05 / supplement-to-2018-guidance-note-on-the-bank-fund-debt-sustainability-framework-for-low-553151.

9. S.A. Zenios, Clim. Change 172, 30 (2022).

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14. 惠誉评级 (Fitch Ratings), “Sovereign Rating Criteria” (Fitch Ratings, 2026年4月27日).

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致谢

作者感谢 K. Mackenzie 和 S. Evans 对手稿提供的专家评审和反馈。资金由东北大学的 Lizzy Warner Fellowship (A.M.) 以及美国国防部的战略环境研究与发展计划 (RC20-1183 to A.R.G.) 提供。E.K. 同时受雇于洲际交易所数据服务公司 (Intercontinental Exchange Data Services),但在此仅以东北大学兼职教师的身份做出贡献。此处表达的观点仅代表作者个人,不反映洲际交易所数据服务公司的观点。

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补充材料

10.1126 / science.aeh3608

$^{1}$ 美国马萨诸塞州波士顿,东北大学,可持续发展与数据科学实验室。$^{2}$ 美国华盛顿特区,公共企业中心。$^{3}$ 美国马萨诸塞州波士顿,东北大学,体验式人工智能研究所,气候与可持续发展人工智能。电子邮件:mishra.aay@northeastern.edu; a.ganguly@northeastern.edu

研究

在《科学》期刊中

编辑

Michael Funk

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神经科学 运动控制的表观遗传制动器

血管与神经元之间的相互作用支撑着中枢神经系统的功能。Lu 等人发现了一种血管特异性机制,该机制对于大脑运动协调中心的神经回路发育至关重要(另见 Bonanomi 的 Focus 报道)。甲基转移酶 PRMT5 在表观遗传层面抑制了编码血管重塑因子 ANGPTL4 基因的表达。脑内皮细胞 PRMT5 缺失的小鼠分泌大量 ANGPTL4,这增加了进入小脑的抑制性突触输入,并导致进行性运动功能缺陷。这些发现扩展了神经血管耦合在发育中的作用。——Leslie Ferrarelli Sci. Signal. (2026) 10.1126 / scisignal.aed6605; 10.1126 / scisignal.aek9091

基于磁共振成像重建的可视化脑血管

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分子生物学

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ncRNA 调节基因表达动力学

基因组的大部分并不编码蛋白质,而是产生非编码 RNA (ncRNAs),其功能在很大程度上仍然是个谜。Batut 和 Levine 利用发育中果蝇胚胎的活体成像发现,这些 ncRNA 有助于控制蛋白质编码基因开启的时间和强度。对于 Hox 基因 Scr,由远端增强子产生的 会延迟其激活,而来自“系留”元件的 则会增强其表达。破坏增强子 RNA 会加强长程 DNA 接触,导致 Scr 提前激活。这些发现表明, 有助于塑造基因组组织和全基因组的长程通信,确保发育过程中基因表达的精确时间和水平。

——Di Jiang

Science p. 402, 10.1126 / science.aek5696

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机器学习 AI 的逐步诊断

AI 在临床医学中的应用持续推进,但通常依赖于书面病例摘要。遗憾的是,这不能真实代表临床医学,因为患者就诊时并不会提供一份关于关键症状和相关实验室检查结果的整洁报告。为了解决这个问题,Nori 等人使他们的 AI 系统从患者的主诉开始,决定询问哪些后续问题以及开具哪些检查,以收集诊断所需的信息。在多种测试设置中,该系统的准确率高于人类响应者,且总成本更低,证明了其作为辅助医生工具的潜力。——Yevgeniya Nusinovich

Science p. 423, 10.1126 / science.aeh7930

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凝聚态物理 阐明声子

热霍尔效应 (THE) 是指在垂直磁场存在的情况下,响应纵向热流而出现横向温度梯度,该效应已在多种材料中被观察到。根据材料是金属还是绝缘体,以及是否表现出磁有序,THE 被分别归因于电子、磁振子,以及最近的声子。但声子究竟如何引起 THE 仍存在争议。Meng 等人研究了蜂窝状反铁磁体 $\text{NiPS}_3$ 中的这种效应。通过测量五个不同的样本,研究人员发现 THE 的幅度与磁各向异性的程度相关。结合计算结果(表明该材料中存在磁振子-声子能带交叉),这些结果与一种可能由磁振子-声子杂化驱动的内禀声子 THE 相一致。——Jelena Stajic

Science p. 419, 10.1126 / science.adt1992

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膜

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旋转门加速流动

多孔膜通道中的离子物种可用于增强膜的选择性,但由于通道变窄,这通常会以牺牲流速为代价。Zhang 等人将铵离子引入分层 MXene 膜中。自旋转的铵功能基团使原本静态的亚纳米通道具备了动态响应能力,从而实现了快速且选择性的传输。

—Marc S. Lavine

Science p. 434, 10.1126 / science.aed8319

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二维材料 可视化强关联相

堆叠的范德华材料中的莫尔超晶格承载了多种具有强电子关联的相。两个研究小组使用扫描隧道显微镜对这些相进行了可视化,并调整实验条件以诱导其熔化。Berger 等人专注于扭曲的二硒化钼双层膜,其三角形莫尔超晶格承载了晶体电子态。研究人员在改变载流子密度时,观察到电子晶体发生熔化:当加入电子时,它变为均匀的类液体状态;而当系统掺杂空穴时,则变为无序状态。He 等人研究了与六方氮化硼完全对齐的 Bernal 堆叠双层石墨烯。将样品置于外部磁场中重塑了电子能级,导致强关联拓扑态的形成。对这些状态的直接成像揭示了其复杂的结构,并阐明了其量子熔化的过程。—Jelena Stajic

p. 450, 10.1126 / .aef0940,

p. 440, 10.1126 / .aee6967

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保育生物学 水来了

全球变暖导致海平面上升,淹没并改变了沿海生态系统。海平面上升已经导致沿海物种数量下降,甚至出现了灭绝。Jiang 等人在全球尺度上评估了预计未来海平面上升对陆生脊椎动物多样性的影响程度。他们发现,根据分类群和预测的不同,有五分之一到三分之二的物种在其栖息地的某些部分将面临海平面上升的影响,其中东南亚的高多样性物种受威胁程度尤为严重。在保育优先事项中考虑海平面上升的避难所,对于未来保护物种可能至关重要。—Bianca Lopez

p. 408, 10.1126 / .aed5772

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天然产物 构建富氮化合物

胍基存在于许多源自植物和微生物的生物活性小分子中,但安装这一功能基团在化学上具有挑战性。Kolling 等人鉴定了一组参与产生含胍天然产物的异戊烯基转移酶,并发现它们能结合并激活游离胍作为亲核试剂来攻击异戊烯基二磷酸。晶体结构和生化实验确立了这一转化的机制。研究人员测试了来自植物和细菌的多种具有类似活性的酶,从而为这一重要类天然产物的生产奠定了遗传基础。—Michael A. Funk

p. 413, 10.1126 / .aeg1821

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其他期刊

编辑:Corinne Simonti 和 Jesse Smith

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植物传感器

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一种用于植物的健康传感器

吐水现象(Guttation)是指液体通过叶缘被称为水孔(hydathodes)的小孔释放,这种情况发生在根压超过蒸腾作用时。吐水现象为植物的营养、代谢和压力状态提供了易于获取的读数,但由于其体积小且蒸发快,使得连续采样变得困难。借鉴人类的非侵入式汗液传感器,Xue 等人设计了一个名为 Plantlonics 的微流控电化学监测平台。其受猪笼草边缘启发而设计的楔形微通道,提供了自驱动的单向流动。一个多通道传感阵列可测量钠、钾和葡萄糖,以及叶片上的温度和湿度。这使得在数天内对多种植物物种中这些生物标志物因压力引起的改变进行非侵入式监测成为可能,代表了向精准农业迈出的一步。——Unnati Sonawala

Nat. Commun. (2026)

10.1038 / s41467-026-77955-6

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细胞生物学 理解着床失败

女性生育能力在 35 岁之后大幅下降。Cavanaugh 等人通过将老年小鼠模型与体外受精(IVF)临床数据集进行对比,研究了与年龄相关的不孕症。来自高龄雌性小鼠胚胎的过度强收缩力损害了胚胎细胞的命运决定和着床。小鼠模型复制了人类在妊娠结果和体外着床测定中观察到的与年龄相关的缺陷。一种围着床期的年龄相关缺陷涉及胚胎表面张力、基质粘附力和粘度的增加,这限制了着床期间的铺展。非侵入性成像特征预测了来自年轻和高龄雌性小鼠胚胎的着床成功率。因此,胚胎力学可以调节生殖寿命,为筛选胚胎以改善 IVF 结果提供了一条潜在途径。

——Stella M. Hurtley

Nat. Cell Biol. (2026)

10.1038 / s41556-026-02052-1

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二维材料 附着于表面

含有金属元素的原子级薄晶体(如金属间化合物和高熵金属合金)可以表现出电子设备所需的独特物理和化学性质。然而,由于热力学不稳定性和动力学限制,合成这些材料的二维(2D)薄膜一直具有挑战性。Zhang 等人报道了一种吸附-转化法,可以使用金属氯盐合成广泛的高质量金属间化合物和高熵金属合金薄膜。在氢环境下,吸附的金属氯化物化合物在表面被还原,释放的金属原子降低了表面能。吸附的氯原子进一步抑制了垂直的 3D 生长。该方法在实际基底上产生了尺寸为几十微米的超薄薄膜。——Sumin Jin

Nat. Mater. (2026)

10.1038 / s41563-026-02752-x

公共卫生

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被紧凑、弯曲的绿地冷却

城市绿地与降温和减少与热相关的疾病相关。绿地的组织方式似乎也很重要,尽管这在标准空间分辨率下尚未得到很好的解决。Wang 等人将 2016 到 2023 年的州级健康记录叠加在亚利桑那州 2000 多个社区的 1 米航空图像上。正如预期的那样,更多的绿地与热相关疾病的减少相关。然而,同样重要的是绿地的复杂性和连通性。他们的研究结果表明,城市绿化降温计划应考虑空间的形状和连接,而不仅仅是其规模。——Angela Hessler

GeoHealth (2026) 10.1029 / 2026GH001978

城市绿地(如澳大利亚阿德莱德的 Rymill 公园)带来的益处与其形状和连通性相关。

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锕系元素化学 碳与铀形成三键

在费舍尔卡宾(Fischer carbyne)中,一个碳原子与金属形成三键,并与氧或氮取代基形成单键,且沿轴线具有一定的电子离域潜力。过渡金属已有多种此类示例被表征,而 Seed 等人现在将这一成键范式扩展到了铀。具体而言,三酰胺铀配合物与二氮磷叶立德的反应产生了一个双核配合物,其铀中心由一个 CNN 桥连接。晶体学、光谱学以及理论研究均支持碳与铀之间具有三键特性。—Jake S. Yeston

Nat. Chem. (2026)

10.1038 / s41557-026-02260-0

毒理学

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甲醛对大脑的影响

甲醛是最简单的毒性物质之一,如果高浓度吸入,可引起急性刺激和严重的长期后果(如癌症)。虽然也有研究声称其与抑郁症相关,但此类影响的分子机制仍缺乏充分研究。Xu 和 Shen 通过使用循环伏安法分析暴露于甲醛的小鼠大脑活动,探讨了这一问题。他们发现,这种处理降低了伏隔核中多巴胺的刺激性释放。作者提出这可能与肠道微生物群的变化有关,但若要全面理解并验证这些影响,仍需进一步的机制实验。—Michael Funk

ACS Chem. Neurosci. (2026) 10.1021 / acschemneuro.6c00121

植物生物学

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树木通过感知来自我矫正

树木通过对重力和光的响应来保持树干直立,但尚不清楚它们是否也能感知并矫正自身的弯曲。Caulus 等人研究了杨树是否利用一种被称为本体感受(proprioception)的自身形状感知能力来主动矫正弯曲的茎干,而非被动地回弹。通过倾斜幼杨树并使其旋转以抵消重力感知,作者发现树木仍然能自我矫正,生长出一种类似肌肉的“张力木”,该组织从茎的一侧转移到另一侧,从而将其拉回原状。这可能意味着树木会主动监测并矫正其姿态,这有助于提高木材质量以及培育更耐风暴的作物。—Di Jiang

New Phytol. (2026) 10.1111 / nph.71238

癌症

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STAT2 内含子保留与免疫疗法

选择性 RNA 剪接是一种调节过程,允许一个基因编码多种信使 RNA (mRNA) 异构体,从而产生具有不同功能的蛋白质。Englander 等人利用长读长 RNA 测序,绘制了肺腺癌中的选择性剪接 mRNA 变体图谱,肺腺癌是一种对当前疗法仅部分响应的癌症类型。研究在免疫相关基因中识别出数千种 mRNA 异构体,且信号转导与转录激活因子 2 (STAT2) 基因中的内含子保留事件导致了改变的蛋白质异构体的产生,这些异构体调节免疫信号传导和干扰素响应。这些分子变化与肺癌患者对抗 PD-L1 免疫疗法的响应相关,表明 STAT2 基因中受调控的内含子保留可能影响治疗结果。—Priscilla N. Kelly

—Priscilla N. Kelly

Science p. 397, 10.1126 / science.aea7156

太阳能电池

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柔性钙钛矿组件的锚定技术

将自组装单分子层(SAMs)与钙钛矿的沉积过程解耦,能够制造出具有高能量转换效率(PCE)的柔性钙钛矿组件(PSMs)。由于柔性基底上脱附的表面羟基会干扰 SAM 的组装,导致柔性器件的稳定性和 PCE 低于刚性器件。Wu 等人利用一种钝化剂加速了 SAM 的锚定,并减少了其对钙钛矿薄膜形成的干扰。一个 25 平方厘米的柔性器件在 85℃ 和 65% 相对湿度的最大功率点追踪 1044 小时后,仍保留了其 22% 的初始 PCE 的 92.5%。—Phil Szuromi

编辑:Michael Funk

Science p. 398, 10.1126 / science.aef9745

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人工智能 AI 智能体协同作战

传统的药物研发是一个劳动密集型且昂贵的过程,不同步骤需要由不同的团队分别完成。Zhang 等人设计了“虚拟生物技术”(Virtual Biotech)方法以简化早期药物研发,该方法采用由专业 AI 智能体团队组成的集成工作流,并由一名担任首席科学官的智能体统一指挥。与任何 AI 驱动的生物研究一样,这些智能体的建议需要通过合成候选药物并进行测试来转化为现实世界的成果。这种方法仅适用于具有足够背景数据供 AI 解释的疾病,但它可能有助于发现那些原本会被遗漏的治疗机会。

—Yevgeniya Nusinovich

p. 399, 10.1126 / .aeg6779

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代谢 告别过量葡萄糖

糖尿病和肥胖在世界范围内变得越来越普遍,且两者经常共存并相互增强。目前已有多种药理学和生物学干预手段,但每种手段都有其优缺点,许多患者仍需要耐受性更好、更有效和 / 或更经济的治疗方案。Maity 等人开发的一种植入式设备有助于填补这一空白,它提供了一种无需药物或胰岛素即可调节血糖浓度的可控方式(参见 Bentley 和 Payne 的观点文章)。该无线供电设备可与临床可用的连续血糖监测仪相连,以催化葡萄糖转化为葡萄糖酸,随后由肾脏排出。在小鼠实验中,该设备使血糖恢复正常,并同时清除了一部分过量的热量负荷。

—Yevgeniya Nusinovich

p. 400, 10.1126 / .ady8560;另见 p.382, 10.1126 / .aem0762

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细胞生物学 线粒体决定死亡机制

对程序性细胞死亡的控制是从发育到癌症治疗等多种过程的核心。导致细胞凋亡死亡的一个关键事件是线粒体外膜的通透化。这通常会导致细胞色素 c 的释放以及 caspase 和凋亡小体的激活。如果这一凋亡死亡过程未能完成,线粒体 DNA 也可能泄漏,从而引起非 caspase 依赖性细胞死亡和炎症。Yang 等人表明,细胞色素 c 的释放和线粒体 DNA 的释放是两个独立的生化过程(参见 Muñoz-Pinedo 和 Martin 的观点文章)。它们分别由仅由 BAK 和 BAX 蛋白形成的复合物,或由 BAK 和 BAX 与其他蛋白结合形成的大复合物所介导。作者将后一种形式的细胞死亡称为“baciptosis”,这在凋亡小体缺陷的人类癌症中可能具有特殊的重要性。—L. Bryan Ray

p. 401, 10.1126 / .aea2181;另见 p. 383, 10.1126 / .aem1247

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比较认知 飞行中的快速思考

鸟类大脑曾被轻视,但现在越来越清楚的是,尽管它们在结构上与哺乳动物不同,但能提供高度类似的认知功能。在基于视觉输入做出快速决策的能力方面,由于鸟类在飞行过程中依赖快速移动,它们承受着一些最强的选择压力。Schmidbauer 和 Neider 测试了寒鸦的决策速度,发现其速度大约是灵长类动物的两倍(参见 Colombo 和 Poutrain-Sorel 的 Perspective 评论)。此外,对 nidopallium caudolaterale(灵长类前额叶皮层的功能类似物)中神经元的记录显示,其选择信号呈现出递增趋势,与灵长类动物在决策过程中该区域内观察到的信号相似。

—Sacha Vignieri

Science p. 445, 10.1126 / science.aed6459; 另见 p. 385, 10.1126 / .aem0341

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冰川起始 人为导致的冰期逆转

人为变暖是否阻止了下一个冰川周期?Young 等人表明,情况可能正是如此(参见 Marcott 的 Perspective 评论)。他们研究了加拿大巴芬岛上巴恩斯冰帽的演变,这是劳伦泰德冰盖(LIS)最后残存的部分,该冰盖曾覆盖北美大部分地区,是更新世最大的冰盖。在全新世早期和中期的大部分时间里持续萎缩后,LIS 在大约 2000 年前开始重新增长,但随后在 1960 年左右再次开始萎缩。作者将

这种逆转归因于人为的温室气体强迫,这证明了人类导致了下一个冰期的终止。

—Jesse Smith

p. 455, 10.1126 / .aed3379; 另见 p. 381, 10.1126 / .aem3295

物理学

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困在金属海中

连续谱中的束缚态(BIC)是指能量位于空间扩展态连续谱之内的局域态,出现在由波动方程描述的系统中。由于可视化金属中的电子 BIC 较为困难,这类状态主要在光子和声学系统中被观察到。Thinel 等人使用扫描隧道谱法测量了 $Pd_{5}AlI_{2}$ 的局域状态密度,这是一种具有装饰棋盘格晶格的范德华金属。在被鉴定为钯缺陷的位点上,作者观察到在金属连续谱内部能量处存在尖锐且孤立的峰值,但在电子上与连续谱状态解耦。计算表明,这些电子 BIC 状态源于与受挫跳跃相关的平带,这一机制可推广到多种类型的晶格。—Jelena Stajic

p. 429, 10.1126 / .adt9825

T 细胞

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糖基化决定 γδ T 细胞的命运

γδ T 细胞在维持组织稳态中发挥重要作用,但在炎症条件下会失调。Santos-Pereira 等人揭示了 γδ T 细胞的糖组在 γδ T17 细胞命运决定中起重要作用,促进了一种超激活的促炎状态,从而加剧免疫介导的炎症性疾病。对人类转录组数据和鼠类模型的分析表明,β1,6 N-乙酰氨基葡萄糖分支 N-聚糖的缺失促进了产生 3 型白细胞介素-17A 的 γδ T 细胞以及耐受性的丧失。在糖工程小鼠模型中,N-聚糖分支的缺失增加了对银屑病、红斑狼疮和炎症性肠病的易感性。为 γδ T 细胞补充 N-乙酰氨基葡萄糖减轻了疾病病理和 γδ T17 细胞的激活,揭示了糖生物学在 γδ T 细胞行为中的重要性以及疾病干预的策略。

—Leoma Bere

Sci. Immunol. (2026)

10.1126 / sciimmunol.aec9553

内含子保留调节 STAT2 功能并与肺癌免疫治疗反应相关

全文及作者所属机构列表:https: / doi.org / 10.1126 / science.aea7156

Ryan P. Englander, Mattia Brugiolo, Maëva Devoucoux, Te-Chia Wu, Mitch Kostich, Nathan K. Leclair, Isha Walawalkar, Hyeon Gu Kang, SungHee Park, Florentina Marches, Mark E. Peeples, Phylip Chen, Jacques Banchereau, Peter Yu, Andrew Salner, Romain Banchereau, Karolina Palucka†, Olga Anczuków†\*

引言:免疫检查点阻断改变了肺癌的治疗方式,但大多数患者仍然没有反应,且治疗反应的分子决定因素尚未被完全理解。替代 RNA 剪接(细胞通过选择性地包含外显子或内含子,从单个基因产生多种信使 RNA (mRNA) 异构体的过程)在包括肺癌在内的癌症中经常出现失调。然而,它对抗肿瘤免疫和免疫治疗反应的贡献尚未得到充分表征。

基本原理:肿瘤中的剪接改变经常产生与标准对应物相比功能改变或受损的异构体,这可能会影响肿瘤生长和治疗反应,但这些异构体中的很大一部分在功能上仍未被表征。长读长 RNA 测序(捕获全长转录本而非短片段)显著提高了在健康和疾病状态下识别并从功能上解释这些异构体的能力。该方法此前已被用于编目肺癌细胞系中的异构体,但尚未应用于原发性人类肺肿瘤。

结果:我们将长读长 RNA 测序应用于原发性人类肺腺癌样本,以绘制最常见肺癌亚型的替代剪接图谱。我们识别出超过 149,000 个全长 mRNA 异构体,其中一半以上未被注释,且许多出现在免疫相关基因中。具有免疫相关性的异构体在参与干扰素反应的基因中富集,而该通路在肿瘤的免疫激活和抑制中都处于核心地位。在这些基因中,我们识别出 STAT2 中的两个保留内含子,STAT2 编码一种 I 型干扰素信号传导所需的转录因子;这两个内含子在肿瘤中均上调,且被预测会破坏正常的蛋白质功能。我们对这两种异构体进行了功能表征:任何一个内含子的保留都会导致全长 STAT2 蛋白减少,但内含子 12 的保留特异性地产生了一种截短的异构体,该异构体能主动抑制干扰素信号传导,而不仅仅是无法支持该信号传导。在抑制无义介导的 mRNA 降解(一种在肿瘤中经常减弱的通路)后,这种显性负性异构体在肺腺癌细胞系中表达。最后,我们分析了肺癌和尿路上皮癌临床试验的治疗前 RNA 测序数据,发现这两种 STAT2 内含子保留异构体的相对丰度与检查点阻断反应相关,且显示出比现有生物标志物更强的回顾性关联。

结论:替代 RNA 剪接是一种普遍且在功能上至关重要的基因调节层级,但其在癌症生物学中的作用尚未被完全定义。在此,我们证明替代剪接调节了肺癌中涉及免疫反应的基因功能,包括 STAT2。STAT2 中的内含子保留通过

STAT2内含子保留破坏干扰素信号传导,并与检查点阻断反应相关。原发性肺腺癌的长读长RNA测序识别出149,673个全长异构体,其中超过一半未被注释。内含子6的保留导致全长STAT2减少,从而降低干扰素刺激基因(ISG)的转录,而内含子12的保留则产生了一种能够积极抑制信号传导的显性负性异构体。内含子6与内含子12保留之间的差异与患者队列中的抗程序死亡配体1(PD-L1)反应相关。FL,全长;ISRE,干扰素刺激响应元件;ri12,内含子12保留。

两种截然不同的机制:在肿瘤中无义介导的衰减被抑制的情况下,功能性蛋白的耗竭以及显性负性异构体的产生。这些内含子保留异构体的相对水平代表了一种与检查点阻断反应相关的候选生物标志物,这有待前瞻性验证。更广泛地说,通过该方法揭示的未注释异构体多样性的规模表明,原发性肿瘤的长读长RNA测序可能会揭示除STAT2之外,具有临床实用价值的其他功能相关异构体。这些发现确定了一种此前未被认识的基于剪接的免疫治疗反应机制,在进一步临床评估后,可能对未来的患者分层策略产生影响。

癌症

内含子保留调节 STAT2 功能并与肺癌免疫治疗反应相关

Ryan P. Englander $^{1,2}$ , Mattia Brugiolo $^{1}$ , Maëva Devoucoux $^{1}$ , Te-Chia Wu $^{1}$ , Mitch Kostich $^{1}$ , Nathan K. Leclair $^{1}$ , Isha Walawalkar $^{1}$ , Hyeon Gu Kang $^{1}$ , SungHee Park $^{1}$ , Florentina Marches $^{1}$ , Mark E. Peeples $^{3,4,5}$ , Phylip Chen $^{3}$ , Jacques Banchereau $^{1,6}$ , Peter Yu $^{7}$ , Andrew Salner $^{7}$ , Romain Banchereau $^{8}$ , Karolina Palucka $^{1,9\dagger}$ , Olga Anczuków $^{1,9,10\dagger*}$

使用检查点抑制剂的免疫治疗彻底改变了癌症治疗,并为包括肺癌在内的多种疾病的治疗带来了显著的治疗进展。然而,导致患者预后差异的分子决定因素仍不清楚。利用长读长 RNA 测序,我们绘制了人类原发性肺腺癌中替代 RNA 剪接的图谱。我们鉴定出超过 149,000 种全长信使 (mRNA) 异构体,其中超过一半未被注释,且许多异构体出现在免疫相关基因中,特别是 I 型干扰素响应通路内。我们对 STAT2 基因中的保留内含子进行了功能表征,这些内含子产生了调节免疫信号传导和干扰素响应的改变蛋白异构体,并与抗程序性死亡配体 1 (PD-L1) 免疫治疗后的患者生存率相关。这些发现将替代剪接定位为肿瘤免疫响应的调节因子,并揭示了 STAT2 中的内含子保留是一个与 PD-L1 检查点抑制剂反应相关的干扰素调节轴。

肺癌是全球主要的死亡原因,其中肺腺癌 (LUAD) 是最普遍的亚型 $(1)$。诸如抗程序性细胞死亡蛋白 1 (PD-1) 抗体等检查点抑制剂免疫疗法显著提高了 LUAD 患者的总生存率 $(2, 3)$。这些疗法通过阻断降低内源性肿瘤反应性 CD8$^{+}$ T 细胞效应功能的免疫抑制通路,从而促进抗肿瘤免疫响应;然而,许多患者对该治疗没有反应,且现有的生物标志物无法充分预测反应 $(4)$。为了改进免疫治疗,深入了解调节 LUAD 中免疫功能的分子通路至关重要。

替代 剪接是一种普遍的转录后过程,可从单个基因产生多种 mRNA (5),这可能是更精确地理解肿瘤免疫响应的关键。尽管人类几乎所有多外显子基因都经过替代剪接,但大多数异构体仍未被表征 (6, 7)。癌症中的剪接经常发生改变,以有利于致癌和免疫逃逸异构体的产生 (8–11),但 LUAD 中这些变化的底层机制尚不清楚。

长读长 测序 (-seq) 允许对全长转录本进行测序,因此能够进行比使用传统短读长 -seq 技术更深层的功能分析 $12-14$。然而,迄今为止,长读长 -seq 仅被应用于 LUAD 细胞系的替代剪接研究,而非原发性肿瘤 $15-17$。在其他癌症类型的原发性肿瘤中,长读长 -seq 揭示了数千种此前未被表征的异构体 $18-21$,凸显了其在 LUAD 中发现具有生物学和临床相关性异构体的潜力。

利用长读长 RNA-seq 和一个多级分析平台,我们绘制了 LUAD 肿瘤中的全长 mRNA 异构体图谱。许多源自长读长的异构体影响了免疫通路中的基因,尤其是干扰素 (IFN) 信号传导。包括 I 型 (IFN-I) 和 III 型 (-III) 在内的干扰素在抗肿瘤免疫和免疫逃逸中发挥着双重作用 $22–27$。我们利用长读长 RNA-seq 在 STAT2 基因中识别并表征了两个保留内含子,STAT2 是一种对于传导 -I 和 -III 响应至关重要的转录因子。这些事件损害了 RNA 的响应能力,在肿瘤中富集,可通过基于 RNA 的方法进行靶向,并且在回顾性分析中与程序性死亡配体 1 (PD-L1) 抑制后的患者生存率相关。我们的研究结果强调了长读长 RNA-seq 在发现癌症免疫调节机制方面的实用性。

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长读长 RNA-seq 揭示人类肺肿瘤中数千个未注释的可变剪接异构体

为了探究人类肺癌的可变剪接图谱,我们分别使用 PacBio 单分子实时 (SMRT) 循环一致性测序和 Illumina 测序,对 12 例 LUAD 肿瘤的 RNA 进行了配对的长读长和短读长 -seq(表 S1, A 至 C)(图 1A)。全长异构体使用异构体测序 (Iso-seq) 流水线进行组装、比对、精炼,并合并为一个统一的转录组 (28, 29)。通过长读长检测到的未注释剪接接头使用来自同一 样本的配对短读长 -seq 进行了验证。我们进一步使用正交数据集验证了转录本的 5' 和 3' 边界,包括现有的参考转录组注释以及先前绘制的多聚腺苷酸化和转录起始位点 (30–34)。我们通过系统地改变这些参数的严苛程度,确定了经验优化后的截断值(图 S1A 和表 S1, D 至 H)。为了评估哪些过滤参数对异构体分类最重要,我们在数据集上训练了梯度提升机器学习分类器,以评估每个参数在区分真实异构体与伪影方面的重要性(图 S1, D 至 I)。高质量异构体被进一步过滤为在 ≥1 个样本中具有 ≥5 条长读长,或在 ≥2 个样本中具有 ≥3 条长读长,并使用 SQANTI3 结构类别进行注释 (35)。经过严格过滤,我们从 18,300 个位点中识别出 149,673 个全长 mRNA 异构体(图 1B 和图 S1B),其中 51% 的异构体与参考转录组相比为未注释(图 1B 和表 S2A)。跨肿瘤的异构体定量显示,患者之间的结构类别比例是一致的(图 S1C 和表 S2B)。值得注意的是,具有未注释剪接接头([目录内新异构体 (NIC) 和目录外新异构体 (NNC) 类别])的异构体中,有 56% (n = 33,267) 在 ≥50% 的患者中被发现,这表明某些由长读长衍生的未注释异构体是 LUAD 转录组的复现成分(图 1℃ 和表 S2B)。此外,各结构类别的异构体表现出比最接近的匹配参考序列更短的 3' 非翻译区 (UTR)(图 S1, J 至 K,以及表 S3A)。这一结果与先前在癌症中描述的 3' UTR 缩短一致 (36),但也可能反映了由降解 mRNA 产生的 3' 截断伪影的影响。在这些异构体中,2% (2940) 起源于基因间区,其中 39% 为多外显子(图 S1M),可能代表未注释或重新表达的基因。

我们预测了长读长衍生异构体的蛋白质编码序列,并将其与来自 UniProtKB / Swiss-Prot 的人类参考蛋白进行了比较 (37)。大多数匹配参考序列的异构体

A

B

C

D

E

F

G

H | J

图 1. 长读长 RNA-seq 在 LUAD 原发性肿瘤中检测到未注释的替代剪接异构体,这些异构体在与 IFN 反应相关的基因中富集。(A) 在人类原发性 LUAD 肿瘤($n = 12$ 名患者)中发现全长剪接 mRNA 异构体的流程。对每个肿瘤的 RNA 进行长读长 (LR) RNA-seq 测序以识别未注释的异构体,这些异构体经过了广泛的质量控制和过滤,包括使用来自同一样本的短读长 (SR) RNA-seq 数据来验证未注释的剪接接头、已知 polyA 位点和已知转录起始位点。保留在 $\geq 1$ 个样本中 reads $\geq 5$ 或在 $\geq 2$ 个样本中 reads $\geq 3$ 的异构体。过滤详情见“材料与方法”。全长异构体使用 SQANTI3 异构体结构类别进行注释:FSM、RM、ISM、NIC 和 NNC。按异构体预测并注释 ORF。(B) 在 LUAD 中检测到的长读长衍生全长 mRNA 异构体使用 SQANTI3 异构体结构类别进行分类。(C) 由 FLAIR 定量的每个异构体阳性患者样本数量,按 SQANTI3 异构体结构类别显示。(D) 通过将计算机模拟翻译的 mRNA 序列与来自 UniProt 的参考蛋白序列进行比较,预测了长读长衍生全长 mRNA 异构体对蛋白质编码潜力的影响,并针对“已知”和“未注释”异构体进行了显示。更多详情见“材料与方法”。(E) 使用来自 MSigDB 的免疫相关 Hallmark 基因集,对未注释异构体多于已知异构体的基因进行通路富集分析。基因名称和异构体数量见表 S4A(显著性使用单侧超几何检验评估;$^{*}P < 0.05$,ns 表示不显著)。(F) 针对影响与 IFN-$\alpha$ 和 IFN-$\gamma$ 反应通路相关基因的长读长衍生未注释异构体 (n = 1079) 与所有长读长衍生未注释异构体 (n = 52,010) 预测了长读长衍生 mRNA 异构体对蛋白质编码潜力的影响(显著性使用超几何检验评估;$*P < 0.05$,$P < 0.01$,$*P < 0.001$,ns 表示不显著)。(G) 使用来自 TCGA-LUAD 肿瘤 (n = 437 名患者) 和正常肺 (n = 46 名患者) 样本的短读长 RNA-seq 数据将内含子保留事件定量为 PSI。内含子保留事件经过过滤,仅保留由长读长 RNA-seq 支持且在标准参考异构体中被跳过的事件,并按 FDR 以及肿瘤与正常肺样本之间 PSI 中位数的差异进行排序(中位数 PSI 由条形表示,FDR 校正值来自 rMATS;$***P < 0.001$)。(H) 在 LUAD 肿瘤样本中由长读长 RNA-seq 检测到的 STAT2 全长剪接 mRNA 异构体,分为内含子保留(中间)和内含子跳过(底部)异构体。基因全结构显示在顶部,突出显示了保留的内含子 6 和 12。SQANTI3 结构类别列在每个异构体旁边。(I 和 J) 通过 RT-PCR 评估内含子 6 (I) 和 12 (J) 的保留情况,引物位于用于长读长 RNA-seq 的 LUAD 肿瘤 (n = 10 名患者)(左侧)和来自健康捐赠者的正常支气管上皮细胞 (NLE; n = 9 名患者)(中间)的侧翼外显子中,并定量为 PSI(右侧;箱线图显示中位数和四分位距,须线延伸至 1.5$\times$ 四分位距;显著性使用 Student's t 检验评估)。

具有完全匹配的蛋白质 [79% 参考匹配 (RM), 75% 全剪接匹配 (FSM)],而新型结构类别 [不完全剪接匹配 (ISM), NIC 和 NNC] 经常编码发散的蛋白质(图 S1L 和表 S3B)。因此,LUAD 中很大一部分蛋白质编码转录组仍未被表征。

为了确定未注释的长读段衍生异构体可能如何贡献于 LUAD 蛋白质组,我们将已知基因异构体的预测开放阅读框(ORF)相对于参考序列分类为:已知、未注释或截断(表 S3C)。我们进一步将预测编码截断 ORF 的异构体分为具有或不具有内含子保留事件的异构体,内含子保留通常通过改变阅读框或引入框内提前终止密码子(PTC)导致 截断 $(38)$。长读段衍生异构体中的内含子富集在异构体的末端 10% 区域,而在基因主体其他部分分布均匀(图 S1N)。值得注意的是,在 52,010 个具有 预测的未注释长读段衍生异构体中,35% 被预测编码截断蛋白,34% 编码未注释蛋白,31% 为已知 (图 1D 和表 S3C)。这些数据表明,在 LUAD 中经常检测到可能编码未表征蛋白和截断蛋白的未注释长读段衍生异构体。

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未注释的异构体在 IFN 相关基因中富集

尽管广泛存在,但大多数可变剪接异构体的功能尚未被表征 $(39)$。我们选择重点研究由长读长测序衍生的未注释异构体在免疫相关通路中的作用,这些通路对于肿瘤免疫至关重要,且是免疫调节疗法的目标 $(40-42)$。有趣的是,对富集了未注释异构体的基因进行通路分析显示,其在 IFN-$\alpha$ 和 -$\gamma$ 响应中显著富集(图 1E)。我们在 217 个 相关基因中的 169 个基因中发现了长读长衍生的未注释异构体,包括 STAT1、STAT2 和 HLA-A(表 S4B);其中 27% $(n = 288)$ 的 IFN 相关基因长读长衍生未注释异构体被预测由于内含子保留而编码截短的 ORF,这一比例高于未注释长读长衍生异构体的整体平均水平(图 1F)。利用来自相同肿瘤样本 $(n = 12)$ 的短读长 RNA-seq 数据,我们发现 $\geq 90\%$ 的长读长衍生未注释异构体可通过基于短读长的全长异构体表达定量被检测到,这为所有编码类别的这些 相关未注释异构体提供了正交的跨平台验证(图 S2A)。由于内含子保留可以通过引入 PTC 或抑制 mRNA 出核来降低蛋白质表达,这些结果表明,含有保留内含子的未注释异构体可能会干扰 LUAD 中的 IFN 信号传导。

为了在更大规模的患者队列中进一步探索 相关基因中肿瘤上调的保留内含子,我们利用来自癌症基因组图谱肺腺癌(TCGA-LUAD)数据库的肿瘤样本 $(n = 437)$ 和正常肺样本 $(n = 46)$ 的短读长 RNA-seq 数据对剪接进行了定量(图 S2B)。我们在 1656 个基因中发现了 3038 个差异剪接事件,其剪接进入百分比(PSI)值在肿瘤样本和正常样本之间存在显著差异 $\left / \left / \Delta\mathrm{PSI}\right / > 5\%$,错误发现率 (FDR) < 0.05],其中包括 32 个 相关基因中的 69 个事件(图 S2, C 和 D,以及表 S4C)。差异剪接事件在所有基因和 IFN 相关基因中显示出相当的内含子保留整体比例(图 S2, C 和 D),这表明内含子保留在 LUAD 中并非 基因所特有。通过筛选内含子保留,在 7 个 相关基因中识别出 10 个经长读长验证的事件(表 S4D)。这些内含子保留事件包括:(i) 在 STAT2(关键的 -I 和 -III 转录因子)中发现的两个事件 $(43, 44)$;(ii) 在 UBA7(一种通过用多肽 ISG15 共价修饰其他蛋白质以促进 响应和肿瘤免疫的酶)中发现的三个事件 $(45)$;以及 (iii) 在 DHX58、OAS1 和 MOV10 中发现的事件,这些基因均编码在肿瘤免疫中具有复杂作用的抗病毒效应因子 $(46–48)$(图 1G 和表 S4, C 和 D)。为了进一步验证这些事件并非由于组样本量差异而被检测到,我们确认除 OAS1 的保留内含子 5 之外,所有事件在对 LUAD 样本进行重复子采样时均具有鲁棒性(表 S4E)。

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带有保留内含子的 STAT2 异构体在肿瘤细胞中表达

我们专注于揭示 STAT2 中内含子保留的功能和调控,因为保留内含子 6 (ri6) 和 12 (ri12) 是 TCGA 中上调最显著的干扰素(IFN)相关事件,且 STAT2 是 IFN-I 和 IFN-III 信号传导中不可或缺且不可替代的介质 (27, 43)。长读长 RNA-seq 鉴定了 22 个 STAT2 异构体,其中 15 个未被注释,包括 12 个保留了 ri6、ri12 或两者兼有 (图 1H)。LUAD 肿瘤中所有由长读长测序衍生的 ri6 和 / 或 ri12 异构体在结构上均与参考转录组注释不同 (图 S2E 和表 S4F)。

作为一种正交验证,我们通过逆转录聚合酶链反应 (RT-PCR) 对 STAT2 内含子 6 和内含子 12 的保留情况进行了定量分析,所用引物可同时扩增包含内含子的转录本和完全剪接的转录本,样本为经长读长 RNA-seq 分析的原发性 LUAD 肿瘤。作为正常对照,我们使用了来自健康捐赠者、在气液界面培养的原发性支气管上皮细胞,该系统可模拟支气管肺泡上皮,包括被认为产生 LUAD 的肺泡细胞 (49–51) (图 1, I 和 J)。与 TCGA 数据一致,与正常支气管上皮细胞相比,肿瘤中这两个内含子的保留水平显著更高(中位数 PSI$_{ri6}$:肿瘤 32% 对比 正常 15%;中位数 PSI$_{ri12}$:肿瘤 25% 对比 正常 15%)(图 1, I 和 J)。LUAD 肿瘤切片的 RNA 荧光原位杂交 (FISH) 证实了 KRT8$^{+}$ 肿瘤细胞中存在 STAT2 ri6 和 STAT2 ri12 信号 (图 S2, F 和 G),表明肿瘤细胞本身表达保留内含子的 STAT2 异构体。一致地,在 6 个 LUAD 癌细胞系中通过 RT-PCR 均可检测到这两个内含子 (图 S2, H 和 I),尽管其水平(中位数 PSI$_{ri6}$ = 15%;中位数 PSI$_{ri12}$ = 12%)低于原发性肿瘤,这可能反映了培养细胞与原发性肿瘤之间基线内含子保留水平的差异。这些数据表明,与正常肺组织相比,STAT2 ri6 和 ri12 在肿瘤中上调,并在肿瘤细胞内表达,同时并不排除它们在其他细胞类型中的表达。

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STAT2 内含子保留调节 STAT2 蛋白表达和 IFN 信号传导

为了评估 STAT2 内含子保留如何影响 IFN 信号传导,我们设计了针对 STAT2 ri6(ri6-ASO1)或 ri12(ri12-ASO1 和 ri12-ASO2)剪接位点的剪接切换反义寡核苷酸(ASOs),将其作为促进内含子保留的分子工具(图 2, A 和 B)。在 A549 肺癌细胞中,这些 ASOs 增加了 ri6、ri12 或两者的保留,且在基线水平和 IFN-I 刺激后效果基本一致(图 2, C 至 H)。针对 ri6 的 ASO 增加了内含子 12 的保留,而对内含子 6 的保留没有显著影响,导致 STAT2 蛋白表达量下降了 >10 倍(图 2, C, E 和 G)。两种针对 ri12 的

B

F

H

J

图 2. 针对 STAT2 保留内含子的 IFN 允许对 STAT2 蛋白表达和 IFN 反应进行动态调节。(A 和 B) 针对内含子 6 (A) 和 12 (B) 的 STAT2 剪接位点 位置的示意图。(C 至 F) 在转染了针对内含子 6 [(C) 和 (E)] 或内含子 12 [(D) 和 (F)] 的 ,或非靶向对照 (NTC) 的 A549 细胞中,在收集前用 100 U / ml IFN-I 处理 0, 6 或 24 小时,通过半定量 RT-PCR 评估内源性 STAT2 内含子 6 [(C) 和 (D)] 或内含子 12 [(E) 和 (F)] 的保留情况,所用引物可同时扩增跳过内含子和保留内含子的异构体。图中显示了代表性图像及 PSI 定量结果($n = 3$ 个独立生物学重复;数据为平均值 ± 标准差 SD;使用 Student's t 检验评估显著性;\*P < 0.05, \*\*P < 0.01, \*\*\*P < 0.001, ns 表示不显著;所有检验均相对于同一 IFN-I 时间点的 NTC-ASO)。(G 和 H) 在转染了针对内含子 6 (G) 或内含子 12 (H) 的 ,或非靶向对照 (NTC) 的 A549 细胞中,在收集前用 100 U / ml IFN-I 处理 0, 6 或 24 小时,使用抗 STAT2 抗体进行 Western blot 定量,并以 GAPDH 作为加载对照。图中显示了代表性图像以及相对于同一 IFN-I 时间点 NTC-ASO 归一化后的定量结果($n = 3$ 个独立生物学重复;数据为平均值 ± 标准差 SD;使用 Student's t 检验评估显著性;\*\*P < 0.01, \*\*\*P < 0.001)。(I 和 J) 在转染了针对内含子 6 (I) 或内含子 12 (J) 的 ,或非靶向对照 (NTC) 的 A549 细胞中,用 100 U / ml IFN-I 处理 6 或 24 小时,通过定量实时 PCR 对 ISGs 的表达进行定量。表达量相对于同一 IFN-I 时间点的 NTC-ASO 进行了归一化($n = 3$ 个独立生物学重复)。FC,倍数变化。

在所有条件下均增加了内含子 6 的保留,并在 IFN-I 作用下增加了内含子 12 的保留,使全长 STAT2 减少高达 \~100 倍(图 2, D, F 和 H)。使用侧翼内含子 6 和 12 的引物进行延伸 RT-PCR 证实,这些效应反映了真实的内含子保留变化而非外显子跳跃(图 S3, A 至 E),并且还发现了一种同时保留内含子 12 和 13 的异构体,该异构体在 LUAD 原发性肿瘤中通过长读长测序也被检测到(图 1H 和图 S3, D 和 E)。ASO 对内含子保留和蛋白表达的影响在另外三种 LUAD 细胞系中基本一致(图 S4, A 至 C)。通过对体外和纤维素结合研究 (52) 中已知的 RNA 结合蛋白 (RBP) 结合基序进行计算映射,揭示了 ASO 靶序列与异质核核糖核蛋白 (hnRNP) 预测结合位点之间的重叠。

丝氨酸 / 精氨酸富集 (SR) 以及 RNA 结合基序 (RBM) 蛋白家族(图 S3, F 和 G),这表明 ASO 介导的对调节性 RBP 结合的空间抑制有助于增加内含子的保留。然而,我们注意到,在 ASO 靶向的剪接位点观察到的 RBP 结合模式并未被现有的计算预测模型完全重现,这凸显了此类工具在捕捉共转录 RBP 动力学复杂性方面的已知局限性。最后,我们利用已知 IFN 刺激基因 (ISG) MX1 和 RSAD2 的表达作为 IFN-I 活性的读数,研究了 IFN 处理如何影响 -I 信号传导。所有促进内含子保留的 IFN 在 -I 刺激后均抑制了 ISG 的诱导(图 2, I 和 J)。综上所述,这些结果表明 STAT2 剪接切换 可以增加内含子的保留,从而降低全长 STAT2 的表达和 -I 活性。

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当无义介导的 mRNA 降解效率低下时,STAT2 保留内含子异构体可产生截短蛋白

尽管内含子保留经常引入触发无义介导的 mRNA 降解(NMD)的提前终止密码子(PTC),但某些含有 PTC 的 mRNA 能逃避降解并产生截短蛋白 $53, 54$。由于在肿瘤中(包括肺腺癌 LUAD $55–57$)NMD 的效率通常低于正常组织,我们推论, NMD 效率降低的肿瘤可能会表达更高水平的截短 STAT2-ri6 或 STAT2-ri12 蛋白。

为了验证这一点,我们首先通过量化 12 个经过充分验证且经实验证实的 NMD 敏感外显子的包含情况 (58–60),对 437 个 TCGA-LUAD 样本的 NMD 效率进行了评分,其中较低的分数表示较低的 NMD 效率(图 S5A)。该方法通过与已发表的、由小干扰 RNA 介导的必需 因子 UPF1 沉默的 RNA-seq 数据 (61) 进行对比得到了验证,其中 缺陷细胞的 NMD 评分显著降低(图 S5B)。 NMD 评分较低的肿瘤显示出更高的 STAT2 ri6 和 ri12 保留率(图 S5, C 和 D,以及表 S5F),这表明肿瘤间 效率的差异导致了 STAT2 内含子保留的不同。值得注意的是,肿瘤的 NMD 评分低于 A549 细胞,这表明细胞系中的 NMD 效率高于体内 LUAD 肿瘤。这种差异不能归因于肿瘤纯度,因为在 TCGA-LUAD 中, NMD 评分与纯度不相关 (62)(图 S5, E 和 F)。

为了直接测试截短的 STAT2 蛋白是否内源性表达,我们利用 CRISPR 技术在 A549 和 H1975 细胞的内源性 STAT2 位点 5' 区域插入了 3xFLAG 标签(图 3A),并通过使用 FLAG 和 C 端 STAT2 抗体检测到全长 FLAG-STAT2 从而予以确认(图 S5G)。在两种细胞系中,均检测到了内源性截短 FLAG-STAT2 蛋白,其分子量与 cDNA 表达的 STAT2-ri6(\~30 kDa)和 STAT2-ri12(\~50 kDa)对照组相匹配(图 3, B 和 C)。使用 SMGIi(一种选择性抑制 必需激酶 SMG1 的抑制剂 (63))处理后,STAT2-ri12 蛋白增加了约 2 到 3 倍,同时 ri12 和 ri6 包含的转录本水平也随之升高(图 3, B 和 C,以及图 S5, H 和 I),这证实了 NMD 积极地限制了截短 STAT2 蛋白的积累。

最后,我们检查了在 NMD 抑制条件下,使用 STAT2 剪接切换 ASO 强制内含子保留时截短蛋白异构体的表达情况。我们使用增强内含子保留的 ri6-ASO1 或 ri12-ASO1 结合

图 3. 保留内含子 6 和内含子 12 的 STAT2 异构体可产生受 NMD 调节的截短蛋白。(A) CRISPR 介导的内源性 STAT2 FLAG 表位标记策略。将靶向 STAT2 起始密码子的 sgRNA、Cas9 核糖核蛋白和编码 FLAG 标签的供体寡核苷酸通过核转染导入细胞。对单细胞克隆进行扩增和基因分型,并通过蛋白质印迹法(Western blot)对 -STAT2 蛋白进行表征。(B 和 C) 使用抗 抗体通过蛋白质印迹法检测经 SMG1i(500 ng / ml,处理 24 小时)或 DMSO(作为阴性对照)处理的内源性 -STAT2 A549 (B) 或 H1975 (C) 细胞中的 NMD 标记 STAT2 蛋白异构体。瞬时转染带有 ri6 或 ri12 的 -STAT2-cDNA 用作分子量对照。图中显示了代表性图像以及对

STAT2-ri6 和 STAT2-ri12 的定量分析,以 GAPDH 作为内参,每个克隆均相对于 DMSO 进行归一化(n = 3 次独立生物学重复;数据为平均值 ± 标准差;使用 Student's t 检验评估显著性;\*P < 0.05,ns 表示不显著)。(D 和 E) 使用抗 抗体通过蛋白质印迹法检测内源性标记的 -STAT2 A549 (D) 和 H1975 (E) 克隆中的 NMD 标记 STAT2 蛋白异构体,这些克隆被转染了靶向 STAT2 内含子 6 或内含子 12 的 ASO(ri6-ASO1 和 ri12-ASO1)或非靶向对照(NTC),并经 SMG1i(500 ng / ml,处理 24 小时)或 DMSO(作为阴性对照)处理。图中显示了代表性图像以及对 STAT2-ri6 和 STAT2-ri12 的定量分析,以 GAPDH 作为内参,每个 ASO 均相对于 DMSO 进行归一化(n = 3 次独立生物学重复;数据为平均值 ± 标准差;使用 Student's t 检验评估显著性;\*P < 0.05, \*\*P < 0.01, 且 ns 表示不

显著;所有测试均相对于同一 ASO 转染的 DMSO 组)。

NMD 抑制。ri6-ASO1 结合 SMG1i 使 -STAT2-ri6 蛋白水平增加了约 3 到 5 倍,这与其在 RNA 水平上 ri6 保留率的增加一致(PSI $_{ri6}$ 为 50% 至 80%,而对照组约为 20%)(图 3, D 和 E,以及图 S5, J 和 K)。ri12-ASO1 结合 SMG1i 使 -STAT2-ri12 蛋白水平增加了约 5 到 6 倍,-STAT2-ri6 增加了约 3 倍(图 3, D 和 E)。ri12-ASO1 处理和 NMD 抑制后 ri6 保留率在细胞系之间的差异,可能反映了多种 敏感的 STAT2 异构体之间的竞争,其中编码 STAT2-ri12 的异构体在这些条件下优先增加。值得注意的是,虽然在各种条件下全长 STAT2 (STAT2-FL) 仍然是最丰富的异构体,但 ri12-ASO1 和 SMG1i 的联合作用使 A549 细胞中的 STAT2-ri6 和 STAT2-ri12 的丰度与 STAT2-FL 几乎相当(图 S5L),这表明高内含子保留伴随低效的 NMD 可以显著改变 STAT2 蛋白异构体的平衡。综上所述,这些结果表明截短的 STAT2-ri6 和 STAT2-ri12 蛋白产生于内源性位点,受到 的积极抑制,并在 NMD 被抑制或内含子保留率升高时积累。

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STAT2-ri12 抑制 IFN-I 响应

在确定 STAT2 内含子保留会产生截短的 STAT2 蛋白后,我们研究了其功能后果。AlphaFold 3 结构预测显示,STAT2-ri6 的卷曲螺旋结构域 (CCD) 被一个 PTC 破坏,该 PTC 将原有的 C 端 CCD 序列替换为由内含子 6 编码的 20 个氨基酸,预测其向外延伸为一段裸 $\alpha$ 螺旋,这可能会损害蛋白质与蛋白质之间的相互作用(图 4A 和图 S6A)。相比之下,STAT2-ri12 在甘氨酸-372 处发生干净的截短,没有独特的氨基酸,使其 N 端结构域 (NTD) 和 CCD 在结构上保持完整,并可能保留了经典的相互作用表面(图 4A 和图 S6A)。两种截短的异构体都缺乏 Src 同源 2 (SH2) 和转录激活 (TAD) 结构域,而这两个结构域是响应 IFN 以实现 STAT2 靶基因转录上调所必需的(图 4A)。为了确认这两种异构体都不能传递 响应,我们在两个独立的 $\mathrm{STAT2}^{\mathrm{KO}}$ A549 克隆中重新表达了带有 FLAG 标签的 STAT2-FL、STAT2-ri6、STAT2-ri12 或空载体 (EV),在这些克隆中,内源性 STAT2 已通过 CRISPR 灭活(图 S6, B 至 F)。只有 STAT2-FL 能够恢复 -I 刺激的 MX1 和 RSAD2 表达,证实了两种截短异构体都不能传递 -I 响应(图 S6G)。

接下来,我们探讨在同样表达全长 STAT2 的细胞中,截短异构体是否会影响 -I 信号传导。为此,我们使用了多西环素 (DOX) 诱导的 A549 细胞系,这些细胞系表达带有 FLAG 标签的 STAT2-ri6、STAT2-ri12 或 STAT2-FL cDNA,且在各自的终止密码子后被截短(图 4, B 和 C)。在 -I 刺激下,STAT2-ri12 的表达在所有测试的 -I 剂量下均降低了 ISG 的表达,而 STAT2-ri6 没有产生影响,STAT2-FL 则如预期地增加了 ISG 的表达(图 4D)。为了明确其机制,我们进行了共免疫沉淀实验,评估其与 IRF9 和 STAT1 的相互作用,这两者与 STAT2 一起组成了介导 -I 响应的 ISGF3 转录因子 (64)。STAT2-ri12 保留了与 IRF9 的结合能力,但未能与 STAT1 结合,这与丢失了 STAT1:STAT2 相互作用所需的 SH2 结构域一致 (64)。STAT2-ri6 与这两个伙伴蛋白均不相互作用,这与其被破坏的 CCD 一致,而 CCD 是 IRF9 结合所必需的 (65)。STAT2-FL 如预期地与两个伙伴蛋白均相互作用(图 4, A 和 E)。无论是否受到 -I 刺激,两种截短异构体主要定位于细胞质中(图 S7A),这表明这些相互作用发生在细胞质内。由于 IRF9 结合和核转位是实现有效的 STAT2 信号传导所必需的 (66),STAT2-ri12 可能通过隔离 IRF9 并阻止 ISGF3 的组装,从而充当显性负性抑制剂。

C

B

D

E

图 4. STAT2 保留内含子 6 和内含子 12 的异构体编码的蛋白无法响应 -I,且其抑制能力有所不同。(A) 由 AlphaFold 3 预测的 STAT2-FL、STAT2-ri6 和 STAT2-ri12 蛋白异构体的蛋白质结构。氨基酸残基按蛋白质结构域着色。DBD,DNA 结合结构域。(B) 构建 DOX 诱导的表达截短 STAT2 蛋白异构体的 A549 细胞系的策略。表达野生型 STAT2 的亲本 A549 细胞被感染编码 STAT2-FL、STAT2-ri6.TR 或 STAT2-ri12.TR 的慢病毒构建体。DOX 结合激活反四环素控制转录激活因子 (rtTA),进而激活驱动 STAT2 异构体表达的四环素响应元件 (TRE) 合成启动子。iSTAT2-ri6.TR 和 iSTAT2-ri12.TR 是

在各自的PTC之后截断。(C) 使用抗FLAG抗体通过蛋白质印迹法(Western blot)评估了携带DOX诱导的STAT2-FL、STAT2-ri6.TR或STAT2-ri12.TR且经DOX或DMSO处理48小时的A549细胞中FLAG-STAT2蛋白异构体的表达情况,并以GAPDH作为加载对照。图中显示了代表性图像,并标明了STAT2-FL、STAT2-ri6和STAT2-ri12的预期位置。,全长。(D) 通过定量实时PCR评估了经DOX或DMSO处理48小时、表达DOX诱导的空载体、STAT2-、STAT2-ri6.TR或STAT2-ri12.TR的A549细胞在IFN-I刺激6小时后ISGs的表达情况,结果以相对于相应DMSO对照组的倍数变化表示(n = 3个独立生物学重复;数据为平均值 ± 标准差;使用Student's t检验评估显著性;\*P < 0.05, \*\*P < 0.01, \*\*\*P < 0.001,ns表示不显著)。(E)

在携带DOX诱导的FLAG标签STAT2-、STAT2-ri12或STAT2-ri6的A549细胞中评估STAT2与STAT1或IRF9之间的相互作用。细胞经DOX处理48小时以诱导表达,随后在裂解前使用1000 U / ml IFN-I刺激1.5小时。使用抗FLAG抗体对FLAG标签蛋白进行免疫共沉淀(IP),用FLAG肽洗脱,并使用所示抗体通过蛋白质印迹法进行分析。

这些数据揭示了两种异构体之间在功能上的重要不对称性。STAT2-ri12能主动抑制IFN-I信号传导,而STAT2-ri6在功能上是惰性的,既不传递也不抑制反应。这种不对称性具有重要意义:由于ri6位于ri12的上游,保留这两个内含子的异构体将编码STAT2-ri6蛋白而非STAT2-ri12,因为ri6 PTC在到达ri12编码序列之前就终止了翻译。

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STAT2 保留内含子与 PD-L1 抑制反应相关

IFN 信号在癌症免疫治疗中扮演着复杂角色:尽管它对于白细胞的激活、分化和肿瘤排斥至关重要 (27, 67),但慢性的 IFN 信号可能会驱动免疫抑制并导致治疗失败 (23, 25, 26)。为了评估 STAT2 内含子保留如何与这种双重功能相互作用,我们检查了来自 OAK 临床试验的非鳞状非小细胞肺癌患者的 STAT2 内含子保留情况,该试验将 PD-L1 抑制剂 atezolizumab 与多西他赛 (docetaxel) 化疗进行了比较 (2, 68)。我们将 OAK 的短读长 RNA-seq 数据映射到我们富含长读长的 LUAD 转录组中,并使用 rMATS 对剪接事件进行了量化(图 5A 和表 S5A)。我们对具有完整元数据的 atezolizumab 治疗患者进行了多变量 Cox 比例风险分析,以评估总生存期与 STAT2 ri6 和 ri12 保留、STAT2 总表达量、

通过免疫组化 (IHC) 检测的瘤内 PD-L1 表达以及肿瘤突变负荷 (TMB) 之间的关联。Cox 比例风险模型在控制模型中包含的其他变量的同时,估计每个测量变量对生存期的独立影响。对于连续变量,风险比 (HR) 表示每个变量增加一个增量对死亡风险的独立影响。对于离散变量,HR 表示该变量与基线相比对死亡风险的独立影响。STAT2 ri12 保留预测了 atezolizumab 治疗患者生存期的改善(死亡 :0.5, P = 0.005),而 STAT2 ri6 则预测生存期恶化(死亡 :2.02, P = 0.002),且这种影响独立于 TMB、PD-L1 IHC 和 STAT2 表达(图 S8A)。高 TMB 预测了生存期的改善(死亡 :0.47, P = 0.035),这在预料之中,因为 TMB 是一个

经美国食品药品监督管理局 (FDA) 批准的免疫治疗生物标志物。相比之下,PD-L1 染色并不能预测总生存期 (P = 0.811),这与已发表的 OAK 数据 (2) 一致(图 S8A)。在对年龄、性别、吸烟情况以及 IFN 信号的转录组标志物 IFNG.GS 和 ISG.RS (69) 进行调整后,这些关联依然存在(图 S8B)。

ri6 和 ri12 的相反效应促使我们将它们的差异作为一种复合生物标志物进行研究。我们发现 $PSI_{ri12-ri6}$ ——即 ri12 与 ri6 保留之间的差值——能强有力地预测 PD-L1 阻断后生存期的改善(死亡 :0.48, P = 0.0008)(图 S8C),而这种效应在多西他赛治疗的患者中并不存在,表明这是一种免疫特异性的关联。我们在生物标志物阴性患者中优化了一个截断值,将患者分为两组($PSI_{ri12-ri6} \geq 5\%$;见材料与方法),发现 High-$PSI_{ri12-ri6}$ 患者的生存期较 Low-$PSI_{ri12-ri6}$ 患者显著改善,且其效应强于 High-TMB(图 5, B 和 C)。值得注意的是,只有 -$PSI_{ri12-ri6}$ 患者从 atezolizumab 治疗中获得了相对于多西他赛的生存获益(死亡 :0.49, P = 0.001),而在 Low-$PSI_{ri12-ri6}$ 患者中未观察到此类获益(图 5D)。-$PSI_{ri12-ri6}$ 患者与 -TMB 及 PD-L1 阳性患者的重叠极少(图 5E 和图 S8E)。将 $PSI_{ri12-ri6}$ 与 TMB 结合使用,使生物标志物阳性的响应者人数从 9 人几乎翻倍至 16 人(图 5F),这使得 $PSI_{ri12-ri6}$ 成为一个可能的独立且互补的免疫治疗生物标志物,尚待前瞻性确认。

在 OAK 研究中,High-PSI$_{ri12-ri6}$ 患者与 Low-PSI$_{ri12-ri6}$ 患者之间共有 304 个基因存在差异表达(表 S5B)。基因集富集分析显示,High-$_{ri12-ri6}$ 肿瘤中的 IFN-$\alpha$ 和 IFN-$\gamma$ 信号传导有所减少(图 5G,图 S8 G 和 I,以及表 S5C),这表明 High-$_{ri12-ri6}$ 肿瘤可能具有较低的慢性干扰素信号传导,从而促进了对 PD-L1 抑制剂的反应。这一结果在 TCGA 中得到了重现(图 S8 H, J 和 K 以及表 S5 D 和 E),表明 $_{ri12-ri6}$ 与 IFN 信号传导之间的负相关性在不同队列中具有可重复性。与 STAT2-ri12 蛋白在抑制 IFN-I 中可能发挥的作用一致,在 OAK 和 TCGA 中,High-$_{ri12-ri6}$ 患者的 NMD 评分均低于 Low-$_{ri12-ri6}$ 患者(图 5H,图 S8F,以及表 S5 F 和 G),这表明其肿瘤可能更高效地产生 STAT2-ri12 蛋白。值得注意的是,NMD 评分并不能独立预测生存期(图 S8D),这表明 $PSI_{ri12-ri6}$ 捕捉到了 NMD 效率之外的生物学特性。

A

B

C

D

E

F

G

H

图 5. STAT2 保留内含子与 3 期临床试验中对阿替利珠单抗(atezolizumab)的反应相关。(A) 使用来自 OAK 开放标签 3 期临床试验的治疗前非鳞状非小细胞肺癌肿瘤( $n = 503$ )的 RNA-seq 数据,通过 rMATS 对可变剪接事件进行定量,重点关注 STAT2 保留内含子事件及其与接受 PD-L1 抑制剂阿替利珠单抗或化疗药物多西他赛(docetaxel)治疗后总生存期的关系。CA,盒状外显子;IR,内含子保留;A5SS,可变 $5'$ 剪接位点;A3SS,可变 $3'$ 剪接位点;MXE,互斥外显子。(B 和 C) OAK 中阿替利珠单抗治疗组的总生存期 Kaplan-Meier 曲线图:High-$_{ri12-ri6}$( $\geq 5\%$ ; $n = 43$ )对比 Low-$_{ri12-ri6}$( $< 5\%$ ; $n = 212$ )(B),或 High-TMB( $\geq 16$ mutations / Mb; $n = 37$ )对比 Low-TMB( $< 16$ mutations / Mb; $n = 113$ )(C)。显著性采用 log-rank 检验评估。$_{ri12-ri6}$ 的最佳二分切点是使用 R 语言包 survminer 中的 surv\_cutpoint 函数得出的(见材料与方法)。(D) OAK 中阿替利珠单抗治疗组的非鳞状非小细胞肺癌患者中,High-$_{ri12-ri6}$( $n = 43$ )或 Low-$_{ri12-ri6}$( $n = 212$ )与多西他赛治疗组( $n = 248$ )总生存期的 Cox 比例风险分析。数据表示 HR $\pm 95\%$ 置信区间 (CI),反映了各组相对于多西他赛治疗组的相对死亡率。显著性采用 Wald 检验评估。

(E) OAK 阿替利珠单抗治疗组中 High-$_{ri12-ri6}$( $\geq 5\%$ )与 High-TMB( $\geq 16$ mutations / Mb)的重叠情况。(F) 根据

最后,为了评估跨肿瘤的适用性,我们利用 IMvigor210(一项针对转移性尿路上皮癌的阿替唑izumab单臂 2 期临床试验 (70))的治疗前短读长 RNA-seq 数据,计算了 STAT2 内含子保留情况和 $PSI_{ri12-ri6}$。$PSI_{ri12-ri6}$ 再次与阿替唑izumab 治疗后的生存率改善相关,无论将其作为单一变量还是协变量,在高 $PSI_{ri12-ri6}$ 患者中,在独立优化的截断值下均显示出显著更好的结果(图 S8, L 和 M,以及表 S5, H 和 I)。

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讨论

在此,我们使用了长读长 RNA-seq(能够解析短读长测序无法区分的全长异构体结构),以全面分析肺腺癌(LUAD)中的可变剪接异构体,揭示了超过 149,000 种 mRNA 异构体,其中包括与干扰素(IFN)反应相关的基因。针对 STAT2,我们表明保留的内含子 6 和 12 会损害全长 STAT2 的表达,能够编码显性负性截短蛋白,并可能预测患者对免疫疗法的反应。这些发现可能为 LUAD 中 RNA 剪接的治疗靶向开辟新途径。

现有的免疫治疗生物标志物并不完善 (4, 71, 72),迫切需要更多且更好的工具来指导治疗决策。我们表明,相对于 ri6,STAT2 ri12 包含率较高(High-PSI $_{ri12-ri6}$)的患者在接受阿替唑瘤(atezolizumab)治疗后生存率显著提高,这一关联在两种不同肿瘤类型的独立临床队列中均被观察到。尽管剪接特征在 LUAD 中具有预后价值 (73),但据我们所知,这是首项将特定可变剪接事件直接与免疫治疗结果联系起来的研究。PSI $_{ri12-ri6}$ 识别出的患者子集与 TMB 或 PD-L1 IHC 的重叠极小,且将其与 TMB 结合使用后,生物标志物阳性响应者的数量几乎翻了一番。这使得 $_{ri12-ri6}$ 成为一个潜在的临床可操作的转录组生物标志物,能够捕捉到现有工具所遗漏的免疫治疗获益,值得在未来的研究中进行前瞻性验证。这种关联的机制基础可能与 STAT2-ri12(而非 STAT2-ri6)能够作为 IFN-I 信号传导的显性负性抑制剂的能力有关:鉴于慢性 IFN-I 会损害免疫治疗的疗效 (25, 26, 69),表达 STAT2-ri12 的肿瘤可能更容易被启动以响应抗 PD-L1 免疫治疗。由于 ri6 位于 ri12 的上游,ri6 的保留可能会阻断 STAT2-ri12 的表达,这可能解释了 ri6 与较低生存率之间的关联。或者,High- $_{ri12-ri6}$ 肿瘤可能具有较低的 NMD 效率,导致编码 PTC 的新抗原水平较高,从而增强免疫识别。进一步研究 STAT2 内含子保留是否在体内驱动抗肿瘤免疫反应中起直接机制作用,将是未来研究的一个明确步骤。

如果 STAT2 内含子保留直接影响治疗反应,那么对其进行操纵可能代表一种创新的治疗策略。使用经 FDA 批准的 ASO 化学方法,我们证明了 STAT2 剪接

根据生物标志物阳性情况分层的试验标准。(G) 使用 MSigDB Hallmark 2020 基因集 (94, 95),在 OAK 队列的 High- $_{ri12-ri6}$ 或 Low- $_{ri12-ri6}$ 患者中显著富集的通路 (FDR < 0.05)。基因根据使用 DESeq2 对 High- $_{ri12-ri6}$ 与 Low- $_{ri12-ri6}$ 患者进行差异基因表达分析所得的 Wald 检验统计量进行排序,并使用 gseapy 对排序后的基因列表进行基因集富集分析。正的归一化富集分数 (NES) 表示该通路在 High- $_{ri12-ri6}$ 患者中富集,而负的 NES 则表示在 Low- $_{ri12-ri6}$ 患者中富集。免疫相关通路以紫色突出显示。(H) OAK 患者中 High- $_{ri12-ri6}$ ($\geq 5\%$ ; n = 70 名患者) 与 Low- $_{ri12-ri6}$ (<5%; n = 433 名患者) 的 NMD 分数(箱线图显示中位数和四分位距,须线延伸至 1.5 倍四分位距;显著性使用 Student's t 检验评估)。较低的 NMD 分数反映了较低的 NMD 效率(见材料与方法)。

可以通过药理学手段进行调节,以调控 STAT2 蛋白的表达和 IFN-I 信号传导强度。针对 STAT2 剪接的 ASO 可使临床医生根据需要精确抑制癌症中的 STAT2 活性以及 IFN-I 和 IFN-III 信号传导,从而提供比目前可能实现的更精细的炎症控制程度。因此,有必要开展进一步研究,以评估在体内将 ASO 介导的 STAT2 剪接操纵与免疫疗法结合所产生的影响。

尽管肿瘤组织与正常组织之间 STAT2 ri6 和 ri12 保留的差异看似不大,但微小的剪接变化可能会产生巨大的功能性后果:正如对其他靶点的描述那样 (74, 75),NMD 可以掩盖 NMD 敏感异构体产量的增加;且多个异构体的同步转变会产生异构体比例的非线性变化,而这些变化通常会被转录、mRNA 稳定性、翻译效率和蛋白质周转之间的复杂相互作用所放大 (76)。值得注意的是, PSI 效率降低的 LUAD 肿瘤显示出显著更高的 STAT2 内含子保留,且药理学 抑制在细胞系中使截短的 STAT2 蛋白增加了 2 到 3 倍。综合来看,这表明 活性较低的肿瘤很可能在功能相关水平上表达截短的 STAT2 蛋白。本研究的主要局限性包括:由于缺乏异构体特异性抗体,无法直接测量原发肿瘤中的 STAT2 蛋白异构体;以及通过长读长 RNA-seq 识别的异构体不一定是癌症特异性或癌症富集的,因为它们尚未与来自正常肺组织的长读长数据进行比较。

尽管 RNA 剪接已被研究了数十年,但剪接异构体的完整多样性(尤其是免疫相关基因)直到最近才开始被充分认识 $12, 13, 15, 18, 21, 77$。本研究在经过深入研究的癌症基因中揭示的大量此前未被注释的异构体目录,强调了仅靠短读长方法无法观察到多少肿瘤转录组及其功能后果。其中一些异构体(包括 STAT2 的异构体)可能会在肿瘤微环境中的多种细胞类型中表达,在未来的研究中,单细胞和空间长读长测序对于解析其细胞类型特异性至关重要。

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材料与方法

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临床样本

涉及人类肿瘤样本的研究是根据杰克逊基因组医学实验室机构审查委员会(IRB 编号 2019-RELY-002-HHC 和 2019-RELY-002)批准的方案进行的。侵袭性 LUAD 患者的术后肿瘤样本是在获得适当知情同意后在哈特福德医院(Hartford Hospital)收集的。本研究中使用的人类支气管上皮细胞及其衍生培养物是通过国家疾病研究交换中心(NDRI)从已故捐赠者处获得,以及通过(俄亥俄州)捐赠者回收计划从去标识化的已故捐赠者处获得。该研究经杰克逊实验室机构审查委员会审查(2019-NHSR-048;2022-NHSR-004),并被认定为符合非人类受试者研究条件,因为所有标本均来自已故捐赠者且在提供时没有直接标识符。所有研究活动均按照机构政策和伦理标准进行。

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人类细胞系

细胞系购自美国标准细胞库(ATCC)。A549 细胞系培养于 Ham's F-12 营养混合液(ThermoFisher Scientific 编号 11765-054)中,并添加了 10% 胎牛血清(FBS)(GeminiBio 编号 100-500)、25 mM HEPES(ThermoFisher 编号 15630-080)、2 mM L-谷氨酰胺(ThermoFisher 编号 25030-081)和 1% 青霉素 / 链霉素混合物(ThermoFisher 编号 15140-122)。NCI-H1373、NCI-H1573、-H1693、-H1755 和 -H1975 细胞系培养于 RPMI-1640 培养基(ThermoFisher 编号 11875-093)中,并添加了 10% FBS(Denville Scientific 编号 C788U23)和 1% 稀释的青霉素 / 链霉素混合物(ThermoFisher 编号 15140-122)。所有细胞系均在 37℃、5% CO₂ 条件下生长。对于常规传代,将细胞培养物与 0.05% trypsin-EDTA(ThermoFisher 编号 25300-054)在 37℃ 下共同孵育直至细胞脱离。使用 MycoAlert 支原体检测试剂盒(Lonza 编号 LT07-318)对细胞进行常规检测,结果均为支原体阴性。

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人类原代支气管上皮细胞

为了从肺上皮祖细胞生成气液界面(ALI)培养物,将原代肺上皮细胞接种在孔径为 0.4 $\mu$ m(Corning 编号 3470)且涂有 0.03 mg / ml 大鼠尾 Collagen I 蛋白(Gibco 编号 A1048301)的嵌件上。接种后,孔槽在 Pneumacult-Ex Plus 培养基(STEMCELL 编号 05040)中维持 8 到 10 天,并添加 10 $\mu$ M ROCK 抑制剂 Y-27632(Abmole 编号 Y-27632),直到细胞达到 100% 汇合,每 2 到 3 天更换一次培养基。随后,细胞在 Pneumacult-ALI 培养基(STEMCELL 编号 05001)中分化 5 到 7 天,并添加 10 $\mu$ M ROCK 抑制剂 Y-27632(Abmole 编号 Y-27632),每 2 到 3 天更换一次培养基,同时每 2 到 3 天测量一次跨上皮 / 内皮电阻(TEER),直到细胞完全分化,具体如前所述(78, 79)。最后,细胞在不含 ROCK 抑制剂的 Pneumacult-ALI 培养基(STEMCELL 编号 05001)中分化约 28 天,每 2 到 3 天在嵌件的基底侧更换一次培养基。一旦 TEER 值达到 >500 ohms / cm $^{2}$ ,则移除顶层的培养基,并每 2 到 3 天在显微镜下检查一次纤毛摆动和黏液产生。分化后,收获气液界面膜并直接在 RLT 中裂解,用于随后的 RNA 提取。

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质粒

所有质粒均通过全质粒 Nanopore 测序或标准 Sanger 测序(Quintara Biosciences)进行了序列确认。用于克隆的所有引物序列均列于表 S6H 中。

pVAX1 瞬时转染质粒:全长 STAT2 异构体序列是通过使用 Phusion Hot Start II DNA 聚合酶(ThermoFisher Scientific 编号 F-549L)从 A549 cDNA 中通过融合 PCR 获得的。所有构建体均是通过对从 A549 cDNA 或 gDNA 中获得的 STAT2 部分元件进行连续融合 PCR 获得的,最后添加了 NheI 和 EcoRI 位点。所使用的所有克隆寡核苷酸均列于表 S6H 中。所得扩增子使用 NheI-HF(New England Biolabs 编号 R3131)和 EcoRI-HF(NEB 编号 R3101)进行酶切,并使用 T4 DNA 连接酶(NEB 编号 M0202)连接到线性化的 pVAX1(Addgene 编号 196624)骨架中。空载体 pVAX1 (pVAX1-EV) 是通过使用 NheI-( 编号 R3131)和 XbaI( 编号 R0145)进行限制性酶切,并使用 T4 DNA 连接酶( 编号 M0202)将骨架自身连接而生成的。

pLJM1 慢病毒插入质粒:编码 3xFLAG 标签 STAT2 异构体的第三代慢病毒是通过使用 T7\_F 和 BGH\_R 扩增插入片段,随后使用 NheI- 和 EcoRI- 进行限制性酶切,将每个异构体从 pVAX1 亚克隆到 pLJM1-Polylinker(Addgene 编号 164143)中生成的。

pINDUCER20 诱导插入质粒:所有插入片段均使用引物 AgeI\_T7 和 PacI\_BGH 从 pVAX1 中扩增,并使用 AgeI-( 编号 R3552)和 PacI( 编号 R0547)位点亚克隆到 pCR8-ccdb-u1(A. Cheng 提供)中。插入片段通过 Gateway 克隆(Invitrogen 编号 11791020)转移到 pINDUCER20(Addgene 编号 44012)中。

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STAT2 敲除细胞系的构建

靶向 STAT2 的 gRNA 是使用 CRISPR 设计工具(https: / design.synthego.com / # / , Synthego)基于 Ensembl GRCh38.p10 人类基因组构建靶向 STAT2(表 S6D)设计的。合成了靶向相关序列且具有标准化学修饰(前三个和后三个碱基为 2'-O-甲基化核苷酸和硫代磷酸酯键)的单导向 RNA (sgRNA)(Synthego)。然后,将 16 $\mu$ g 的 sgRNA 与 20 $\mu$ g 的 Alt-R HiFi Cas9 核酸酶 V3(IDT 编号 1081060)在室温下孵育 30 分钟。收集 A549 细胞,并使用 4D-Nucleofector X Unit(Lonza)以及表 S6E 中列出的电转染溶液和程序,将 sgRNA:Cas9 核糖核蛋白混合物电转染至细胞中。细胞在补充了 5 $\mu$ M Alt-R HDR Enhancer V2(IDT 编号 10007921)的完全生长培养基中孵育。电转染 24 小时后,移除培养基并更换为不含 HDR Enhancer 的完全生长培养基。收集电转染后的细胞并进行梯度稀释至 5 cells / ml 的浓度,然后接种到 96 孔板的每个孔中。扩增单细胞克隆,并使用 QIAamp DNA Mini Kit(Qiagen 编号 51306)提取 gDNA。使用表 S6F 中列出的引物扩增编辑区域,并通过 Sanger 测序确认 PCR 产物。使用 DECODR(https: / decodr.org / )将单细胞克隆的色谱图文件解卷积为组成等位基因,并以亲本 A549 细胞作为对照。通过 Western blot 和 IFN 刺激,随后对已知的 STAT2 依赖性 ISGs MX1 和 RSAD2 (80) 进行 RT-qPCR,确认 STAT2 敲除(缺失)。

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CRISPR介导的内源性STAT2 FLAG表位标记

通过CRISPR-Cas9介导的同源定向修复(HDR),将编码3xFLAG表位标签的序列插入到A549和H1975细胞中STAT2起始密码子的紧下游。按照上述方法合成针对STAT2起始密码子区域的sgRNA(表S6D)并与Cas9形成复合物。随后,将200 pmol的单链HDR供体寡核苷酸(由STAT2同源臂侧翼包围,编码3xFLAG标签;IDT;序列列于表S6G)添加到电穿孔反应中。使用4D-Nucleofector X Unit,配合表S6E中列出的电穿孔溶液和程序,将sgRNA:Cas9核糖核蛋白和供体寡核苷酸电穿孔至细胞中。电穿孔后立即将细胞重悬于补充了5 $\mu$ M(A549)或3 $\mu$ M(H1975)Alt-R HDR Enhancer V2(IDT编号 10007921)的完全生长培养基中。24小时后,将培养基更换为不含HDR Enhancer的完全生长培养基。3天后,收获细胞并将其梯度稀释至5 cells / ml,接种于96孔板中进行单细胞克隆。使用表S6F中列出的引物扩增编辑区域,并通过Sanger测序确认PCR产物。使用抗FLAG抗体通过Western blot确认FLAG标签的成功框内插入。

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构建表达STAT2异构体的稳定细胞系

根据制造商说明,使用Lipofectamine 3000(Invitrogen编号 L3000015)将10微克慢病毒质粒与5 $\mu$ g psPAX2(Addgene编号 12260)和2.5 $\mu$ g pMD2.G(Addgene编号 12259)共同转染至HEK293T细胞中。在48和72小时收集慢病毒上清液,并按前述方法(81)进行浓缩。浓缩后的慢病毒随后重悬于Opti-MEM(Invitrogen编号 31985)中,并储存于$-80^{\circ}$ C直至进一步使用。

细胞以$4 \times 10^{4}$ cells / cm $^{2}$的密度接种,2小时后通过在培养基中补充polybrene(Sigma编号 TR-1003-G)至最终浓度为8 $\mu$ g / ml,并逐滴加入所需体积的浓缩慢病毒进行转导。对于使用pLJM1衍生病毒构建的细胞系,使用1 $\mu$ g / ml puromycin(Gibco编号 A1113803)进行筛选;对于使用pINDUCER20衍生病毒构建的细胞系,使用4 mg / ml G418(Gibco编号 10131035)进行筛选。

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IFN刺激

使用完全生长培养基作为稀释剂,以指定的剂量和时长用通用I型人干扰素(PBL Assay Science编号 11200)刺激细胞。

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ASO转染

根据制造商说明,使用Lipofectamine RNAiMAX(Invitrogen编号 13778150),在24孔板中将2'-O-甲氧基乙基-硫代磷酸ASO(IDT)以100 nM的最终浓度反向转染至LUAD细胞系中。目标ASO序列列于表S6C。转染72小时后,通过在孔板中直接裂解收集用于RNA或Western blot的细胞裂解液。

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NMD抑制

为了抑制NMD,在收集RNA或Western blot样本前24小时,用补充了500 ng / ml SMG1i(Sigma-Aldrich编号 SML3864)的完全生长培养基处理细胞,或使用二甲基亚砜(DMSO)作为阴性对照。对于ASO转染与NMD抑制的联合处理,细胞按上述方法转染ASO 72小时,并在样本收集前的最后24小时使用SMG1i处理。

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肿瘤和细胞系的 RNA 提取

使用 RNeasy Mini Kit(Qiagen 编号 74106)从样本中提取高质量 RNA。对于原发性肿瘤样本,使用恒温切片机(Cryostat)从每个 OCT 包埋的肿瘤中切取三片 30-$\mu$ m 的组织切片,并直接放入含有 1% $\beta$-巯基乙醇的 350 $\mu$ l RLT 裂解缓冲液中。对于细胞系,通过直接向孔中加入 350 $\mu$ l 含有 1% $\beta$-巯基乙醇的 RLT 裂解缓冲液使细胞裂解。按照制造商说明,样本在室温下用 DNase I(Qiagen 编号 79256)处理 1 小时。对于从原发性肿瘤样本中提取的 ,使用 2100 Bioanalyzer(Agilent)和 6000 Pico Kit(Agilent 编号 5067-1513)评估 质量。仅选择 完整性数值(RIN)高于 7.0 的样本进行测序。

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cDNA 合成和 RT-PCR

提取如上所述,使用 SuperScript III 逆转录酶(Invitrogen 编号 18080093)将 200 至 1000 ng 的 PCR 逆转录。使用半定量 RT-PCR,通过 Q5 高保真聚合酶(Q5 High-Fidelity Polymerase)和 High-GC 缓冲液(NEB 编号 M0491S),在优化的熔解温度和循环数下扩增 20 ng 的 cDNA。引物序列列于表 S6A 中。PCR 产物在含有 SYBR Safe(Invitrogen 编号 S33102)的 2% 琼脂糖凝胶上分离,并使用 ChemiDoc MP 成像系统(Bio-Rad)成像。条带强度使用 ImageLab 6.1.0(Bio-Rad)进行定量。PSI 的计算方法为:目标事件的包含条带(included band)强度除以目标事件的包含条带与跳过条带(skipped bands)强度之和。对于每个目标事件,使用凝胶提取试剂盒(Gel Extraction Kit, Qiagen 编号 28704)提取感兴趣的条带,并进行 Sanger 测序(Quintara Biosciences)以确认其身份。仅经过验证的条带被纳入 PSI 的计算。

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定量 RT-PCR

cDNA 合成如上所述。使用 QuantStudio 7 Flex 仪器(Applied Biosystems),在 384 孔板(Applied Biosystems 编号 4309849)中,利用 iTaq Universal SYBR Green Supermix(- 编号 1725120)扩增 10 ng 的 cDNA。引物列于表 S6B 中。数据使用 QuantStudio Real-Time PCR 软件进行分析。所有基因表达均相对于管家基因 GAPDH(甘油醛-3-磷酸脱氢酶)进行归一化。

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Western blot 分析

细胞通过在预热至 95℃ 的 2x Laemmli 缓冲液(- 编号 1610737,含 5% (v / v) $\beta$-巯基乙醇)中直接在细胞培养皿内裂解进行收获。样本在 95℃ 下煮沸 20 分钟,孵育期间进行短暂的涡旋混匀。样本冷却后,要么在 -80℃ 下冷冻,要么在 4 到 15% 梯度 TGX Stain-Free 凝胶(- 编号 4568086)上电泳。凝胶被转移到 0.2-$\mu$m 硝酸纤维素膜(- 编号 1620168)上,并在含有 5% (w / v) 脱脂奶粉的 Tween 20-TBST(50 mM Tris pH 7.5, 150 mM NaCl, 0.05% (v / v) Tween 20)中封闭。印迹与一抗在 4℃ 下孵育过夜,与二抗在室温下孵育 1 小时。使用 ChemiDoc MP 成像系统(-)进行红外或化学发光检测。使用辣根过氧化物酶(HRP)偶联二抗探查的印迹在成像前用 Clarity Western ECL 底物(- 编号 1705060)孵育 1 分钟。蛋白质表达使用 ImageLab 6.1.0 软件(-)定量,首先相对于 GAPDH 作为加载对照进行归一化,然后表示为相对于实验对照的倍数变化。所有使用的抗体及其相应的稀释比例列于表 S6I 中。

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免疫荧光

细胞在黑色 96 孔成像板(Revvity 编号 6055300)中培养 48 小时,并使用磷酸盐缓冲盐水(PBS)中 4% (w / v) 的多聚甲醛孵育孔板进行固定。使用 PBS 中 0.2% (v / v) 的 Triton X-100 对细胞进行通透化,并使用 10% (v / v) 山羊血清(Sigma-Aldrich 编号 G6767,溶于 PBS 中 0.2% (v / v) 的 Triton X-100)进行封闭。孔板在 4℃ 下用稀释在封闭液中的一抗孵育过夜,并使用 Alexa-fluor-488 抗兔或 Alexa-fluor-568 抗鼠结合的二抗(Invitrogen,在封闭液中稀释比例为 1:500)进行检测。细胞在室温下使用 PBS 中的 Hoechst 33342(ThermoFisher 编号 H3570,1:2000)和 phalloidin-AlexaFluor 647 结合物(ThermoFisher 编号 A22287,1:1000)共染 15 分钟。使用 Opera Phenix 高内涵筛选仪(Revvity)对孔板进行成像。所有使用的抗体及其相应的稀释比例列于表 S6J 中。

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ViewRNA FISH

使用 ViewRNA 组织分析荧光试剂盒(ThermoFisher 编号 QVT0700)在最佳切割温度(OCT)包埋的肺肿瘤切片中对 RNA 转录本进行可视化。人 STAT2 4 型探针、人 KRT8 6 型探针以及人 STAT2\_ri6 或 \_ri12 1 型探针购自 ThermoFisher(表 S6K)。该分析按照基于组织的 分析方案进行,包括甲醛固定和 20 分钟的蛋白酶处理。使用 Leica TCS SP8 共聚焦显微镜在 $40\times$ 倍率下检测 探针。

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全细胞提取和 FLAG 免疫共沉淀

表达 3×FLAG 标签的 STAT2-FL、STAT2-ri12 或 STAT2-ri6 的多西环素诱导 A549 细胞系用 DOX (100 ng / ml) 诱导 48 小时,随后在收获前用 IFN-I (1000 U / ml) 刺激 1.5 小时。使用高盐裂解方案制备全细胞提取物(WCEs)。简而言之,用冰冷的 PBS 洗涤细胞,并在含有 50 mM Tris-HCl (pH 8.0)、450 mM NaCl、1% Triton X-100、2 MgCl₂、0.1 ZnCl₂、2 EDTA、10% 甘油、1 DTT、蛋白酶抑制剂混合物、1 Na₃VO₄ 和 50 NaF 的缓冲液中在 4℃ 下裂解 30 分钟。加入等体积的无 NaCl 缓冲液,将最终 NaCl 浓度调整为 225 。裂解液在冰上孵育 5 分钟,通过离心(14,000 rpm, 30 分钟, 4℃)澄清,收集上清液作为 WCE。

对于 FLAG 免疫共沉淀,将预先在 WCE 缓冲液(225 NaCl)中平衡的 anti-FLAG M2 琼脂糖珠(Sigma 编号 A2220)与提取物在 4℃ 下旋转孵育过夜。用 WCE 缓冲液洗涤珠子四次,并使用洗脱缓冲液(20 HEPES pH 7.5, 100 KCl, 0.1% Triton X-100, 20% 甘油, 100 $\mu$ M ZnCl $_{2}$ , 1 DTT)中的 3×FLAG 肽(200 μg / ml)依次洗脱 FLAG 标签蛋白。在进行下游分析前,在 4℃ 下连续孵育两次后收集洗脱液。

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肿瘤样本的长读长 RNA-seq

根据 Iso-seq Express 模板制备方案(Pacific Biosciences),使用 300 ng RNA 制备 Iso-seq 文库。使用 NEBNext 单细胞 / 低输入 cDNA 合成与扩增模块(NEB)结合 Iso-Seq Express Oligo 试剂盒(Pacific Biosciences)生成全长 cDNA,并进行 12 个循环的 PCR 扩增。使用 ProNex 磁珠纯化扩增后的 cDNA。所有样本产生的 cDNA 均超过 160 ng,并用于文库制备。按照制造商建议进行 SMRTbell 文库制备,包括 DNA 损伤修复、末端修复和 A 尾加成,以及与 SMRTbell 接头(Pacific Biosciences)连接。按照制造商建议,使用 PacBio SMRTLink 软件制定每个样本的加载方案。文库在 PacBio Sequel II 或 PacBio Sequel IIe 仪器(Pacific Biosciences)上进行测序。每个样本在单个 SMRT 细胞上单独测序。

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肿瘤样本和细胞系的短读长 RNA-seq

短读长 RNA-seq 文库使用 KAPA mRNA Hyperprep Kit (Roche) 根据制造商说明进行制备。首先,使用 oligo-dT 磁珠从 300 ng 总 中分离 polyA 。随后将纯化后的 RNA 在 85℃ 下片段化 6 min,目标片段长度为 250 至 300 个碱基对 (bp)。片段化后的 RNA 使用随机引物进行逆转录,孵育条件为 25℃ 10 min、42℃ 15 ,并在 70℃ 下失活 15 。随后在 16℃ 下进行 30 以及在 62℃ 下进行 10 的第二链合成和 A 尾加成。A 尾加成的双链 cDNA 片段与 Illumina 唯一接头 (Illumina) 连接。接头连接后的 DNA 使用 KAPA Pure 磁珠进行纯化。随后进行 10 个循环的 PCR 扩增。最终文库使用 KAPA Pure Beads (Roche) 进行清理。文库定量使用实时 qPCR (ThermoFisher) 完成。测序在 Illumina NovaSeq 6000 仪器上进行,生成 150 bp 的双端读长,每个样本的目标读数在 1 亿 到 2 亿 之间。

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长读长 数据处理

长读长 -seq 文件根据 Pacific Biosciences 提供的 Iso-Seq 流程(网址:https: / github.com / PacificBiosciences / pbbioconda)进行处理。简而言之,测序运行产生的 HiFi CCS BAM 文件使用 lima (v2.7.1) 并在使用 -ccs 和 -peak-guess 参数的情况下进行修剪和解复用。所得读长使用 isoseq refine (v4.0.0) 并在使用 -require-polya 参数的情况下进行质量控制,以去除 polyA 尾部和人工串联体。读长使用 isoseq cluster2 (v4.0.0) 组装成独特的异构体簇,并使用 pbmm2 (v1.13.0) 比对到 hg38 基因组。最后,比对后的异构体簇使用 isoseq collapse (v4.0.0) 合并为非冗余的全长异构体。

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长读长异构体过滤与质量控制

通过长读长 -seq 识别的异构体使用 SQANTI3 (v5.2) 流程 $(35)$(网址:https: / github.com / ConesaLab / SQANTI3)进行过滤,以去除低质量异构体和人工产物。为了使用 SQANTI3 验证未注释的剪接接头,选择进行长读长 -seq 的样本同时也进行了短读长 -seq 测序。简而言之,短读长 -seq FASTQ 文件使用 fastp (v0.20.0) 进行修剪,并使用 STAR $(82)$ (v2.7.10b) 通过多样本两轮比对(two-pass mapping)比对到 hg38 基因组,以最大限度地提高检测未注释剪接接头的灵敏度。长读长异构体使用 SQANTI3 发行版中的 sqanti3\_qc.py 脚本进行分类,参考转录组采用了参考染色体上的 GENCODE v44 全面基因注释 $(30)$、来自 refTSS 数据库 (31) (v3.1)、人类 polyA 基序列表以及从 STAR 获取的剪接接头输出文件。异构体使用 SQANTI3 发行版中 sqanti3\_filter.py 的 rules 模式进行过滤以去除人工产物;有关所用过滤参数的完整描述,请参阅 rulesFilter.json 文件 (Data S1)。我们使用来自 FLAIR 的每样本异构体计数(见下文“长读长异构体表征”部分)进一步过滤异构体;仅保留在 $\geq1$ 个样本中长读长计数 $\geq5$ 或在 $\geq2$ 个样本中长读长计数 $\geq3$ 的异构体。最终过滤后的 GTF 使用自定义 Python 脚本进行注释,并与参考 GTF GENCODE v44 中支持良好的异构体合并。

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长读段异构体的表征

单样本异构体定量(来自长读段 RNA-seq):我们使用 FLAIR (83) (v3.0.0) 对长读段 RNA-seq 样本中的异构体计数进行定量。简而言之,我们使用 UCSC 基因组浏览器 (84) (https: / hgdownload.soe.ucsc.edu / admin / exe / ) 的 gtfToGenePred 和 genePredToBed 工具,在默认选项下将长读段 GTF 转换为 BED12 格式。我们通过命令行将测序运行产生的 HiFi CCS FASTQ 文件转换为 FASTA 格式,并使用长读段 BED12 文件,在 -tpm、-stringent 和 -check\_splice 选项下运行 flair quantify。我们使用自定义 Python 脚本查询每个患者样本的原始计数文件,如果原始计数 $\geq 1$,则认为该样本中检测到了异构体。

计算 LUAD 中检测到的全剪接匹配异构体的 UTR 长度差异:对异构体进行过滤,仅保留被 SQANTI3 分类为全剪接匹配(full-splice match)或参考匹配(reference match)的异构体。将 SQANTI3 分类步骤中的 diff\_to\_TSS 和 diff\_to\_TTS 参数乘以 -1,以获得相对于最接近匹配参考序列的 5' 和 3' UTR 长度差异值;其中,正数表示该异构体相对于最接近匹配参考序列的 UTR 较长,负数则表示其 UTR 较短。

ORF 预测及其与参考序列的比较:我们在长读段转录组 FASTA 文件上运行开放阅读框(ORF)预测工具 CPAT (85) (v3.0.2),选项为 -top-=10 和 -min-=25。收集每个转录本得分最高的预测 ,并过滤以保留所有编码概率得分 $\geq 0.364$(人类 的最佳值)的 。使用 blastp (86) (v2.14.0+) 将这些推定的 ORF 与来自 UniProtKB / Swiss-Prot 数据库 (37) 的人类参考蛋白质序列进行比较。我们按如下方式计算 与 UniProt 参考序列的同一性:$(2\times\text{匹配残基}) / (\text{查询长度}+\text{参考长度})\times 100\%$。对于每个 ,我们取最佳 同一性值并使用向下取整函数进行舍入。结果按 SQANTI3 的结构类别进行分组,并按所示方式分箱。

编码潜能预测:为了识别可能存在移码或框架内提前终止密码子的异构体,我们使用自定义 Python 脚本,并以来自 UniProtKB / Swiss-Prot 数据库 (37) 的人类参考蛋白质序列作为参考。对于每个对应于参考序列中存在基因的转录本,脚本在所有三个阅读框中对其进行翻译,并将所得肽序列与注释的参考蛋白进行比较。我们首先识别出其翻译产物包含与参考蛋白匹配的 N 端和 C 端区域的异构体。如果这些末端被分割在不同的阅读框中,或者在同一阅读框内被终止密码子分隔,且其 N 端 的终止密码子位于最后一个剪接接头 (87) 上游 55 个核苷酸以外,则分别将其分类为包含移码或包含框架内 PTC。如果终止密码子位于最后一个剪接接头上游不超过 55 个核苷酸,则该异构体被分类为编码此前未表征的 C 端。翻译结果在单个连续 中与参考蛋白的 N 端和 C 端匹配的异构体则被分为 (i) 精确匹配(与参考序列相同)或 (ii) 不精确匹配(相对于参考序列包含内部不匹配或空隙)。缺乏 N 端或 C 端匹配的异构体将被相应标记。无法使用这些定义进行分类的异构体被分类为未知,且不纳入进一步分析。

含有保留内含子的异构体鉴定:为了鉴定含有保留内含子的异构体,我们使用了一个自定义 Python 脚本,从我们的长读长 GTF 中收集所有可能的保留内含子,并剔除那些在 GENCODE v44 全面基因注释 $(30)$ 的标准参考异构体中已被保留的内含子。

异构体的分类:根据编码潜能和内含子保留状态,将异构体分为以下几类:“与参考蛋白精确匹配”,指异构体包含一个与参考蛋白完全匹配的开放阅读框(ORF);“新型蛋白序列”,指最接近的匹配 ORF 在内部或 C 端包含新型氨基酸序列;“导致蛋白截短的内含子保留”,指异构体包含一个移码或含有提前终止密码子(PTC)的 ORF,且包含一个保留内含子;或“无内含子保留的蛋白截短”,指异构体包含一个移码或含有 PTC 的 ORF,且不包含保留内含子。

基于机器学习的特征重要性分析:SQANTI3 分类表中的每个异构体根据其 filter\_result 被标记为“异构体(Isoform)”或“人工制品(Artifact)”。针对每个异构体结构类别,训练了一个梯度提升分类器(XGBoost v3.2.0; 300 棵树,max\_depth = 5, learning rate = 0.05),旨在从 SQANTI3 特征集中恢复异构体 / 人工制品的判定结果,并通过分层五折交叉验证(scikit-learn v1.7.2, sklearn.model\_selection.StratifiedKFold, sklearn.metrics.roc\_curve 和 auc)估算 ROC 曲线下面积(AUC)的平均值。随后,使用 sklearn.inspection.permutation\_importance(scoring="roc\_auc"),通过对该特征在各异构体中的值进行 30 次独立随机排列,将单个特征的重要性量化为 AUC 的平均下降值。

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差异剪接与基因表达分析

我们使用了一套自定义的内部流水线进行差异剪接分析,该流水线可在 https: / github.com / TheJacksonLaboratory / splicing-pipelines-nf 获取。简而言之,该流水线使用 trimmomatic (88) (v0.39) 对 FASTQ 文件进行修剪,并使用 STAR (82) (v2.7.9a) 将其与合并了长读段和参考 GTF 的人类参考基因组进行比对。每个样本中每个剪接事件的 PSI 是使用 rMATS (89) (v4.1.2) 计算的,通过利用剪接接头读数以及外显子和内含子主体读数来推断 PSI。在适用时,计算 $\Delta$ 值,其中 $\Delta$ = (mean ) $_{case}$ – (mean ) $_{control}$ 。基因和异构体计数估计使用 StringTie (90) (v2.1.7) 完成,以 STAR 比对的 BAM 文件作为输入,并使用自定义 Python 脚本编译成计数矩阵。差异基因分析使用 DESeq2 (91) (v1.44.0) 进行,采用 Wald 检验计算 P 值,并使用 Benjamini-Hochberg 方法推导经 FDR 校正的 P 值。

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TCGA 剪接分析、基因表达和肿瘤纯度估计

来自 LUAD 患者 (TCGA-LUAD) 的基因组映射 RNA-seq 文件的相应 BAM 文件,是通过 gdc-client 可执行文件 (https: / github.com / NCI-GDC / gdc-client) 从 Genomic Data Commons (登录号 phs000178.v11.p8) 下载的,其清单是通过检查以下选项得出的:数据类型 (Data Type): Aligned Reads,实验策略 (Experimental Strategy): RNA-Seq,工作流 (Workflow): STAR 2-Pass Transcriptome,以及数据格式 (Data Format): 。 BAM 文件使用 samtools (92) (v1.4.1) 转换为原始 FASTQ 格式,以按名称对 BAM 文件进行排序 (选项 -n),并使用 bedtools (93) 的 bamtofastq 工具将排序后的 BAM 文件转换为双端 FASTQ 文件。FASTQC (https: / www.bioinformatics.babraham.ac.uk / projects / fastqc / , v0.11.9) 被用于计算所得 FASTQ 文件的质量指标。只有两个 FASTQ 文件均通过默认指标的样本才被纳入进一步分析。剪接分析和基因表达分析使用上述内部流水线进行,读长设为 50 bp,链特异性 (strandedness) 设为 “false” 以表示文库是非链特异性的。来自 TCGA-LUAD (62) 的肿瘤纯度估计值从 https: / raw.githubusercontent.com / BioinformaticsFMRP / TCGAbiolinks / master / data / Tumor.purity.rda 下载。

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来自 OAK 和 IMvigor210 的剪接分析与基因表达

来自 OAK 的非鳞状非小细胞肺癌患者、IMvigor210 的转移性尿路上皮癌患者的治疗前肿瘤样本的 FASTQ 文件以及相关的元数据,是从欧洲基因组-表型档案 (European Genome-phenome Archive) 下载的 (登录号 EGAD00001008549, EGAD00001008550, EGAD00001007703, EGAD00001006630, 和 EGAD00001006631)。剪接分析和基因表达分析使用上述内部流水线进行,读长设为 51 bp,链特异性设为 “first-strand” 以表示文库是反向链特异性的。

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NMD 评分

为了对 NMD 效率进行评分,我们使用了基于 rMATS 流水线中 SR 家族剪接因子 12 个 NMD 敏感毒性外显子 (58–60) 的数值。剪接事件值经过 Z-score 标准化,每个样本中单个事件的 Z-score 求和,然后乘以 -1 以得出 NMD 评分。所包含事件的剪接事件 ID 列在表 S5, F 和 G 中。来自 siRNA 介导的 UPF1 沉默实验的 FASTQ 文件从 Gene Expression Omnibus (登录号 GSE176197) 下载,剪接分析和基因表达分析使用上述内部流水线进行,读长设为 150 bp,链特异性设为 “first-strand” 以表示文库是反向链特异性的。

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IFN 信号评分

IFNG.GS 和 ISG.RS 评分是按照此前所述的基因列表计算的 $(69)$。简而言之,将来自 DESeq2 的、经过 VST 标准化的每个列表中的基因(不包括 STAT2)计数在每个样本内求和,并在每个组内进行 Z 分数标准化。

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基因集富集分析

为了对差异表达基因进行基因集富集分析,基因根据 DESeq2 (91) (v1.44.0) 计算的 Wald 检验统计量进行排序。使用 GSEApy (94) (v1.1.3) 的“Prerank”模块,利用 Molecular Signatures Database (MSigDB) Hallmark 2020 基因集 (95) 对排序后的基因列表进行富集分析。

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RBP 基序预测

我们使用 http: / rbpmap.technion.ac.il / 上的 RBPmap 工具 (52) 来识别与 STAT2 ri6- 和 ri12- 靶向 ASO 的靶点重叠的预测 RNA 结合蛋白基序。重叠的基序使用 UCSC 基因组浏览器进行可视化。

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AlphaFold 3 蛋白质结构预测

为了预测蛋白质结构,多肽序列通过 AlphaFold 3 (96) 在线服务器(https: / alphafoldserver.com)进行处理。生成的蛋白质结构文件使用 ChimeraX-1.9 (97) 进行可视化。

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统计分析

对于按编码序列影响分层的 novel 异构体比例,使用超几何检验评估显著性,并根据情况采用过富集或欠富集的 P 值。对于短读长 RNA-seq 的剪接分析,使用 rMATS 统计模型 $(89)$ 并采用经 FDR 校正的 P 值评估显著性。对于子采样分析,使用 numpy (v1.26.4) 的 random.choice 函数选择等数量的肿瘤样本和正常样本,使用双侧 Mann-Whitney U 检验评估显著性,并重复 100 次。所有基因、通路和细胞类型富集分析结果均过滤为 FDR 调整后的 P < 0.05。对于 RT-PCR、蛋白质印迹(Western blots)和定量 RT-PCR,数据以平均值 ± 标准差(mean ± SD)表示,除非另有说明,否则使用非配对双尾 Student's t 检验评估显著性。生存分析使用来自 OAK 和 IMvigor210 的右删失生存数据,对于使用 R 包 survivalAnalysis (v0.3.0) 的 Cox 比例风险模型,使用 Wald 检验评估显著性(不进行多重比较校正);对于使用 R 包 survival (v3.8.3) 的 Kaplan-Meier 曲线,使用对数秩检验(log-rank test)评估显著性 (98)。我们对来自 OAK 和 IMvigor210 的生物标志物阴性(TMB < 16 mutations / Mb 或 TMB 未指定)患者使用 R 包 survminer (v0.5.0) 的 surv\_cutpoint 函数,以确定 Kaplan-Meier 生存分析的最佳 PSI $_{ri12-ri6}$ 截断值。

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用于编写代码的生成式 AI

我们使用 Claude Code (Claude Sonnet 4.6; Anthropic, PBC) 辅助编写代码,并在编辑过程中将其作为编辑助手。所有人工智能 (AI) 生成的代码均在特定的子目录中产生,无法访问父级数据,也无法在这些文件夹之外写入。脚本生成的提示词包含严格指令,要求不得修改父目录中的任何数据,且所有 AI 生成或 AI 编辑的脚本在运行前均经过人工检查。

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图表与插图

数据使用 Python 或 R 处理,图表使用 R 的 ggplot2 库或 Microsoft Excel 生成。插图使用 Adobe Illustrator 2023 for Mac 制作,符合 Science / AAAS 关于图像完整性的指南。

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致谢

我们感谢 Anczuków 和 Palucka 实验室的所有成员在手稿讨论和评论方面提供的帮助,以及来自 ThermoFisher 的 A. Patel 在 ViewRNA 探针设计方面提供的协助。我们感谢杰克逊实验室(The Jackson Laboratory)显微成像、基因组编辑和基因组技术测序服务部门提供的帮助,这些服务部分由美国国家癌症研究所(NCI)拨款 P30CA034196 支持。我们在编辑过程中使用了 Claude Code (Claude Sonnet 4.6; Anthropic, PBC) 作为辅助编辑工具,以优化代码设计并精简语言。我们使用 UCSF ChimeraX 进行分子图形绘制和分析,该软件由加州大学旧金山分校(University of California, San Francisco)的生物计算、可视化和信息学资源中心开发,并得到了美国国立卫生研究院(NIH)拨款 R01-GM129325 以及国家过敏和传染病研究所网络基础设施与计算生物学办公室的支持。本研究使用了由 Genentech 生成的数据。资金支持:我们感谢美国国立卫生研究院(NIH)拨款 U19AI142733 (K.P., O.A.)、R01CA248317 (O.A.)、R01GM138541 (O.A.)、F30CA278494 (R.P.E.) 和 P30CA034196 (K.P., O.A., R.P.E.) 的资金支持,以及来自赛诺菲(Sanofi S.A.)SANOFI-SRA-FY19-JFB (J.B.) 的资金支持。作者贡献:概念化:R.P.E., O.A., J.B., K.P.;方法论:R.P.E., O.A., K.P., M.K., N.K.L., M.B., T.-C.W., S.P., I.W., F.M., M.E.P., P.C.;调查:R.P.E., M.B., A.S., P.Y., R.B., M.D., H.G.K., I.W.;可视化:R.P.E., O.A., M.B.;资金获取:O.A., K.P., J.B., R.P.E.;项目管理:R.P.E., O.A., K.P.;监督:O.A., K.P., J.B.;初稿撰写:R.P.E., O.A., M.B.;审阅与编辑:R.P.E., O.A., K.P., R.B., J.B., N.K.L., M.B., S.P.。竞争利益:R.P.E., O.A., N.K.L.,

J.B. 和 K.P. 被列入一项由杰克逊实验室提交的专利申请(D25-008-USPROV1,美国临时申请号 63 / 852,095)中,该申请涵盖了靶向 STAT2 的剪接调节 ASO 的使用以及作为免疫治疗生物标志物的 STAT2 内含子保留事件。在研究早期,J.B. 是 Neovacs 和 Ascend Biopharma 的董事会及科学顾问委员会成员,也是 Cue Biopharma 的科学顾问委员会成员。目前,J.B. 是 Immunoledge LLC 的创始人,该公司旨在为生物技术初创公司提供咨询。在此角色中,J.B. 担任 Georgiamune 的首席信息官、Metis Therapeutics 的科学顾问委员会成员以及杰克逊实验室的顾问。在本研究过程中,K.P. 是 Cue BioPharma 顾问委员会的成员和 Guardian Bio 的创始成员。OA 是 NeoSplice、Akari Scientific 和 EnteloBio 科学顾问委员会的成员。作者声明没有其他竞争利益。数据、代码和材料可用性:我们的剪接分析流水线 v2.0 此前已在 (99) 中描述,并可在 Github (https: / github.com / The.JacksonLaboratory / splicing-pipelines-nf) 上免费获取。所有其他数据均可在论文和补充材料中获得,或根据要求从通讯作者处获得。表 S1 至 S6 也可以通过 https: / github.com / ryanpe13002 / Supplementary-Tables-2 / 访问。作为本研究一部分生成的测序数据可在 dbGaP(基因型和表型数据库)中获取(登录号 phs004211.v1.p1)以及 ImmPort 中获取(研究登录号 SDY3373)。许可信息:版权所有 © 2026 作者,保留部分权利;独家许可方为美国科学促进会(AAAS)。

不对美国政府原始作品主张权利。https: / www.science.org / about / science-licenses-journal-article-reuse

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补充材料

图 S1 至 S8;表 S1 至 S6;MDAR 可重复性检查清单;数据 S1

2025年7月24日提交;2026年4月1日重新提交;2026年8月26日接受

10.1126 / science.aea7156

解耦自组装单层与钙钛矿沉积以实现高效柔性太阳能组件

Yeyong Wu, Xikun Zhang, Tiankai Zhang, Guiying Xu\*, Yunxiu Shen, Chengxin Guo, Qing Miao, Junyuan Ding, Yue Yin, Qinrong Cheng, Wen Liu, Xiaoxiao Wu, Kaiqiang Chen, Wenwen Kou, Zhiyun Cao, Haiyang Chen, Weijie Chen, Yujin Chen, Feng Gao, Yaowen Li\*, Yongfang Li

全文及作者所属机构列表:https: / doi.org / 10.1126 / science.aef9745

引言:柔性钙钛矿太阳能电池(PSCs)能够在建筑、交通、可穿戴设备和便携式设备等曲面及移动场景中实现高效的太阳能采集,从而大幅扩展了清洁能源供应的边界。尽管小面积柔性 PSCs 的能量转换效率(PCE)已达到 26.22%,接近刚性 PSCs,但器件的规模扩大会导致 PCE 和运行稳定性显著下降,使得大面积柔性钙钛矿太阳能组件(PSMs)与其刚性对应产品之间存在显著的性能差距。这种巨大的效率和稳定性缺陷仍然是单结和叠层柔性钙钛矿光伏商业化的关键障碍。

原理:大面积柔性 PSMs 的性能较差与柔性基底独特的表面性质密切相关。其 ITO 表面通常具有较低的羟基密度且分布不均,从而损害了自组装单层(SAM)的锚定以及极性钙钛矿前驱体的润湿。表面处理可以暂时增加羟基密度,而 SAM-钙钛矿前驱体共沉积可以克服润湿限制。然而,这些羟基在极性前驱体溶液中会迅速流失,导致羟基流失与 SAM 锚定之间出现动力学失配。具体而言,钙钛矿胶体与 SAM 分子的膦酸基团之间的相互作用会延迟 的吸附,导致在高效 锚定之前羟基就被耗尽,最终损害 的覆盖率和钙钛矿的结晶。因此,我们将 3,5-双(甲基磺酰基)苯铵碘 (BSAI) 作为解耦剂引入共沉积前驱体中。我们假设 BSAI 优先与钙钛矿前驱体物种相互作用,从而削弱它们与 Me-4PACz 的相互作用并加速 锚定。

结果:系统研究表明,BSAI 通过其与钙钛矿胶体强结合的铵基和双磺酰基发挥双重功能。首先,它破坏了 Pb-I 胶体与 Me-4PACz 膦酸基团之间的配位,以促进在表面羟基脱附之前快速吸附到基底上,从而在大面积基底上实现均匀的 SAM 锚定。同时,它还延迟了钙钛矿的成核以促进定向晶体生长,从而在大面积上产生优化的薄膜形貌。解耦共沉积策略中的紧凑 Me-4PACz 锚定和高钙钛矿结晶度使小面积柔性 PSCs 获得了 26.9% 的认证 PCE,而基底面积分别为 25, 100, 和 1050 cm $^{2}$(器件面积分别为 14.55, 80, 和 750 cm $^{2}$ )的柔性 PSMs 分别实现了 22.3, 20.6, 和 20.2% 的认证 PCE。在 ISOS-L-3 协议(85℃,65% 相对湿度)下经过约 1000 小时的最大功率点跟踪后,组件保留了 92% 以上的 PCE,并由 TÜV SÜD 认证通过了所有 IEC TS 63163:2021 测试序列。该策略还显示出对刚性基底和不同 分子的广泛适用性。

结论:我们确定了限制柔性 PSM 性能的关键基底表面特性因素,并开发了一种解耦共沉积策略,以解决柔性 PSM 在规模扩大过程中长期存在的性能损失瓶颈。解耦剂 BSAI 降低了钙钛矿与 SAM 之间的强相互作用,从而促进了紧凑的 SAM 锚定和高钙钛矿结晶度,这使得高效、稳定的大面积柔性光伏器件成为可能。这项工作提升了柔性钙钛矿光伏的商业可行性,并证明了其在便携式和移动电源场景中的实际潜力。□

通过解耦 SAM-钙钛矿共沉积策略,在柔性基底上实现了紧凑且均匀的 Me-4PACz 和钙钛矿薄膜。解耦剂 BSAI 优先与 Pb-I 框架结合,从而降低了 Me-4PACz 与钙钛矿之间的相互作用。这种效应促进了 Me-4PACz 快速锚定在 PET / ITO 基底的表面羟基上,并改善了钙钛矿的结晶动力学,最终产生了稳定的三齿锚定 SAM 和均匀的钙钛矿薄膜。

Me-4PACz:BSAI:钙钛矿溶液

解耦自组装单层与钙钛矿沉积以实现高效柔性太阳能组件

Yeyong Wu $^{1\dagger}$ , Xikun Zhang $^{1\dagger}$ , Tiankai Zhang $^{2\dagger}$ , Guiying Xu $^{1*}$ , Yunxiu Shen $^{1}$ , Chengxin Guo $^{3}$ , Qing Miao $^{1}$ , Junyuan Ding $^{1}$ , Yue Yin $^{1}$ , Qinrong Cheng $^{1,3}$ , Wen Liu $^{1}$ , Xiaoxiao Wu $^{1}$ , Kaiqiang Chen $^{1}$ , Wenwen Kou $^{1}$ , Zhiyun Cao $^{1}$ , Haiyang Chen $^{1}$ , Weijie Chen $^{1}$ , Yujin Chen $^{3}$ , Feng Gao $^{4}$ , Yaowen Li $^{1,5*}$ , Yongfang Li $^{1,3,6}$

由于柔性基底上的表面羟基会发生脱附,从而破坏自组装单层(SAM)的锚定和钙钛矿的结晶,因此柔性钙钛矿太阳能组件(PSMs)的光电转换效率(PCE)和稳定性低于其刚性器件。我们开发了一种解耦的 SAM-钙钛矿共沉积策略,通过减少 与钙钛矿之间的相互作用来加速 的锚定,并改善钙钛矿的结晶。在使用苯乙基铵碘作为钝化分子的 PSMs 上,器件面积为 750 cm $^{2}$ 时,认证的 PCE 为 20.2%。使用 1,3-二氨基丙烷二氢碘化物作为钝化剂时,器件面积为 14.55 cm $^{2}$ 的 SAM 为 22.0%,在 85℃ 和 65% 相对湿度的最大功率点跟踪下,1044 小时后下降了 8%。该器件通过了柔性便携式 PSMs 国际商业化评估标准的所有序列。

具有成本效益且高效的柔性钙钛矿太阳能电池(PSCs)可以将太阳能的应用扩展到曲面建筑、车辆、飞机和可穿戴电子设备(1-3)。尽管小面积柔性 PSCs 已经实现了 $26.22\%$ 的光电转换效率()(4-6),但在器件规模扩大时, SAM 和稳定性会出现明显的下降(图 S1 以及表 S1 和 S2),这导致大面积柔性钙钛矿太阳能组件(PSMs)与其刚性对应器件之间存在性能差距(7-13)。这种显著的效率和稳定性缺陷给单结和叠层柔性 PSMs 的商业可行性带来了挑战。

基底属性的显著差异是大面积 PSMs 性能较差的主要原因(14–16)。柔性塑料基底仅允许低温氧化铟锡(ITO)沉积,这会形成结晶度较低的 ITO 层,其表面具有在极性溶剂中容易脱附的羟基。与刚性玻璃基底相比,这些特性增加了均匀沉积大面积自组装单层(SAMs)和钙钛矿薄膜的难度(17–19)。即使是 -钙钛矿前驱体共沉积法(该方法规避了钙钛矿在 SAM 层上大面积润湿性差的问题,并在刚性钙钛矿组件上实现了最先进的效率),在应用于柔性基底时仍然失效(20, 21)。

共沉积法在柔性基底上失效的关键原因在于快速的表面羟基脱附与延迟的 SAM 锚定之间的动态竞争。柔性基底上的表面羟基迅速脱附,而钙钛矿与 SAM 分子中膦酸基团之间的强相互作用阻碍了 SAM 的锚定过程(22, 23),导致 沉积不均匀且钙钛矿结晶度受损(24–27)。为了解决这种动态竞争,我们通过在钙钛矿-([4-(3,6-二甲基-9H-咔唑-9-基) 丁基] 膦酸,Me-4PACz)共沉积过程中加入一种解耦剂 3,5-双(甲基磺酰) 苯铵碘 (BSAI),开发了一种解耦共沉积策略。BSAI 的铵基和两个磺酰基使其能与钙钛矿胶体强力结合,并破坏 Pb 离子与 Me-4PACz 中膦酸基团之间的配位。

这种双重功能不仅能够在大面积柔性基底上实现干扰极小且有效且均匀的 SAM 层沉积,还能延缓成核以促进钙钛矿的定向生长,从而在高达 $1050 \, cm^2$ 的面积上实现了优化的形貌。这种解耦共沉积策略在小面积( $0.0628 \, cm^2$ )柔性 PSCs 上实现了 26.9% 的记录 PCE(经认证为 26.9%)。此外,它实现了可扩展的柔性 PSMs,在 25, 100, 和 $1050 \, cm^2$ 基底上(器件面积分别为 14.55, 80, 和 $750 \, cm^2$ )分别达到了 23.1%(经认证为 22.3%)、21.0%(经认证为 20.6%)和 20.6%(经认证为 20.2%)的记录 PCE,减轻了随着模块器件尺寸增加而导致的 PCE 损失限制。此外,在 ISOS-L-3 协议 [ $85^\circ C$ ,65% 相对湿度 (RH)] 下,经过 \~1000 小时的最大功率点跟踪 (MPPT) 连续运行后,柔性 PSMs 保留了 >92% 的初始 PCE,并成功通过了由 TÜV SÜD 认证的 IEC TS 63163:2021(一项针对柔性便携式光伏模块的国际商业化评估标准)所定义的所有测试序列。我们还将这种解耦共沉积策略应用于刚性模块,在相同协议下实现了经认证 PCE 为 23.8% 且 $T_{97} >2500$ 小时老化的刚性 PSMs( $5 \, cm \times 5 \, cm$ )。解耦共沉积策略部署了高效柔性 PSMs,使其在集成到便携式充电器和无线电控制无人机 (RC-UAVs) 中时能够提供稳定的电源,验证了它们的实际适用性和商业可行性。

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柔性基底上表面羟基氧的易脱附特性

最初,我们通过采用两种不同的常用制备方法:顺序沉积法和传统的共沉积法,对比了刚性与柔性 PSM(尺寸为 $5 \, cm \times 5 \, cm$)的性能(详细的制备步骤见“实验”部分)。在玻璃 / ITO 基底上,采用共沉积法制备的 PSM 所实现的平均 PCE 略高于采用 Me-4PACz-钙钛矿顺序沉积法制备的 (22.0% 对比 21.7%),突显了其在大面积模块制备中的优越性。然而,在聚对苯二甲酸乙二醇酯 (PET) / ITO 基底上(其电学和光学特性与玻璃 / 基底相似,见图 S2),采用传统共沉积法和顺序沉积法制备的 ITO 所交付的平均 PCE(分别为 14.6 和 15.8%)均远低于采用相同沉积法制备的刚性器件(22.0 和 21.7%),这突显了此前报道的制备方法在高性能柔性 方面的内在局限性(图 1A,图 S3 和表 S3)。

改变的表面化学性质,特别是表面羟基的稳定性,成为了将常用制备方法应用于柔性基底的主要障碍。X 射线光电子能谱 (XPS) 显示,PET / 上的羟基氧与晶格氧之比 (15%) 仅为玻璃 / 上 (29%) 的一半(图 1, B 和 C,图 S4 和表 S4)(28–30)。低密度的表面羟基覆盖导致润湿性较差(图 S5)(31, 32)。特定的表面处理,例如等离子体处理,可以暂时增加 / 表面的羟基密度并提高初始阶段的润湿性(图 S5)。然而,这些由等离子体处理产生的表面羟基仍然会迅速脱附,尤其是在外部扰动下 (28, 33)。

图 1. 柔性基底上表面羟基氧的易脱附特性。(A) 使用顺序沉积和共沉积法在刚性 (glass / ) 和柔性 ( / ) 基底上制备的 ITO 的 PCE 分布。(B 和 C) 玻璃 / (B) 和 / (C) 基底在初始状态、等离子体处理后、EtOH 洗涤后以及 DMF 洗涤后的 XPS O 1s 光谱。(D) 通过顺序沉积和共沉积法处理的玻璃 / 和 / 表面的 XPS P 2p 光谱。(E) 通过顺序沉积和共沉积法在 / 上实现的羟基密度、SAM 锚定和钙钛矿薄膜质量的示意图。

在接触极性溶剂(包括乙醇 (EtOH) 和二甲基甲酰胺 (DMF) —— 分别常用于处理 SAM 层和钙钛矿层)后,玻璃 / 上的羟基与晶格氧之比仅轻微下降(EtOH 洗涤后从 58 降至 48%,DMF 洗涤后从 58 降至 49%)。相比之下, / 上相应的羟基与晶格氧之比剧烈下降(EtOH 洗涤后从 53 降至 19%,DMF 洗涤后从 53 降至 21%)(图 1, B 和 C,图 S4 和表 S4)(28, 34),这意味着表面羟基迅速脱附。我们将 / 上羟基的易脱附特性归因于该层较低的结晶度,这导致了更高浓度的氧空位和更多缺电子的 In / Sn 位点(图 S6 和补充文本第 1 节)(35)。这些缺电子的 In / Sn 位点通过路易斯酸碱相互作用,容易与路易斯碱性溶剂(如 DMF 和 EtOH)发生相互作用,从而干扰表面羟基的结合并促进羟基流失(图 S7 和补充文本第 2 节)(36–38)。

PET / ITO表面羟基易脱附的特性在顺序工艺中极大地影响了自组装单层(SAM)的沉积。PET / ITO上Me-4PACz的XPS P 2p信号强度约为glass / ITO上强度的一半(~6800对比~3300)(图1D),这表明Me-4PACz在柔性基底上的锚定效率较低。此外,随后的钙钛矿结晶受到本质上非极性的Me-4PACz末端基团的不利影响(图S8至S11),导致通过顺序沉积制备的柔性钙钛矿太阳能电池(PSMs)的光电转换效率(PCEs)分布较宽且重复性降低(图1A和图S3)。这些结果表明,顺序沉积并不适用于大面积柔性PSMs(示意图见图1E)。

共沉积方法缓解了钙钛矿前驱体在SAM覆盖表面上的大面积润湿性限制(图S12)。然而,DMF对表面羟基的易去除作用在柔性基底的共沉积方法中也严重干扰了Me-4PACz的锚定过程。在使用DMF冲洗共沉积的Me-4PACz-钙钛矿层后(图S13),PET / ITO上的P 2p信号强度再次约为glass / ITO上强度的一半(~2800对比~4500)(图1D),证实了即使采用共沉积,柔性基底上的锚定效率依然较低。鉴于Me-4PACz与溶液中的钙钛矿前驱体之间存在强相互作用(图S14至S17及补充文本 section 3),有限的Me-4PACz锚定会损害空穴提取,而前驱体中残留的Me-4PACz会干扰钙钛矿薄膜的生长,这在柔性基底上观察到的较差薄膜形貌中得到了证实(图S18至S21及补充文本 section 4;示意图见图1E)。

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解耦共沉积策略与解耦剂的选择

鉴于 PET / ITO 基底上的表面羟基容易发生脱附,仅仅增加其数量无法实现有效的自组装单分子层(SAM)锚定。理想的 SAM-钙钛矿共沉积需要加速 SAM 分子与羟基之间的锚定动力学。我们在传统的共沉积方法中引入了一种对 Pb-I 框架具有更强亲和力的解耦剂,以开发一种“解耦共沉积”策略,从而避免在 SAM 上沉积钙钛矿薄膜(尤其是大规模沉积)时出现的润湿性差的问题。解耦剂优先与 Pb-I 框架结合,从而减少 Me-4PACz 与钙钛矿的相互作用,使 Me-4PACz 能够快速锚定在 PET / ITO 上。一旦锚定,-4PACz 即可在 ITO 表面稳定。

我们设计了三种含有路易斯碱或铵基的分子,它们可以通过配位和离子键与 Pb-I 框架相互作用:3,5-双(甲基磺酰)苯胺 (BSA,含有两个 -S=O 基团)、碘化苯铵 (PAI,含有铵基) 以及碘化 3,5-双(甲基磺酰)苯铵 (BSAI,整合了上述两种功能) [图 S22;BSAI 的详细合成步骤见补充材料 (SM) 的材料与方法部分,作为解耦剂的候选物] (39)。为了评估这些添加剂的解耦功效,我们分别在引入 BSA、PAI 和 BSAI 后,系统地追踪了全前驱体溶液中 -4PACz 的相互作用。傅里叶变换红外 (FTIR) 和核磁共振 (NMR) 光谱 (图 2, A 和 B, 图 S23, 以及补充文本第 5 节) 共同表明,双功能 触发了 -4PACz 从 Pb-I 框架胶体中最大程度的释放,超过了 BSA 和 PAI,并实现了 -4PACz 与钙钛矿前驱体最有效的解耦。密度泛函理论 (DFT) 计算还显示,通过协同的 S=O…Pb 配位和 N-H…I 离子相互作用, BSAI 对前驱体 Pb-I 框架表现出强结合力 (-1.43 eV),大幅超过 -4PACz (-0.60 eV) (图 S24)。相互作用区域指标分析进一步证实了两种结合基元均具有强吸引相互作用 (图 S25)。这种协同的双重强相互作用使 在与 Pb-I 胶体的结合竞争中胜过 -4PACz,从而有效地产生了最强的解耦效果。

我们将 BSAI 作为解耦剂引入共沉积方法中,以减少 -4PACz 与钙钛矿之间的相互作用,并促进 -4PACz 释放以锚定到 ITO 上。通过原位 FTIR 光谱追踪了有无 时 -4PACz 的吸附和锚定动力学 (图 2, C 至 E, 以及图 S26 和 S27)。在初始阶段 (0 min),不含 的沉积薄膜相对于前驱体溶液 (分别为 1260.74 和 1106.46 cm $^{-1}$),其 P=O 和 P-O-(H) 峰仅显示出轻微偏移 (分别为 1260.17 和 1107.05 cm $^{-1}$),表明大多数 -4PACz 与 Pb-I 框架胶体相关联,从而抑制了其在 PET / ITO 上的初始吸附 (图 S26)。相比之下,含有 的薄膜表现出明显的峰值偏移,分别从 1266.04 和 1103.08 cm $^{-1}$ 偏移至 1259.50 和 1105.60 cm $^{-1}$,这意味着 -4PACz 与 PET / ITO 上缺电子的 In / Sn 位点发生了大量的

配位。

在随后的处理过程中,两个样本均表现出三个渐进阶段(阶段 I 至 III)。对于不含 BSAI 的样本,我们观察到在最初 9 分钟内(阶段 I),P–O–(H) 峰移极小(从 1107.05 移至 1106.66 cm $^{-1}$ ),随后在接下来的 11 分钟内移至 1104.83 cm $^{-1}$ (速率约为 $\sim0.17~^{-1}~min^{-1}$ ),这表明在此期间仅形成了有限数量的 P–O–In / Sn 键(阶段 II)。峰位置在 20 分钟后稳定在 1104.64 $^{-1}$ ,意味着锚定过程已接近完成(阶段 III)。相比之下,含有 BSAI 的样本表现出明显加速的锚定动力学。快速移位发生得更早(5 分钟后),且以更高的速率 $\sim0.64~^{-1}~min^{-1}$ 进行,表明 P–O–In / Sn 键的形成更为显著(阶段 II)。P–O–(H) 振动信号在 16 分钟后稳定在 1097.98 $^{-1}$ ,表明锚定已接近饱和(阶段 III)。这种更大的峰移速率表明,BSAI 的加入有效地破坏了 Me-4PACz 与 Pb-I 框架之间的相互作用,并促进了 Me-4PACz 在 PET / ITO 表面上的快速释放和更有效的锚定。此外,DFT 计算揭示了一种三齿锚定构型,其特征为一个 P=O $\cdots$ In / Sn 配位相互作用和两个共价 P–O–In / Sn 键,具有 -4.650 eV 的高结合能( $E_{b}$ )(图 S28)。总体而言,原位 FTIR 和 DFT 的结合结果表明,-4PACz 在 PET / ITO 上采用了三齿锚定构型。

我们通过时间分辨的外位测量进一步检查了加入 BSAI 后 -4PACz 锚定的有效性,包括 XPS(图 2, F 至 H,图 S29 和表 S5)、原子力显微镜-红外光谱(AFM-IR,图 S30)以及扫描电化学电池显微镜-薄层循环伏安法(SECCM-TLCV,图 S31)(40)。所有测量结果均显示出 -4PACz 三阶段锚定过程的证据(补充文本第 6 节)。

基于这些结果,-4PACz 在常规共沉积和解耦共沉积过程中在 PET / ITO 上的锚定过程可总结如下(图 2, I 至 P):在预阶段,常规共沉积过程(不含 BSAI)在 -4PACz 与 Pb-I 框架胶体之间表现出强相互作用,使大部分 -4PACz 保留在前驱体溶液中并抑制其在 PET / ITO 上的吸附,导致 $\mathrm{P = O\dots In / Sn}$ 配位有限。DMF 与缺电子 In / Sn 位点的便捷配位扰乱了局部电子环境,削弱了羟基-In / Sn 相互作用,并促进了相邻羟基之间的相互作用(图 2I)。相比之下,在加入 BSAI 后,-4PACz 有效地从 Pb-I 框架胶体中释放,并通过更强的配位相互作用迅速吸附到 PET / ITO 上。随后,表面羟基与吸附的 -4PACz 的膦酸部分发生相互作用,使富含羟基的界面位点在 DMF 诱导的扰动下保持稳定(图 2M)。

在第一阶段,在相对较低的温度下,吸附的 Me-4PACz 的 P-OH 基团与表面羟基之间缓慢发生脱水缩合,在两种体系中逐渐形成 In / Sn-O-P 键。在常规工艺中,竞争性的 DMF 诱导脱水缩合同时消耗了表面羟基物种并重新形成了金属-氧-金属键(图 2, J 和 N)。在第二阶段,在较高温度下,锚定反应变得更有利。然而,在常规工艺中,尽管钙钛矿结晶诱导 Me-4PACz 部分向 ITO 界面迁移,但羟基的耗尽抑制了高效锚定(图 2K)。相比之下,含有 BSAI 的体系由于有效的初始吸附而显示出加速的锚定(图 2O)。在第三阶段,随着锚定位点接近饱和且表面羟基密度降低,两种体系的锚定速率均显著减慢(图 2, L 和 P)。

图 2. 解耦共沉积策略与 -4PACz 的锚定动力学。(A) 纯 -4PACz、-4PACz:DMF:FAI:PbI$_{2}$ 溶液、-4PACz::FAI:PbI$_{2}$:BSA 溶液、-4PACz::FAI:$_{2}$:PAI 溶液以及 -4PACz::FAI:$_{2}$:BSAI 溶液的 FTIR 光谱。(B) 纯 -4PACz、-4PACz:$_{2}$、-4PACz:$_{2}$:BSA、-4PACz:$_{2}$:PAI 和 -4PACz:$_{2}$: 样品在 -d$_{7}$ 中的 ${}^{1}$H NMR 光谱。(C 至 E) 在 PET / ITO 基底上,不含 (C) 和含有 (D) 样品的原位 FTIR 光谱,以及在退火过程中相应的 P–O–(H) 振动峰位置的演变 (E)。(F 至 H) 锚定动力学的时间分辨离位 XPS 追踪。不含 (F) 和含有 (G) 处理样品的 P 2p 高分辨率光谱。P / In 信号强度比随退火时间变化的演变图 (H)。(I 至 P) -4PACz 在 PET / ITO 上,在常规 (I 至 L) 和解耦 (M 至 P) 共沉积过程中的锚定过程示意图。

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解耦共沉积对 SAM 形貌和钙钛矿结晶的调制

在解耦共沉积过程中,Me-4PACz 加速的锚定动力学使得 PET / ITO 表面能够形成均匀的 SAM 形貌。飞行时间二次离子质谱 (ToF-SIMS) 分析显示,与传统共沉积(对照组)薄膜相比,在引入 BSAI 的解耦共沉积(目标组)薄膜中,代表 $\mathrm{PO}_2^-$ 信号的 Me-4PACz 在基底区域的分布更加紧凑且在垂直方向上更集中(图 3, A 和 B)。此外,我们将钙钛矿层从基底上剥离,以直接监测使用不同共沉积方法的 -4PACz 信号。在对照组样本中,从钙钛矿的埋底界面观察到了更明显的 -4PACz 信号,而在目标组样本中,则在 ITO 表面追踪到了更强的 -4PACz 信号,这两者都反映了解耦共沉积策略中 SAM 的理想形貌(图 S32)。

-4PACz 的横向分布在目标组样本中也更加紧凑且均匀。在高角环形暗场扫描透射电子显微镜 (HAADF-STEM) 的截面图像中(图 3, C 和 D),由于原子序数对比,-4PACz 在较暗的 ITO 层和氧化钼 $(\mathrm{MoO_x})$ 层之间呈现为一层微弱且较亮的层。与对照组样本中厚度不规则且覆盖稀疏(部分区域测量值 $< 1\mathrm{nm}$)的情况相比,目标组样本在整个监测区域内展现出连续的覆盖以及 1 到 $2\mathrm{nm}$ 的均匀厚度 (41)。-4PACz 在基底上的横向均匀锚定通过 AFM-IR 得到了进一步证实,追踪到了 -4PACz 在 14:18 cm $^{-1}$ 处均匀分布的特征 P–C 伸缩振动信号(图 3, E 和 F)。均匀的 -4PACz 锚定增强了空穴提取并抑制了非辐射复合(图 S33 至 S37,表 S6,以及补充文本第 7 节)。此外,在高达 30 cm × 35 cm 的大面积柔性基底上实现了均匀的 -4PACz 锚定,证明了解耦共沉积策略在大面积柔性组件中的可扩展性(图 S38 至 S44,表 S7,以及补充文本第 8 节)。

A

C

B

D

F

G

H

|

J

图 3. 通过解耦共沉积实现的钙钛矿结晶和 SAM 释放。(A 和 B) 对照组 (A) 和目标组 (B) 钙钛矿薄膜的 ToF-SIMS 深度剖面图。$PbI^{-}$、$In^{-}$、$PO_{2}^{-}$ 和 $SO_{2}^{-}$ 离子的空间分布分别对应于钙钛矿、ITO、Me-4PACz 和 BSAI 的分布。(C 和 D) $MoO_{x}$ 与 PET / ITO 之间对照组 (C) 和目标组 (D) SAM 的截面 HAADF-STEM 图像。比例尺为 10 nm。(E 和 F) 对照组-ITO (E) 和目标组-ITO (F) 在 $1418\ cm^{-1}$(Me-4PACz 的 P–C 伸缩振动)处的 AFM-IR 映射图。比例尺为 2 $\mu$ m。(G 和 H) 对照组 (G) 和目标组 (H) 钙钛矿薄膜在 $N_{2}$ 吹刀处理及随后退火过程中的原位 PL 光谱。(I 和 J) 对照组 (I) 和目标组 (J) 钙钛矿薄膜在退火过程中的原位同步辐射 GIWAXS。

除了辅助 Me-4PACz 实现稳固且紧凑的锚定外,与对照组薄膜相比,解耦剂 BSAI 还能调节目标薄膜中的结晶动力学。从狭缝模涂布过程中的原位光致发光 (PL) 光谱来看,钙钛矿的生长经历了三个阶段:第一阶段是前成核阶段(阶段 I),由 $Pb_{3}I_{8}\cdot2DMF\cdot2FA$ 溶剂复合物 (42) 主导,其 强度较低。第二阶段是中间相成核(阶段 II),表现为在 $\sim780$ nm 处出现陡峭的 BSAI 激增。经过退火后,薄膜进入晶体生长阶段(阶段 III),伴随着 强度的快速上升和峰位的轻微红移。与传统的共沉积相比,在掺入 BSAI 的解耦共沉积中,阶段 I 期间 700 nm 附近的 BSAI 强度明显降低,这证明了溶剂复合物形成的有效抑制,可能是由于 BSAI 与 Pb–I 框架之间的强相互作用所致。这种强相互作用延迟了中间相的形成,从而将成核的开始时间从对照组共沉积的 22.1 s 推迟到 30.5 s(图 3, G 和 H)。此外,与目标薄膜相比,对照组薄膜在环境条件下的稳定性较差,经历了逐渐分解以及相应的 BSAI 强度下降(图 S45)。解耦共沉积中延迟的钙钛矿结晶在原位 UV–vis 吸收光谱中通过吸收边出现速度较慢而得到了进一步证实(图 S46 和补充文本第 9 节)。

延迟的结晶动力学改善了解耦共沉积策略中的钙钛矿结晶度。从原位同步辐射掠入射广角 X 射线散射 (GIWAXS) 结果来看,由于异质成核,对照组薄膜在生长早期不仅包含 $\delta$ 相,还包含具有不同 (001)、(011) 和 (111) 取向的 $\alpha$ 相晶粒。退火后,$\delta$ 相和无序的 $\alpha$ 相钙钛矿畴依然存在(图 3I)。相比之下,目标薄膜显示出对 $\delta$ 相以及具有 (011) 和 (111) 取向的 $\alpha$ 相组分的有效抑制。相反,观察到了 $\alpha$ 相 (001) 信号显著且逐渐的增长(图 3J 和图 S47),证实了在解耦共沉积中实现了面取向结晶。更详细的入射角依赖 GIWAXS 测量进一步揭示,解耦共沉积中 BSAI 的掺入促进了整个钙钛矿薄膜一致的高结晶度并消除了杂质(图 S48 至 S52 和补充文本第 10 节)。

凭借改善后的钙钛矿结晶度,我们评估了目标薄膜的大规模水平均匀性。我们通过狭缝模涂布(slot-die coated)制备了尺寸为 $5 \times 5 \, cm^{2}$、$10 \times 10 \, cm^{2}$ 和 $30 \times 35 \, ^{2}$ 的钙钛矿层,并通过光学和形貌表征检查了九个子区域(标记为 I 至 IX)(图 S8, S40 和 S53)。在对照组 $25 \, ^{2}$ 薄膜中,不同子区域的 PL 强度和吸光度存在显著差异,且这种差异在更大尺寸的样品($100 \, ^{2}$ 和 $1050 \, ^{2}$)中变得更加明显(图 4A 以及图 S54 至 S57)。相比之下,目标薄膜在所有区域的 PL 强度和吸光度变化极小,即使对于 $1050 \, ^2$ 的样品也是如此(图 4B 以及图 S54 至 S57)。此外,在扫描电子显微镜(SEM)图像(图 S58)中观察到,对照组薄膜的底部界面由于局部不可润湿性而存在大量空隙,而目标薄膜即使在整个 $1050 \, ^2$ 区域内也仅显示出致密且无针孔的微观结构(图 S59)。我们在仅添加 BSAI 的钙钛矿中观察到了类似的结晶延迟过程和定向晶格生长,这表明钙钛矿层的优化主要源于解耦剂 BSAI 与 Pb–I 框架胶体之间的强相互作用(图 S60 和补充文本第 11 节)。

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通过解耦共沉积策略提高效率与稳定性

我们通过引入 BSAI 的解耦共沉积策略(配置为 PET / ITO / 钙钛矿: Me-4PACz / 苯乙铵碘化物 (PEAI) / C $_{60}$ / 2,9-二甲基-4,7-二苯基-1,10-菲啰啉 (BCP) / 铜 (Cu))制备了柔性钙钛矿太阳能电池 (PSCs),该策略展现出快速的瞬态光电流衰减、延长的电荷载流子寿命、降低的陷阱密度以及最小化的非辐射复合(图 S61 和补充文本第 12 节)。对于通过旋涂法制备的小面积 (0.0628 cm $^{2}$) 柔性器件,采用 0.5 mg mL $^{-1}$ BSAI 的解耦共沉积策略实现了 26.9% 的记录 PCE [由 TÜV SÜD 认证为 26.9%,由德国电工协会测试与认证机构 (VDE) 认证为 26.9%,由中国光伏产品质量检验检测中心 (CPVT) 认证为 26.8%]。

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图 4. 通过解耦共沉积策略实现的柔性 PSMs 的效率。(A 和 B) 对照组 (A) 和目标组 (B) 钙钛矿薄膜 $(30 \times 35 \, \text{cm}^{2})$ 九个区域的 PL 强度映射。(C) $0.0628 \, ^{2}$ 柔性 PSCs 在 AM 1.5G 光照 $(100 \, \text{mW }^{-2})$ 下的 J-V 曲线。(D) 已报道的柔性 PSCs 的 PCE 随年份演变图。实心和空心符号分别代表认证值和实验室测量值。(E 至 G) 孔径面积为 $14.55 \, ^{2}$ (E)、$80 \, ^{2}$ (F) 以及活性面积为 $750 \, ^{2}$ (G) 的柔性模块的 I-V 曲线;插图显示了模块照片。(H) 柔性 PSCs 的 PCE 随器件面积的变化函数。(I) 不同器件面积下柔性模块的认证记录 统计。

(图 4, C 和 D,图 S62 至 S68,表 S8 至 S11,补充文本第 13 和 14 节),其性能优于使用传统共沉积方法所达到的 24.5% 。

SAM 锚定和钙钛矿结晶的高度均匀性也有助于实现高效的柔性钙钛矿太阳能模块 (PSMs)。柔性 PSMs 的详细制备过程见图 S69 和 S70。光束诱导电流 (LBIC) 映射表明,采用解耦共沉积的目标模块在整个区域内表现出更均匀且更强的外量子效率响应(图 S71)。因此,使用解耦共沉积策略的目标微模块 ($5 \times 5 \, \text{}^2$,孔径面积:$14.55 \, \text{}^2$) 实现了 23.1% 的 PCE 和 22.6% 的稳定输出(反向扫描下的认证 为 22.3%,认证稳态 为 22.2%,图 4E,图 S72 和 S73,以及表 S12),这显著高于对照组柔性子模块 (15.3%)。目标柔性 PSMs 的 PCE 同样

表现出更优异的可重复性,这由显著更窄的器件间偏差分布所证明(图 S74)。通过进一步扩大规模,我们基于解耦共沉积策略,制备了面积为 $10 \times 10 \, cm^2$(孔径面积:$80 \, cm^2$)和 $30 \times 35 \, ^2$(活性面积:$750 \, ^2$)的柔性 PSM,分别实现了 21.0%(认证值为 20.6%)和 20.6%(认证值为 20.2%)的 PCE(图 4, F 和 G,图 S75 和 S79,以及表 S12),而对照模块的 PCE 较低,仅为 11.5 和 7.95%。解耦共沉积策略表现出可忽略不计的 “规模扩大效率损失”(图 4H),并实现了商业尺寸柔性 PSM 的记录 (图 4I 和表 S13)。

我们进一步证明了解耦共沉积策略对不同基底和 SAM 分子的通用适用性。通过解耦共沉积制备的不同面积的刚性 PSM 分别实现了 24.2%(认证值为 23.8%,14.55 $^{2}$)、22.1%(80 $^{2}$)和 21.6%(750 $^{2}$)的 (图 S80 和 S81 以及表 S14)。此外,在钙钛矿前驱体中引入不同 SAM 分子,即 [2-(3,6-二甲氧基-9H-咔唑-9-基)乙基]膦酸 (MeO-2PACz)、[4-(7H-二苯并[c,g]咔唑-7-基)丁基]膦酸 (4PADCB) 和 (4-(2,7-二溴-9,9-二甲基吖啶-10(9H)-基)丁基)膦酸 (DMAcPA) 的柔性 PSM 交付了相似的 (22.5, 22.6, 和 22.8%),强调了该方法在不同 SAMs 中的广泛适用性(图 S82 和表 S15)。

为了评估柔性 PSM 的商业可行性,我们根据标准化的国际有机太阳能电池稳定性峰会 (ISOS) 协议,系统地评估了它们在光热老化、潮湿热暴露和热循环后的运行稳定性。为了尽量减少钝化对解耦共沉积策略长期稳定性评估的干扰,我们将 PEAI 替换为更鲁棒的钝化分子 1,3-二氨基丙烷二氢碘化物(图 S83 和 S84,表 S16)。如图 5A 和表 S17 所示,在 ISOS-L-3 测试条件下($85^{\circ}$ C 下 1-sun 光照及 MPPT),封装的目标柔性 PSM (5 × 5 ) 在 1044 小时后仍保留了其初始 22.0% 的 92.5%,而对照器件仅维持在 42.1%。

解耦共沉积策略首次实现了柔性 PSM 在 $85^{\circ}$ C 下的稳定运行,而之前的稳定性测试结果仅限于 $<70^{\}$ C(图 5E 和表 S18)。在 $N_{2}$ 气氛下、$85^{\}$ C 连续 1-sun 光照的未封装器件中也观察到了类似的趋势(图 S85)。目标器件在 900 小时后保留了初始效率的 91.8%,而对照器件仅为 43.0%,这证实了解耦共沉积策略显著提高了柔性模块的内在运行稳定性。在潮湿热测试($85^{\}$ C 和 85% RH, ISOS-D-3)期间,目标模块在 1050 小时后维持了初始 的 94.6%,而对照模块则降至 62.9%(图 5B,图 S86A,以及表 S17)。在 $-40^{\}$ C 至 $+85^{\}$ C 之间的热循环测试(ISOST-3)中,目标模块在 200 个循环后保留了初始性能的 95.1%,而对照模块则大幅下降, PCE 降低至初始值的 51.5%(图 5℃,图 S86B,以及表 S17)。

我们将增强的稳定性归因于两个主要因素。首先,解耦剂抑制了钙钛矿与 Me-4PACz 之间的相互作用,并促进了 Me-4PACz 在基底上的完全锚定,从而抑制了在高湿度、高温和光照条件下膦酸基团与钙钛矿之间产生的有害反应(图 S87 至 S94,补充文本第 15 和 16 节)(43)。其次,PET / ITO 上缺电子的 In / Sn 表面位点的存在促进了 Me-4PACz 以强三齿结合模式锚定,从而进一步增强了锚定稳定性(图 S95 至 S98,表 S19,以及补充文本第 17 节)。

通过在 10 mm 半径下进行循环弯曲(1% 应变,轴线 $\perp$ 电流方向),我们还评估了柔性模块的机械耐久性(图 S99 和 S100,表 S20,以及补充文本第 18 节)。在 10,000 次弯曲循环后,目标模块保留了其初始 PCE 的 92.1%,而对照模块仅保留了 75.5%。我们将这种增强的机械耐久性归因于由致密且无针孔的钙钛矿薄膜底表面所形成的增强型 SAM / 钙钛矿界面,该界面最大限度地减少了内部自由表面,从而抑制了在循环剪切应力下沿埋入界面的裂纹萌生和扩展(图 S101 至 S105,表 S21,以及补充文本第 19 节)。

为了评估在复合复杂老化条件下的运行鲁棒性,我们将 PSM 送至技术监督协会 TÜV SÜD,它们成功完成了根据 IEC TS 63163:2021(一项针对柔性便携式光伏模块的国际商业化评估标准)要求的所有测试(图 S106 和 S107,表 S17,以及补充文本第 20 节)。此外,采用解耦共沉积策略制备的刚性钙钛矿模块在封装后,根据 ISOS-L-3 协议进行 2520 小时老化后,仍保留了 \~97.4% 的 PCE,而对照器件的 PCE 则下降至 \~63.3%(图 5D 和表 S17)。刚性模块的运行寿命进一步验证了解耦共沉积策略增强稳定性的能力(图 5F 和表 S22)。

我们在两个关键场景中展示了高效柔性钙钛矿模块的实际应用:便携式充电器和遥控无人机(RC-UAV),展示了接近商业成熟的技术就绪度。这些演示中使用的柔性 PSM 重量仅为 20.31 g(相当于四张 A4 纸;见视频 S1)。在晴朗天气下(辐照度为 $1058 \, W m^{-2}$),便携式 PSM 可产生 20.5 W 的电能,并在多云的傍晚(辐照度为 $635 \, W m^{-2}$)维持 12.1 W 的输出,完全满足个人电子设备的充电需求(图 5G 和视频 S2)。将柔性 PSM 层压在 RC 无人机经过空气动力学设计的曲面机翼上,使总重量增加了 $\sim8\%$。然而,它将飞行续航时间从 8 分钟延长至 19 分钟,并将飞行范围从 $\sim4$ 公里扩大到 $\sim9.5 \, km$。这种增强在不损害飞行高度或平衡的情况下,显著扩大了 RC 无人机的飞行范围(图 5H,图 S108 和 S109,视频 S3,以及补充文本第 21 节)。

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讨论

我们通过在传统的 SAM-钙钛矿共沉积前驱体溶液中加入 BSAI 作为定制调节剂,开发了一种解耦共沉积策略。BSAI 与钙钛矿前驱体之间的强相互作用阻碍了 Me-4PACz 与钙钛矿之间的相互作用,从而促进了 Me-4PACz 在 PET / ITO 电极上的快速高效锚定,以及高质量钙钛矿薄膜的生长,这解决了在柔性基底的大面积范围内实现均匀且致密的 SAM / 钙钛矿堆叠层的挑战。这种解耦共沉积策略使小面积柔性 PSCs 达到了创纪录的 26.9% PCE(由 TÜV SÜD 认证为 26.9%,VDE 认证为 26.9%,CPVT 认证为 26.8%);同时,在基底面积分别为 25, 100, 和 1050 cm $^{2}$(有效面积分别为 14.55, 80, 和 750 cm $^{2}$ )的柔性 PSMs 上,分别实现了 23.1%(认证值为 22.3%)、21.0%(认证值为 20.6%)和 20.6%(认证值为 20.2%)的 PCE。由此产生的柔性 PSMs(器件面积 14.55 cm $^{2}$ )在 85℃ 下经过 \~1000 小时的 MPPT 后,仍保留了初始效率(22.0%)的 >92%。此外,商业规模的柔性 (器件面积 900 cm $^{2}$;PCE 19.9%)成功通过了由 TÜV SÜD 认证的 IEC TS 63163:2021 可靠性测试的所有序列。刚性 在相同条件下经过 \~2500 小时老化后,PCE 仍保持在 >97%,强调了该解耦共沉积策略的普适性。我们的工作在分子水平上提供了对 SAM 锚定与钙钛矿结晶之间竞争相互作用的机理理解,并为高效商业规模柔性 提供了一种有效且可行的调节策略。

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图 5. 柔性钙钛矿组件的稳定性与实际应用。(A) 封装的柔性 (孔径面积 $14.55 \, cm^2$ )在 1-sun 全光谱照射、85℃ 和 $\sim65\%$ RH 下运行时的 MPPT PCE 演变 (ISOS-L-3)。(B) 封装的柔性 (孔径面积 $14.55 \, cm^2$ )在 85℃ 和 85% RH 下加热时的 PCE 演变 (ISOS-D-3)。(C) 在黑暗条件下从 $-40^\circ C$ 到 $+85^\circ C$ 的热循环老化 (ISOS-T-3)。(D) 封装的刚性 (孔径面积 $14.55 \, cm^2$ )在 1-sun 全光谱照射、85℃ 和 $\sim65\%$ RH 下运行时的 MPPT PCE 演变 (ISOS-L-3)。(E) 已报道的柔性 PSCs 和 PCE 的 MPPT 稳定性 ( $T_{90}$ ) 与测试温度关系图。(F) 已报道的刚性 的 MPPT 稳定性(在 85℃ 下维持的 PCE)与寿命关系图。(G) 柔性 在 2025 年 11 月 18 日至 24 日期间的便携式充电性能和实时功率输出;深蓝色点表示辐照度。(H) 集成了柔性 的 RC-UAVs 在 2025 年 11 月 22 日至 28 日期间的功率输出;深蓝色点表示辐照度。

补充材料(SM)提供了支持本研究结论的额外信息,包括材料与方法、21节补充文本、109幅补充图、22张补充表、四段动态视频以及额外的引用文献。这些内容共同证实了实验观察结果,并验证了正文中提出的机制框架。

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参考文献与注释

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致谢

本研究得到了江苏省高校重点学术计划(PAPD)、苏州纳米科学与技术协同创新中心、苏州大学生物医学功能高分子材料设计与合成重点实验室以及清华大学柔性电子技术实验室的支持。作者感谢中国科学院纳米技术与纳米仿生研究所(SINANO)为 Nano-X 提供的技术支持。我们衷心感谢上海同步辐射光源(SSRF)提供 BL14B 光束线的使用支持。资金支持:本研究得到了以下项目的支持:中国国家自然科学基金(项目号 52325307 和 52273188,资助 Y.W.L.);中国国家自然科学基金(项目号 52573207,资助 G.Y.X.);国家重点研发计划(项目号 2024YFF1401103,资助 Y.W.L.);苏州关键核心技术项目(SYG2024146,资助 Y.W.L.);内蒙古自治区重点研发与成果转化计划项目(2025YFHH0021,资助 Y.W.L.);江苏省科技重大专项(BG2025024,资助 Y.W.L.);中国江苏省高校自然科学基金(25KJB480012,资助 G.Y.X.)。作者贡献:概念化:Y.W.L.。方法论:Y.W.L.、G.Y.X.、Y.J.C.、C.X.G.、W.J.C.、H.Y.C. 和 Q.R.C.。调查:Y.W.L.、G.Y.X.、Y.Y.W.、X.K.Z.、Y.X.S.、Q.M.、J.Y.D.、Y.Y.、W.L.、X.X.W.、Z.Y.C.、K.Q.C. 和 W.W.K.。可视化:Y.W.L.、G.Y.X. 和 Y.Y.W.。资金获取:Y.W.L.。项目管理:Y.W.L.。监督:Y.W.L. 和 G.Y.X.。论文初稿撰写:Y.W.L.、G.Y.X.、Y.Y.W. 和 T.K.Z.。论文审阅与编辑:Y.W.L.、G.Y.X.、Y.Y.W.、T.K.Z.、F.G. 和 Y.F.L.。竞争利益:Y.W.L.、G.Y.X.、Y.Y.W. 和 Y.F.L. 是由苏州大学提交的一项与本研究相关的专利申请的发明人。其余作者声明没有竞争利益。数据、代码和材料可用性:评估本研究结论所需的所有数据均可在正文或补充材料(SM)中获得。源数据和关键定量分析可在 Zenodo (44) 获取。许可信息:版权所有 © 2026 作者,保留部分权利;独家许可方为美国科学促进会(AAAS)。不对美国政府原始作品主张权利。https: / www.science.org / content / page / science-licenses-journal-article-reuse

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补充材料

材料与方法;补充文本;图 S1 至 S109;表 S1 至 S22;参考文献 (45–110);视频 S1 至 S4

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虚拟生物技术公司:一个用于治疗药物发现与开发的多智能体 AI 框架

Harrison G. Zhang\*, Peter Eckmann, Jiacheng Miao, Andrew B. Mahon, James Zou\*

全文及作者所属机构列表:https: / doi.org / 10.1126 / science.aeg6779

引言:药物发现需要整合跨生物尺度和数据模态的证据,以做出从靶点优先级排序到临床开发的系列复杂决策。相关的数据、工具和专业知识在不同组织和孤立的工作流中仍然处于碎片化状态。要克服这种碎片化,不仅需要单个的人工智能(AI)模型,还需要能够将专业知识、工具和数据组织成协调的治疗决策系统的整体系统。

基本原理:AI 智能体是配备了工具和数据库的语言模型,能够自主执行多步分析。我们推出了“虚拟生物技术公司”(Virtual Biotech),这是一个模仿药物开发公司的多智能体组织,其智能体部门涵盖靶点发现、安全性评估、模态选择和临床开发。一名虚拟首席科学官负责解读科学问题,将分析任务委派给领域专业的科学家智能体,并综合其研究结果。该系统提供了对 100 多个专业工具的访问权限,涵盖 78,726 个靶点和 39,530 种疾病,能够进行深入且细致的原始数据分析。在证据综合之前,一名科学评审员会对分析进行评议,且分析产物将被保留以确保透明度和可重复性。我们将虚拟生物技术公司应用于三个早期开发决策点:靶点优先级排序、模态选择以及临床转化失败分析。

结果:首先,虚拟生物技术公司自主标注并分析了临床试验结果,以识别与试验成功相关的药物靶点转录组特征。超过 37,000 个智能体整理了结构化的试验结果。在 55,984 项试验中,虚拟生物技术公司发现,靶向细胞类型特异性基因的药物从 phase 1 到 phase 2 的可能性高出 $40% 且上市的可能性高出 $48%,同时不良事件发生率低 32%。在考虑遗传证据后,这些关联依然存在,这表明单细胞特征为靶点优先级排序提供了与遗传学互补的信息。其次,虚拟生物技术公司评估了 B7-H3 作为肺癌靶点的潜力,整合了统计遗传学、单细胞、空间和临床基因组数据。智能体将 B7-H3 的过表达定位在癌症相关成纤维细胞中,将 B7-H3 高表达区域与免疫排除和生存率降低联系起来,并提出了一种抗体偶联药物策略。第三,该系统分析了一项针对抑瘤素 M 受体(OSMR)且已终止的溃疡性结肠炎试验。纵向单细胞分析表明,OSMR 并非该抗体旨在阻断通路的主导驱动因子,因为相关受体汇聚在同一信号通路中。在所有案例研究中,虚拟生物技术公司的表现优于三个最先进的智能体系统,能够从多种数据模态中产生更准确的试验标注和更具生物学意义的结论。人类专家重新实现了核心分析,确认了智能体的结论和代码的正确性。

一个用于治疗研究的多智能体 AI 系统。虚拟生物技术公司由一名虚拟首席科学官(中心)协调,该官引导领域专业的 AI 智能体执行早期药物发现的各项分析。在三个案例研究中,虚拟生物技术公司开展了涵盖靶点优先级排序、靶点验证与模态选择以及临床转化失败分析的多步调查。

结论:Virtual Biotech 表明,一个有组织的 AI 智能体系统能够针对早期治疗开发进行综合且多模态的推理,其规模是纯人类团队难以实现的。通过系统地将多样化的证据应用于治疗决策,同时让科学家参与其中,该系统可以帮助识别机会并支持更明智的开发选择。□

\*通讯作者。电子邮件:hgzhang@stanford.edu (H.G.Z.); jamesz@stanford.edu (J.Z.) 引用本文请注明 H. G. Zhang et al., Science 394, eaeg6779 (2026). DOI: 10.1126 / science.aeg6779

靶点优先级排序

靶点验证与模态选择

临床转化

失败分析

人工智能

虚拟生物技术公司:一个用于治疗药物发现与开发的多智能体 AI 框架

Harrison G. Zhang $^{1*}$ , Peter Eckmann $^{2}$ , Jiacheng Miao $^{1,3}$ , Andrew B. Mahon $^{4}$ , James Zou $^{1,2*}$

药物开发需要跨生物尺度和模态的证据整合,但相关工具目前处于碎片化状态。我们推出了“虚拟生物技术公司”(Virtual Biotech),这是一个模仿药物开发公司的人工智能(AI)智能体组织,其智能体部门涵盖了靶点发现、安全性评估、模态选择和临床开发。我们在三个药物开发决策点证明了其效用。首先,超过 37,000 个智能体对 55,984 项试验的结果进行了标注,发现针对细胞类型特异性基因的药物进入市场的可能性高出 48%,且不良事件减少了 32%。其次,它整合了多模态证据,提出了一个肺癌治疗策略。第三,它分析了一项已终止的溃疡性结肠炎试验,并推断了潜在的失败机制。这些结果表明,人类引导的多智能体系统可以进行透明的、多尺度的分析,从而为治疗开发决策提供信息。

药物发现是生物医学领域最具影响力且最具挑战性的尝试之一。将一种治疗药物从概念推向临床通常需要十多年的开发时间,且成本高达数十亿美元 (1-3)。尽管有这些投入,进入 1 期试验的候选药物中约 90% 最终未能获得批准,失败的主要原因通常是疗效不足和安全性缺陷 (4-7)。为了降低这种损耗,现代药物发现越来越多地利用来自多种来源的证据来验证靶点,包括但不限于人类遗传学、功能基因组学、单细胞和空间图谱、结构生物学、药物化学以及临床医学 (8)。

组织和科学上的瓶颈限制了这些证据在实践中的正确使用。收集和分析这些证据的专业知识分散在不同的学科、格式和生物尺度中,导致工作流程孤立 (3, 9, 10)。此外,权衡截然不同且有时相互冲突的证据非常困难,特别是当组织动态或不同的先验信念影响决策时 (3, 9)。碎片化的团队在记录工作流程时也各不相同,使得研究结果难以审计,决策过程难以重建 (3, 11, 12)。此外,近期生物数据规模的爆炸式增长使得跨模态的手动整合变得更加困难 (3, 9)。因此,尽管数据驱动方法取得了进展,早期药物开发仍然缓慢、资源密集且容易失败 (1-7)。

人工智能(AI)智能体被提议用于加速涉及大量数据分析的科学任务,因为它们是配备了工具和数据库的语言模型,能够自主执行复杂的多步任务。通过指定角色并提供特定领域的工具(如生物信息学软件),可以让智能体专门从事某一类任务。最近的研究还探索了多智能体系统,即由多个专业智能体协作解决复杂问题 (13)。

在此,我们介绍“虚拟生物技术公司”(Virtual Biotech),这是一个多智能体 AI 研究平台,能够检索、分析并整合多模态证据,以回答人类早期治疗药物发现中的科学问题。一个虚拟首席科学官(CSO)编排者将查询分解为可管理的子任务,将其分派给专业的 AI 科学家智能体,并对其结果进行推理。这种结构化的协作鼓励对原始证据进行深入的数据驱动分析,并允许使用统一的推理层权衡不同的证据来源,从而得出细致的结论。

智能体系统在化学和 AI 研究自动化等科学领域已经展现出潜力 (14–17)。在生物医学领域,针对特定工作流定制的智能体方法已经出现,其应用涵盖基因编辑、空间和单细胞组学、罕见病诊断以及纳米抗体设计 (18–22)。最近的研究通过整合更广泛的工具、数据库和代码执行工作流以进行通用数据分析,扩展了智能体推理的领域 (23–28)。尽管如此,这些框架主要集中在生物数据分析上,且通常由单个智能体管理。相比之下,Virtual Biotech 是一个多智能体系统,专门为贯穿整个人类治疗研发管线的转化推理而设计。通过协调对大规模且复杂的药物研发数据进行分析,该系统能够以整体的、数据驱动的推理方式回答科学问题。

我们首先描述 Virtual Biotech 的工具环境和多智能体编排。随后,我们将展示三个转化案例研究,旨在证明 Virtual Biotech 如何为早期治疗药物发现和开发中的关键决策点提供证据。第一个案例研究侧重于通过将靶点层面的分子特征与临床试验结果相结合,进行大规模的靶点优先级排序。第二个案例从靶点验证和模态选择的角度,探讨肺癌中的药物靶点 B7-H3。第三个案例则调查一项已终止的 oncostatin M 受体 (OSMR) 溃疡性结肠炎试验,以推断临床转化失败的可能原因,并概述由生物标志物驱动的临床开发策略。

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结果

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虚拟生物技术公司概览

虚拟生物技术公司(Virtual Biotech)模拟了一个跨功能的治疗研究组织。它由四个科学家智能体部门组成,负责处理药物研发管线中的关键步骤(图 1A 和表 S1)。每个部门中具有领域专业知识的科学家智能体拥有互补的专业技能和领域特定工具,使他们能够跨翻译光谱查询、分析和整合生物医学信息,从而对药物研发问题进行基于证据的评估(详见“材料与方法”)。

我们创建了领域特定的模型上下文协议(MCP)服务器,为主要的生物医学数据库和知识源提供统一的程序化接口,将异构数据格式和查询 API(应用程序编程接口)的复杂性抽象为标准化工具(图 1B 和补充文本 I)(29–31)。每个科学家智能体通过访问经过策划且与专业知识相匹配的 MCP 工具,从相关来源收集证据,将静态数据库转化为交互式知识层,智能体可根据用户问题对这些知识层进行动态分析。

我们开发了专门的 MCP,为虚拟生物技术公司的科学家智能体提供 >100 种分析工具,用于审视大规模、异构的生物医学数据,涵盖 78,726 个靶点、39,530 种疾病、1450 万个蛋白质-蛋白质相互作用、>300 万个可靠的遗传集以及 >1 亿个单细胞图谱 (32, 33)。该平台进一步整合了化学信息学和药理学资源,涵盖 18,119 种药物、6332 种不同的作用机制、114,270 份美国食品药品监督管理局(FDA)不良事件报告,

A

图 1. 虚拟生物技术公司 AI 智能体、工具及编排流程概览。(A) 多智能体 AI 系统组织及科学部门。(B) 按领域划分的模型上下文协议(MCP)服务器概览,这些服务器提供定制化工具以查询和分析多样化的生物学和临床数据源。(C) 虚拟生物技术公司的工作流程。针对用户查询,虚拟首席科学官(CSO)在进行高成本分析之前,首先提出任何相关的后续问题以明确用户意图。与此同时,幕僚长智能体准备一份关于该主题的简报,包含最新进展、数据可用性和一般领域背景。随后,虚拟 CSO 协调专业科学家智能体部门进行分析以回答用户查询。接着,科学评审智能体评估科学家智能体的方法论和主张,CSO 在审查反馈后,要么协调科学家智能体进行修正分析,要么将证据综合成一份报告。

32,783 个药物基因组学变异,以及来自 Tahoe-100M 的药物扰动表达测量值 (34)。此外,可通过我们的 MCP 访问 ClinicalTrials.gov 的记录 (35)。科学家智能体还可以通过 PubMed 查询生物医学文献,并通过基于 Web 的工具检索额外的定向数据集。这些资源主要以人类为中心,因此支持针对数据中所代表的人类疾病进行以靶点为中心的查询。

我们为虚拟生物技术公司开发了一个用户界面,用于显示智能体的推理过程,指示当前正在使用的工具,并允许用户下载每次会话期间生成的相应数据、可重复代码和报告(图 S1)。

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虚拟生物技术编排

在接收到用户查询且在启动科学家工作之前,虚拟首席科学官(CSO)会启动其自身的战略导向(图 1℃ 和补充文本 II)。其幕僚长代理首先生成一份关于通用领域认知、数据概况和最新进展的简报,以帮助虚拟 CSO 构建分析框架,为用户设定合理的可行性预期,并确定关键问题。与此同时,虚拟 会对用户进行访谈,以明确用户的意图并增强人机协作的一致性 (36, 37)。在获得简报后,虚拟 将任务路由至相关的科学家代理(图 1℃)。

在科学家代理完成分析后,科学评审代理会对他们的输出进行评估,以了解其在多大程度上解决了用户的原始问题、支持其结论的证据强度以及分析的整体彻底程度(图 1℃ 和补充文本 III)。如果科学评审代理发现了漏洞或未经证实的主张, CSO 将重新委派给相关的科学家代理进行迭代优化。

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靶点优先级排序:Virtual Biotech 将临床前生物学与临床结果相结合,以识别与试验成功相关的药物靶点特征

药物研发项目面临着巨大的损耗,其中缺乏疗效和安全性问题导致了约 79% 的临床试验失败 $(38)$。早期的靶点优先级排序工作已经证实,有人类遗传学证据支持的靶点更有可能通过临床开发 $(39-41)$。为了扩展这些结果以实现更好的靶点优先级排序,我们将之前的这项工作提供给 Virtual Biotech,并指示该系统批判性地评估其自身的基础设施,并建议扩展此分析的方向 $(40)$。虚拟 CSO 使用其临床试验员代理(clinical trialist agent)为包含 55,984 项试验的 Open Targets 临床试验数据集补充了额外的结果标注。它还建议使用其单细胞代理,参考 Razuvayevskaya 等人的研究 $(33, 40, 42)$,设计基因组特征以进行与试验结果的关联测试。基于代理的结果标注是必要的,因为原始的 Open Targets 数据集缺乏终点数据,且 ClinicalTrials.gov 的记录经常提供不完整、不一致或仅为自由文本的结果 $(43, 44)$。因此,需要通过代理进行策展,以标准化结果,并从出版物和新闻稿等来源中恢复缺失或冲突的数据。

大规模并行且可追踪来源的试验结果提取:临床试验员代理提出了用于大规模提取的关键结果变量,包括试验阶段的进展、主要和次要终点结果以及不良事件率。它开发了一套系统协议,用于从出版物和新闻稿等来源获取试验结果。工作流程始于人类用户指示虚拟 CSO 为 Open Targets 数据集中的 2 期和 3 期试验策展临床试验结果。虚拟 CSO 将这一目标转化为一个分布式提取任务,并将协议设计委派给一个临床试验员代理,该代理指定了所需的结果字段、证据层级和来源追踪要求。随后,虚拟 CSO 并行调度了 37,075 个临床试验员代理,每个代理被分配到一个国家临床试验标识符(NCT ID)(图 2A)。在这种规模下,如果没有并行化,全面的策展是不切实际的,因此需要一个能够以分布式方式执行数据策展的多代理架构。

每个临床试验员代理为其分配的 NCT ID 遵循一个三级证据级联:首先系统地查询 ClinicalTrials.gov 数据库;当主要数据不完整时,然后在 PubMed 中搜索包含试验结果的出版物;最后查阅在线新闻稿和监管公告(图 2A 和补充文本 IV)(35)。代理记录了每项标注的信息来源。每项试验的 Anthropic API 费用中位成本为 \$0.23。对于 1 期试验,成功在算法上被定义为进展到 2 期,因为 1 期试验评估的是安全性及其剂量,而非疗效。

为了评估标注质量,研究人员对随机选择的 100 项临床试验进行了人工审核,结果显示:主要终点与代理标注的一致性为 88.4%(在 86 项适用试验中占 76 项),次要终点的一致性为 88.4%(86 项中占 76 项),不良事件率的一致性为 92.4%(在报告精确统计数据的 66 项中占 61 项)。此外,在与人工策展的 Therapeutic Data Commons (TDC) 试验结果预测数据集重叠的 7666 项试验中,主要终点的一致性为 85.6%(详见“材料与方法”部分)$(45)$。这些一致性指标表明,代理能够可靠地标注试验,且所得标签适用于分析。

利用单细胞图谱进行翻译特征工程:为了推导药物靶点的单细胞表达特征,单细胞智能体为 Tabula Sapiens(一个包含 27 种组织的健康人类参考图谱)提出并实现了一个全面的特征提取框架 (46)。该智能体设计的特征分为两类:细胞类型特异性指标和表达异质性度量。对于特异性,智能体提出了 tau 细胞类型特异性指数,其中数值接近 0 表示普遍表达,而数值接近 1 则表示表达局限于单一细胞类型 (47)。为了捕捉细胞群体内的表达异质性,智能体提出了一种双峰系数,该系数由表达细胞中表达分布的偏度和峰度计算得出,较高的数值可能表明组织内存在“开启 / 关闭”的表达模式 (48, 49)。虽然基因表达分析中已经提出了多种双峰度量方法,但这种最初开发于心理学和社会科学的特定双峰系数,是一种尚未被充分探索且具有可解释性的基因表达双峰指标 (50–55)。这两个特征呈中度相关(Pearson $\rho = 0.54$),表明它们提供了一些互补信息。

虚拟生物技术驱动的分析揭示了与试验成功相关的基因组特征:最终的集成数据集包含 55,984 项临床试验,涵盖 1 期 (n = 14,237)、2 期 (n = 22,164)、3 期 (n = 14,911) 和 4 期 (n = 4672) (图 2B)。试验层级的结果标注与虚拟生物技术提取的靶点层级分子特征以及来自 Open Targets 的遗传证据评分相关联。

临床试验专家智能体首先成功复制了 Razuvayevskaya 等人报道的遗传证据结果,发现遗传支持与试验进展相关,并且能防止试验过早停止 (图 S2A) (40)。利用虚拟生物技术整理的额外试验结果,它还发现,那些达到主要终点且不良事件较少的试验在遗传证据方面更为丰富 (图 S2, A 和 B)。参考关于遗传证据的类似研究方法,临床试验专家智能体随后评估了药物靶点的单细胞转录组特征与试验结果之间的关联 (39, 40)。

A

B

图 2. 使用虚拟生物技术进行的大规模临床试验数据提取。(A) 数据提取和整理过程概览。对于每个国家临床试验 (NCT) ID,临床试验专家智能体通过调用 ClinicalTrials.gov、PubMed 和网络的工具来收集有关该试验的信息。在对发现进行推理后,智能体将信息输入到结构化的 JSON 本体中以进行下游分析。(B) 整理后的临床试验数据集 (n = 55,984) 的桑基图,显示了试验阶段、试验状态和结果。

tau 细胞类型特异性和表达双峰评分均与临床开发阶段的试验进展相关 (图 3A)。在根据 tau 指标将靶点二值化为细胞类型特异性类和广泛表达类后(详见材料与方法),临床试验专家智能体发现,作用于细胞类型特异性靶点的药物进入 4 期的可能性高出 48%。

具有更高细胞类型特异性的靶点更有可能达到定义的主要终点 [比值比 (OR) = 1.12;95% 置信区间 (CI):1.09–1.14]、次要终点 (OR = 1.12;95% CI: 1.09–1.14),以及成功从 1 期推进到 2 期 (OR = 1.27;95% CI: 1.22–1.33)(图 3A)。具有细胞类型特异性靶点的药物从 1 期推进到 2 期的可能性高出 40%。同样,具有较高表达双峰得分的靶点更有可能实现阳性主要终点、阳性次要终点以及成功从 1 期推进到 2 期(图 3A)。

虚拟生物技术公司(Virtual Biotech)进一步发现,靶点具有更高细胞类型特异性和表达双峰得分的试验,在许多器官系统中报告的不良事件率较低(图 3B)。测试细胞类型特异性靶点的试验,其不良事件率平均低 $32%。这表明,具有更异质且细胞类型受限表达模式的靶点可能会提供更好的安全性。

接下来,我们证明了这些发现对混杂因素具有鲁棒性。为了评估观察到的关联是否可能是由偶然因素或复杂的“试验-靶点”映射中的混杂因素引起的,我们进行了 >1000 次迭代的排列检验,确认所有发现相对于经验排列零假设均保持统计学显著性(排列 P < 0.05)(图 S3, A 和 B)。为了控制疾病适应症之间以及药物模态之间潜在的混杂影响,我们进一步使用针对试验阶段和入组年份进行调整的混合效应模型来估算 OR,并将药物模态和疾病适应症领域作为随机效应。细胞类型特异性和表达双峰得分的调整后比值比在混合效应模型中依然保持统计学显著性(图 S3, C 和 D)。

另一个关键问题是,靶点的单细胞转录组特征是否在已建立的将靶点与疾病联系起来的人类遗传证据之外,提供了独立价值。因此,我们在调整遗传证据后复制了我们的发现。调整后,试验结果与两种单细胞特征(细胞类型特异性和表达双峰得分)之间的关联依然保持统计学显著性,且效应值的降低可以忽略不计(图 S4, A 和 B)。我们进一步估算了没有遗传证据的试验(占试验的 75%)中单细胞特征的 OR,发现单细胞特征在该子集中具有相似甚至更强的效应值(图 S4, C 和 D)。综上所述,这些结果表明,单细胞信息捕捉到了除遗传证据之外的、与临床试验结果相关的额外生物学信号。Dann 等人最近的一份报告同样发现,细胞类型受限的靶点与阶段推进相关,但并未研究其与终点或不良事件的关联 (56)。

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靶点验证与模态选择:虚拟生物技术研究为肺癌 B7-H3 抗体偶联药物开发构建临床前理论依据

A

接下来,我们研究了一个常见的药物项目级决策点:多模态证据是否能够支持在特定疾病背景下,针对一个提名靶点形成连贯的治疗假设和模态选择。为了证明虚拟生物技术公司(Virtual Biotech)快速生成严谨证据以支持该任务的能力,我们提示系统评估 B7-H3(也称为 CD276)在肺腺癌(LUAD)和小细胞肺癌(SCLC)中的治疗潜力。B7-H3 是一种跨膜免疫检查点蛋白,在包括肺癌在内的实体瘤中高度表达 $57$。其受体尚不明确,且其在癌症中的作用仍不清晰,尽管它可能同时具有免疫学和非免疫学功能 $58$。用户的初始查询为:“评估 B7-H3 作为肺癌靶点的治疗候选资格。”虚拟首席科学官(CSO)将其解读为一项治疗靶点评估任务,并将其分解为一组证据生成模块,涵盖人类遗传学、靶点生物学、单细胞转录组学、空间转录组学、基于生物标志物分层的生存分析以及先前的临床试验数据。

统计遗传学代理首先评估了 B7-H3 作为肺癌靶点的生殖系遗传支持。在 B7-H3 位点未发现与肺癌相关的显著关联或可信集,该代理得出结论,B7-H3 作为肺癌靶点的生殖系遗传证据较弱(图 4A)。尽管如此,虚拟 CSO 正确地将全基因组关联研究(GWAS)信号的缺失解读为非排除性的,并指出对于潜在的免疫检查点靶点,治疗依据可以源自体细胞肿瘤的过表达,而非生殖系风险变异。这一推理将 B7-H3 与那些必须依赖遗传证据的靶点区分开来。

B

图 3. 与关键临床试验结果显著相关的药物靶点临床前单细胞图谱特征。(A) 药物靶点的单细胞衍生特征与阶段进展、试验停止及疗效结果之间的关联。图表显示了标准化比值比(所有特征均标准化为标准差 1)及 95% 置信区间(CIs)。(B) 单细胞衍生特征与按器官系统分组的严重不良事件发生率之间的关联。森林图显示了 beta 回归系数及 95% 置信区间(CIs)。

A

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“评估 B7-H3 (CD276) 在肺癌中的治疗潜力...

B

\- 在四项人群水平的肺癌 GWAS 中未发现 B7-H3 变体或可信集。

\- 未发现机器学习得出的位点到基因的因果预测。

\- 遗传约束显示,预测的 LoF 观察值 / 预期值比率为 0.67,表明对 LoF 具有中度耐受性。

\- ENCODE E2G 在正常肺部的 B7-H3 位点识别出高置信度的调节区域,支持强调节活性。

\- 有限的生殖系证据并不能否定治疗潜力。其原由可能源于体细胞肿瘤的过表达而非遗传风险。

继续进行基于表达的分析。”

C

“LUAD 和 SCLC 的肿瘤富集 B7-H3 表达在癌症相关成纤维细胞 (CAFs) 中最强,而非恶性细胞。

下一步是了解细胞间通信如何被破坏,以及 B7-H3+ CAFs 向免疫细胞发送什么信号。这弥补了已知哪些细胞表达 B7-H3 与理解其功能之间的差距。”

E

“Visium LUAD 空间转录组分析表明,B7-H3 的表达促成了一个免疫排除生态位。混合效应模型显示,相对于 B7-H3 低表达点,高 B7-H3 表达点周围的免疫细胞丰度降低。这为已识别的免疫抑制配体-受体相互作用提供了空间验证。

我想了解这种免疫抑制表型是否能转化为具有临床意义的生存差异。”

验证,促使虚拟 CSO 指令其单细胞代理执行分析以获得更清晰的结果。

该单细胞代理查询并下载了来自 CELLxGENE Census 的单细胞图谱,包括 SCLC 图谱中来自 9 位捐赠者的 62,341 个细胞,LUAD 图谱中来自 69 位捐赠者的 337,002 个细胞,以及来自 26 位健康捐赠者肺组织的 86,478 个细胞(图 4B)(59)。该代理进行了带有伪体块(pseudobulk)聚合的细胞类型解析差异表达分析,结果显示 B7-H3 的上调在所有细胞类型中并非均匀分布,而是集中在 SCLC $\left[\log_{2}\text{ fold change (log2FC)} = 2.13, \text{ false discovery rate (FDR) adjusted P value} = 3.5 \times 10^{-9}\right)$ 和 LUAD ( $\log_{2}FC = 1.79, FDR P value = 2.0 \times 10^{-8}$ ) 的成纤维细胞中(图 4℃)。

F

“查询 CELLxGENE Census 的 LUAD、SCLC 和健康肺图谱,以在单细胞分辨率下表征 B7-H3 的表达。执行 QC,使用 Harmony 纠正批次效应,使用 UMAP 可视化图谱。”

“B7-H3+ 成纤维细胞显示出免疫抑制程序。

接下来让我们分析空间转录组,以验证这些预测的免疫抑制相互作用是否转化为物理上的免疫排除表型。”

“B7-H3 似乎是 NSCLC 中的一个潜在预后生物标志物。结合免疫排除的空间证据,这些结果支持了 B7-H3 介导的免疫抑制导致不良临床结果的假设——为在肺癌中将 B7-H3 作为治疗靶点提供了机制和临床依据” 图 4. Virtual Biotech 将 B7-H3 (CD276) 作为肺癌的治疗靶点进行评估。(A) 统计遗传学智能体关于 B7-H3 在肺癌中生殖系遗传发现的总结。(B) 由单图谱智能体准备的肺腺癌 (LUAD) 和小细胞肺癌 (SCLC) 单细胞图谱的 UMAP。(C) 按类型进行的 B7-H3 差异表达分析显示,成纤维细胞中的表达显著增加。(D) 集成——由单智能体进行的通信推断揭示了在 SCLC(如图所示)和 LUAD(图 S5)的 B7-H3+ 癌症相关成纤维细胞中发现的独特信号通路。(E) LUAD 原发部位组织的空间转录组分析显示,相对于 B7-H3 表达量最低的四分位数点,B7-H3 表达量最高的前四分位数点中存在免疫排除生态位。柱状图量化了 12 个 LUAD 肿瘤样本中,B7-H3 表达量最高和最低四分位数点之间相邻免疫丰度的百分比变化(基于 10,000 次重采样 95% 的自助法置信区间)。统计显著性使用线性混合效应模型进行评估,该模型将局灶点总 UMI 计数、成纤维细胞丰度、恶性上皮丰度和内皮丰度作为固定效应进行调整,并将患者以及患者内的样本作为嵌套随机效应( $P < 0.01$ , $*P < 0.001$ )。(F) 对来自癌症基因组图谱 (The Cancer Genome Atlas) 项目的肺腺癌队列进行生存分析,确定 B7-H3 为无病生存期的潜在预后生物标志物。

基于这些发现,单智能体假设 B7-H3 高表达的成纤维细胞可能会积极塑造一个免疫抑制的肿瘤微环境 (TME)。随后,它进行了配体-受体相互作用分析,以识别 B7-H3 表达量处于群体最高四分位数与最低四分位数的成纤维细胞之间在信号传导上的差异 (60)。这在 SCLC 中识别出 180 个显著相互作用,在 LUAD 中识别出 226 个相互作用(详见材料与方法),这些相互作用特异性地存在于 B7-H3 高表达成纤维细胞与免疫细胞的通信中(图 4D 和图 S5A)。单智能体识别出五个主要的信号组:从免疫表面释放激活配体的脱落酶、将巨噬细胞极化为免疫抑制状态的髓系重编程介质、重塑肿瘤血管的新血管生成因子、与抑制性受体结合的免疫抑制细胞因子,以及将免疫细胞保留在成纤维细胞生态位中的趋化因子通路。这些结果表明,B7-H3 高表达的基质细胞可能利用 B7-H3 标准检查点功能之外的额外免疫调节机制。

随后,科学评审代理被派遣,并指出配体-受体分析是从解离的单细胞数据中推断细胞间通信的,而这些数据丢失了空间组织背景。因此,虚拟首席科学官(CSO)推论需要进行空间分析,以验证这些预测的免疫抑制相互作用是否对应于物理上的免疫排除表型。随后,它派遣单细胞代理分析了一个 Visium 数据集,该数据集包含来自诊断为 LUAD 患者的 12 份肺组织样本,共计超过 25,000 个空间分辨率点 (61)。为了推断点级别的细胞类型丰度,单细胞代理使用先前的 LUAD 单细胞图谱作为参考,应用了 Cell2Location (图 S5B) (62)。接着,它实施了一个混合效应回归模型,以评估表达 B7-H3 处于前四分位数的点,其紧邻空间邻域内的免疫细胞组成是否相对于后四分位数的点有所改变。B7-H3 高表达点显示出邻近免疫细胞(如 T 细胞、巨噬细胞、单核细胞和树突状细胞)的丰度较低 (图 4E)。值得注意的是,这些效应显示出空间衰减,因为在紧邻邻域(Visium 点周围的第一层六边形环)中缺失最严重,并在第二层和第三层环中逐渐减弱,这与局部排除机制一致。这证明了 B7-H3 的表达在空间上与免疫排除的 TME 相关,支持了免疫抑制表型的假设。

接下来,虚拟 CSO 想要了解这种免疫抑制表型是否对应于患者预后的差异。虚拟 CSO 指派临床试验代理对 TCGA PanCancer Atlas LUAD 队列进行生物标志物分层生存分析,该队列包括 477 名具有基因表达测量值和详细生存结果的患者 (63, 64)。为了最大限度地分离生物学上的不同组别,临床试验代理根据 B7-H3 表达四分位数对患者进行分层,基于 B7-H3 表达情况比较前四分位数和后四分位数的患者 (图 4F)。在针对年龄、癌症分期和性别进行调整的 Cox 比例风险模型中,B7-H3 高表达与较差的总生存期 [风险比 (HR) = 1.62; 95% CI: 1.05–2.49; P = 0.028] 和较差的无病生存期 (HR = 2.06; 95% CI: 1.08–3.90; P = 0.027) 显著相关。结合免疫排除的空间证据,虚拟 CSO 认为 B7-H3 介导的免疫抑制可能会导致不良的临床结果,从而为在肺癌中靶向 B7-H3 提供了机制和临床依据。

最后,虚拟 CSO 派遣靶点生物学家代理来确定最佳治疗形式。该代理检索了 Human Protein Atlas 数据,确认了 B7-H3 的细胞表面表达及其亚细胞囊泡定位 (65)。结合单细胞研究发现 B7-H3 主要在 TME 成纤维细胞而非仅在恶性细胞中过表达,这促使虚拟 CSO 提名一种抗体偶联药物 (ADC)。CSO 推论 ADC 可以通过三种与这些发现一致的机制发挥作用:将细胞毒性载荷递送到表达 B7-H3 的癌细胞中;通过抑制 B7-H3 介导的免疫抑制检查点相互作用来改变 TME;以及对相邻的 B7-H3 阴性癌细胞进行旁观者杀伤。在药理学家代理的可开发性分析未发现现有化学结合剂后,小分子和蛋白降解靶向嵌合体 (PROTAC) 方法被降低了优先级。

本案例研究在没有进行网络搜索的情况下开展,以防止信息泄露,且底层语言模型的知识截止日期为 2025年1月。值得注意的是,现有文献强调 B7-H3 在癌细胞上的表达及其典型的检查点相关功能,这使得基于抗体和 ADC 的研发项目在很大程度上是通过以癌细胞为中心的视角来推动的 (57, 58)。相比之下,虚拟生物技术公司(Virtual Biotech)整合证据,提出了一个探索较少但在机制上自洽的假设:B7-H3 在癌症相关成纤维细胞中过度表达更为强烈,在空间上与免疫排除相关,并能对不良临床结果进行分层;这一解读无法直接从任何单一数据集或出版物中得出。2025年8月,FDA 授予 ifinatamab deruxtecan “突破性疗法认定”,这是一种首创的 B7-H3 靶向 ADC (66–68)。由于虚拟生物技术公司无法获取此信息,该监管公告为该系统的机制驱动治疗设计提供了外部支持。

这一系统化且数据驱动的分析共耗费了 $50.00 的 Anthropic API 额度。它展示了虚拟生物技术公司如何加速靶点验证和模态选择,而这通常是由跨职能药物研发团队执行的手动过程。完整的对话记录见补充文本 V。

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临床转化失败分析:Virtual Biotech 识别针对溃疡性结肠炎中 OSMR 的首创单克隆抗体 (mAb) 已终止的 2 期临床试验的可能失败机制

随后,我们使用 Virtual Biotech 分析了后期临床开发失败的案例。我们重点关注了 2 期 MOONGLOW 研究 (NCT06137183),这是一项针对溃疡性结肠炎 (UC) 的试验,旨在评估肿瘤生长抑制因子 M 受体亚单位 OSMRβ 作为治疗靶点的潜力 (69)。OSMRβ 是一种细胞因子受体亚单位,它与 gp130 形成异源二聚体,以介导与炎症和纤维化相关的肿瘤生长抑制因子 M 信号通路,例如 JAK-STAT (70, 71)。先前的研究表明,黏膜 OSMR 表达升高似乎标志着一种治疗耐药的 UC 炎症状态,且黏膜 OSMR 表达与抗 TNF(肿瘤坏死因子)无反应独立相关 (71–73)。

Vixarelimab 是一种旨在阻断 OSMRβ 介导信号传导的首创 mAb (69)。在 MOONGLOW 研究中,中至重度 成年患者被随机分配接受 vixarelimab 或安慰剂。然而,该试验于 2025 年 6 月终止,因为中期无效性分析表明原 endpoints(主要终点)不太可能实现 (69)。因此,向虚拟首席科学官 (CSO) 提出的初始查询为:“我们想了解试验 NCT06137183 终止的原因。该试验在 OSMR 患者中测试了一种针对 OSMR 的首创单克隆抗体。结果已经公布,试验因中期无效性分析显示缺乏疗效而终止。此次终止与安全性顾虑无关。”虚拟 CSO 将其解读为一项临床转化失败分析,并将该查询分解为若干子任务,重点关注试验方案和入组资格审查、OSMRβ 信号传导的机制评估、治疗耐药肠道组织中的通路冗余分析,以及 OSMR 相关基质激活程序的跨疾病探索。

临床试验专家智能体首先利用 ClinicalTrials.gov 记录分析了试验设计,其中包含了完整的研究方案 (Protocol GA44839, Version 2 PDF) (69)。它重点关注了入组标准,指出该试验筛选的是对常规或先进疗法反应不佳的治疗耐药 患者研究群体 (图 5A) (69)。由于药物靶点 OSMRβ 通过 JAK-STAT 通路传导信号,该智能体推论,了解 OSMRβ 在治疗耐药 生物学中是作为 JAK-STAT 信号传导的主要驱动因子,还是仅代表进入同一信号级联反应的一个冗余切入点,至关重要。

为了回答这个问题,单细胞智能体随后独立识别了 TAURUS 数据集(来自 20 名 患者的 435,857 个细胞),以调查 MOONGLOW 的失败机制,因为该数据集是抗 TNF 治疗前后收集的 OSMR 肠道活检单细胞转录组图谱。该智能体推论,与治疗初试的 OSMR 图谱相比,该数据集能够调查来自生物制剂无反应者的 OSMR 细胞状态,而这些患者与 MOONGLOW 的特定患者群体相似 (74)。

通过访问原研究的补充材料,该智能体首先确认,在治疗后,OSMR 的表达仅在非响应者的三种成纤维细胞状态中增加,这与该试验针对此受体的理论依据以及现有研究 $(71, 72)$ 一致。随后,该智能体设计了原研究中未包含的计算实验。为了研究这种 OSMR 上调如何影响下游信号传导,该智能体利用 CollecTRI 调节子数据库实现了转录因子 (TF) 活动的全基因组筛选,并应用混合效应模型来识别治疗后组织中非响应者与响应者之间具有差异活性的 TF $(75)$。此次筛选显示,在表达 的非响应者基质中,STAT1 的活性普遍升高,在 10 种基质细胞类型中的 9 种中达到了显著水平(FDR 校正后,混合效应 P < 0.05)。这证明了 $\beta$ 下游的 JAK-STAT 信号轴在治疗耐药组织中持续处于激活状态。

然而,该智能体注意到目标生物学的一个关键结构方面:$\beta$ 与 gp130 (IL6ST) 形成异二聚体,而 gp130 是白细胞介素-6 (IL-6) 细胞因子家族(包括 IL-6, LIF, IL-11, CNTF, 和 CT-1)共用的信号传导亚单位。这一观察结果引发了疑问:持久的 STAT 激活在多大程度上真正归因于 $\beta$ 本身,还是由其他汇聚在同一通路上的 gp130 家族受体介导的。为了量化每个受体对推断的 STAT1 活动的贡献,该智能体针对非响应者治疗后组织中每种基质细胞状态内的 gp130 家族受体基因,设计了一种基于 Shapley 值的方差分解分析。分析发现,尽管 是药物靶点,但在大多数表达 的基质细胞类型中, OSMR 表达对 STAT1 活动产生的变异贡献低于其他共受体(图 5B)。这些发现提出了这样一种可能性,即在治疗耐药性溃疡性结肠炎 (UC) 的生物学背景下,抗 $\beta$ 疗法仅构成了部分阻断。这一概念与最近的一项研究一致,该研究报告称,治疗耐药性 UC 可能反映了通过平行受体复合物持续存在的炎症通路,而这些复合物汇聚在相同的下游通路中 (76)。

随后,该智能体假设,如果 gp130 轴内的冗余性导致了治疗耐药性 UC 的生物学特性,那么一个捕捉基线 gp130 轴表达的综合评分,可能比单独使用 能更好地预测治疗的非响应情况。因此,这位临床试验智能体设计了一个 gp130 轴风险评分(详见“材料与方法”),并在四个接受英夫利昔单抗治疗的 UC 队列数据集 (77–80) 中,将其性能与单独的 OSMR 表达以及此前报道的五基因非响应特征进行了比较。在所有四个队列中,gp130 轴评分的性能始终优于单独的 (图 5℃)。尽管 gp130 轴评分完全源自智能体之前的单细胞机制洞察,而非来自监督基因筛选,但其在所有队列中的表现与 Arijs 特征相当。这些发现支持了以下假设:gp130 信号轴而非单独的 $\beta$ 能更好地捕捉 UC 中的治疗耐药性疾病。

最后,虚拟生物技术公司(Virtual Biotech)研究了 OSMR 的上调是溃疡性结肠炎(UC)所特有的,还是反映了跨疾病的保守基质激活程序。它通过查询 CELLxGENE Census 单细胞图谱中代表的 112 种疾病的 OSMR 通路基因表达,进行了一次系统的跨疾病表达调查,并应用线性混合模型来测试相对于健康组织而言疾病特有的 OSMR 上调情况,同时考虑了捐赠者和数据集的批次效应(图 5D)(59)。该调查分析恢复了在 UC、结直肠癌和胃癌的基质成分中,以及心肌炎的心肌细胞中已知的 OSMR 生物学特性 (74, 81–83)。除此之外,虚拟生物技术公司还强调了 OSMR 在急性肾损伤、毛细胞性星形细胞瘤、牙周炎以及阿尔茨海默病及相关痴呆症中的作用,其表达增加主要集中在成纤维细胞、内皮细胞或神经元细胞类型中。 OSMR 表达在解剖学和病因学多样化的疾病中富集,表明存在一种与慢性炎症相关的保守疾病程序。这种跨疾病信号提出了这样一种可能性,即以 为导向的治疗策略在 UC 之外可能具有相关性。

综上所述,这次回顾性评估证明了虚拟生物技术公司可以从一项已终止的临床研究开始并产生机制性见解。这些智能体结合了试验方案审查、治疗耐药研究人群的目标生物学、单细胞信号询问、生物标志物性能比较以及跨疾病表达挖掘,从而得出了缺乏疗效的统一原由:$\beta$ 可能标记了 UC 中一种治疗耐药的基质炎症表型,但在相关的 OSMR 表达细胞状态中,它可能不是下游 JAK-STAT 信号传导的主要驱动因素。相反,这些发现指出,沿 gp130 轴的更广泛冗余是治疗耐药 UC 生物学更准确的表征,从而能够推导出一种复合生物标志物,在预测独立队列的无反应率方面优于单独的 。该案例研究完成的总成本为 59.00 美元的 Anthropic API 积分,完整的对话记录见补充文本 VI。

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Virtual Biotech 分析的正确性与可复现性

为了评估 Virtual Biotech 执行的案例研究分析的正确性和可复现性,我们进行了人类专家评审。我们将两个案例研究中的每一个都拆分为四个独立的分析(共八个)。对于 B7-H3,这些分析对应于图 4 的 C 至 F 面板。对于 OSMR,它们对应于图 5 的 B 至 D 面板。我们招募了四位人类评审员,每位评审员被分配负责由 执行的两个分析。对于每项分析,评审员被要求通过编写自己的代码,按照虚拟 CSO 给 AI 科学家的相同指令执行分析。随后,他们被问到:“在亲自执行分析后,您的结论是否与 的结论基本一致?请添加笔记描述您的发现和思考过程。”

专家对所有八项分析均回答了“是”,确认其分析结果与智能体的发现一致。随后,专家审查了该分析对应的智能体编写的代码,并被问到:“ 编写的代码是否正确,且没有显著影响分析结论的错误?请添加笔记描述您的发现和思考过程。”评审员对所有八项分析均回答了“是”,并指出了一些在他们自己的分析中会采取不同处理方式的细微风格设计选择。这些差异并不影响发现和解释。专家笔记示例请参阅补充文本 VII, 与专家生成结果的并排对比请参阅图 S6 和 S7。这些结果证明了 的执行是准确的。

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与其他智能体系统的比较

为了将 的响应质量与类似的智能体系统进行比较,我们使用我们的案例研究(临床试验注释、B7-H3 和 OSMR)对 Biomni、Kosmos 和 PantheonOS (23–25) 这三个最先进的通用智能体系统进行了查询。对于临床试验注释,我们发现这三个系统产生的结果准确度较低

A

“正在分析 NCT06137183 试验方案和公布的结果。我将把此任务委派给临床试验专家智能体……”

“正在访问 ClinicalTrials.gov 记录。我看到这是一个已终止的 II 期试验,旨在测试 vixarelimab 在中至重度溃疡性结肠炎 (UC) 患者中的效果。

正在分析研究人群……”

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已终止

基于一项死亡率分析,该分析表明 Moonglow 研究不太可能达到其主要终点。

一项旨在评估 Vixarelimab 在中至重度溃疡性结肠炎 (UC) 患者中有效性、安全性和药代动力学的研究

ClinicalTrials.gov ID NCT06187183

“我找到了 TAURUS,一个关于 UC 患者接受阿达木单抗治疗的单细胞图谱。原研究作者发现,在接受阿达木单抗治疗后,仅在无反应者 (NRs) 的 3 种成纤维细胞状态中 OSMR 表达增加。”

我现在正在对细胞类型解析的 TF 活性进行评分,随后进行混合效应筛选……

我看到在 9 / 10 种基质细胞类型中,NR 治疗后组织中的 STAT1 活性升高。但是,OSMR 与其他 6 个受体共享 gp130 信号链。正在执行 Shapley 主导分解以量化冗余……

很有意思:尽管 是药物靶点,但在绝大多数基质细胞类型中, OSMR 对 STAT1 变异的解释程度低于 gp130、LIFR 或 IL27RA —— JAK-STAT 信号传导是通过其他受体驱动的。”

D

“我想知道 的上调本身是否仅限于 ?正在 CELLxGENE Census 中启动跨 112 种具有单细胞数据的疾病的 OSMR 表达分析。

该调查分析恢复了 OSMR 成纤维细胞和心肌中已确立的 OSMR 生物学特性。有趣的是,它提示 在急性肾损伤、毛细胞性星形细胞瘤、牙周炎和阿尔茨海默病中具有此前未被充分探索的作用——主要分布在成纤维细胞、内皮细胞或神经元细胞区室中。

表达的显著增加跨越了多种疾病,表明存在一种保守的炎症程序,对于 vixarelimab 在 OSMR 之外的治疗可能具有相关性。”

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入组标准

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描述

入组标准:

\+ 诊断为 至少 3 个月 + 中至重度活动性 (由 mMS 评估)+ 对常规或先进的 疗法反应不足、失去反应或不耐受

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排除标准:

\+ 诊断为克罗恩病或不确定性结肠炎

+ 疑似缺血性、放射性、微观或感染性结肠炎

  • 既往有结肠切除史

B

\- 对既往使用托法替尼 (tofacitinib)、乌帕替尼 (upadacitinib) 或其他全身性詹纳斯激酶 (JAK) 抑制剂治疗 UC 的反应不足或反应丧失

“NCT06137183 招募了一个治疗耐药的 UC 队列:患者此前对常规疗法和 / 或先进疗法(生物制剂和靶向小分子)反应不佳。他们也没有招募 JAK 抑制剂无反应者。”

“我想更好地了解该患者群体中治疗耐药的生物学机制……”

“如果信号冗余可能解释了为什么抗 OSMR mAb 失败,那么我假设 gp130 轴评分在预测无反应方面应优于单独的 OSMR。

我正在通过计算 gp130 轴基因治疗前表达量的平均值来构建一个 gp130 轴评分。在四个英夫利昔单抗 (infliximab) UC 临床试验数据集上进行测试以验证……”

图 5. Virtual Biotech 对终止的 2 期临床试验方案进行回顾性评估,从而优化了溃疡性结肠炎 (UC) 中 OSMRβ 靶向疗法的开发策略。(A) 研究 vixarelimab 的 2 期 UC 试验 (NCT06137183) 的代理总结。(B) TAURUS UC 图谱的单细胞信号分析。Shapley 主导分析分解了跨 gp130 家族 $\alpha$ 受体的 STAT1 活性,结果显示在大多数无反应者的基质细胞类型中, OSMR 并非驱动持续 STAT1 活性的主导受体。右侧面板显示了每种细胞类型中的 OSMR 检测比例,以及无反应者与

gp130 轴评分始终优于单独的 。来自单细胞分解的 Virtual Biotech 机制见解被验证为大块组织中更强的临床生物标志物。”

反应者治疗后组织中的 STAT1 活性富集情况,以及整体细胞状态丰度。(C) 在四个具有大块 RNA-seq 数据的 UC 患者队列中进行外部验证,使用 10 基因 gp130 轴评分来预测反应者与无反应者。其性能与单独的 OSMR 以及已发表的五基因炎症特征进行了比较。每个试验中每个评分的 AUC 已标注。(D) 跨疾病 表达分析。在 CELLxGENE Census 的 112 种疾病中查询每个捐赠者的伪大块 (pseudobulk) 表达,并通过线性混合效应模型(疾病对比匹配的正常组织)进行测试。热图显示了 OSMR 表达显著增加的疾病设置和细胞类型;黑点表示 FDR P < 0.05。

与 Virtual Biotech 相比,手动审查集和 TDC 标签上的注释(表 S2)。对于 B7-H3 和 ,我们使用与 Virtual Biotech 相同的初始提示词查询每个系统,并让它们进行开放式分析(表 S3 和 S4)。为了公平比较,我们为每个系统提供了与案例研究中 Virtual Biotech 类似的程度的人工引导:在每次分析后询问系统可能的后续步骤,并手动选择最有希望的步骤。为了可比性,我们选择了与案例研究中所做分析最一致的选项。总体而言,与 Virtual Biotech 相比,在两个案例研究中,这些其他代理系统使用的数据模态较少,分析严谨程度较低,且产生的具有生物学意义的结果较少(详见补充文本 VIII)。

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讨论

Virtual Biotech 是一个用于早期药物研发的多智能体平台。其核心是一个虚拟首席科学官(CSO),负责规划并协调多个领域特定的科学家智能体,这些智能体对原始数据源进行分析和推理。领域专业化的科学家智能体镜像了核心研发职能,并能够访问多种工具和数据源。这种协作设置允许基于对许多原始数据源的集体且细致的理解,做出统一的决策。

我们的实验表明,Virtual Biotech 能够对临床试验进行大规模分析,并识别出与临床试验成功相关的药物靶点的若干转录组特征。此外,针对真实世界药物开发场景的两项案例研究表明,Virtual Biotech 可以产生具有洞察力的假设,这些假设能够补充现代生物制药公司所达成的证据和结论。这项工作有助于围绕专家生物医学工作流构建的智能体 AI 系统的广泛出现 $(21)$。除了这些科学发现外,Virtual Biotech 还实现了集成跨领域推理、更具可审计性的循证决策以及可扩展的分析(详见补充文本 IX 的扩展讨论)。

Virtual Biotech 识别出的药物靶点单细胞转录组特征本身作为临床试验成功的预测指标,具有独立的研究价值。遗传证据被认为是临床成功最强有力的预测指标之一,并在现代靶点优先级排序中发挥着核心作用 $(39)$。此前的工作还表明,源自单细胞的信号包含有意义的临床信息,将这些特征与临床阶段的推进联系起来 $(56)$。在此基础上,我们证明了基于单细胞的特征不仅与阶段推进相关,还与成功的终点结果和降低的不良事件率相关。此外,我们表明单细胞证据与遗传证据是正交的,并且在没有支持性遗传证据的试验中,单细胞特征与试验结果之间的关联在统计学上仍然显著。这些发现共同表明,在药物开发计划中,将源自单细胞的证据与遗传支持相结合可能会提供重要的指导。

本研究存在局限性。Virtual Biotech 是一个用于早期人类治疗研究的决策支持系统,它能针对在遗传学、转录组学、功能基因组学、化学生物学和临床试验资源方面有深度覆盖且特征明确的人类疾病,全面地回答以靶点为中心的问题。相应地,对于罕见或研究不足的疾病、注释不足的靶点、代表性不足的组织或人群,以及缺乏信息化人类遗传或单细胞证据的问题,其结论较弱。目前的配置侧重于人类而非兽医,且针对病原体的传染病分析进一步受到模型提供商安全保障措施以及专用病原体和抗微生物资源短缺的限制。

值得注意的是,这些是当前数据和工具覆盖范围的边界,而非架构的边界:由于数据访问是通过模块化 MCP 接口介导的,因此可以在无需重新设计多智能体框架的情况下连接公共、专有或用户特定的资源,尽管每次扩展都需要其自身的策展、专业工具和评估(详见补充文本 IX 的扩展讨论)。

此外,我们的试验分析属于观察性分析,应据此进行解读。可能的混杂因素包括试验目标、适应症、终点定义以及与赞助商相关的影响。为此,我们对试验阶段、入组年份、治疗领域和药物模态进行了调整,以应对其潜在的混杂影响,并观察到了一个致的结果。分析范围还局限于在 ClinicalTrials.gov 数据库中注册的试验以及具有映射分子靶点的药物。对于案例研究,Virtual Biotech 生成了数据驱动的假设,这些假设必须经过测试和进一步验证。语言模型训练可能会使智能体倾向于现有假设,存在这种风险。为了减轻这一影响,我们特意选择了试验结果在语言模型 2025 年 1 月知识截止日期数月后才公布的案例研究。

最后,目前实现的 Virtual Biotech 涵盖了早期治疗药物开发中的计算分析、证据整合和优先级排序组件,而非生物技术组织的全部运作。实验测试仍在其范围之外。其模态评估反映了系统可用的数据资源,因此,缺乏已知结合剂或既定可药性应被解读为证据缺失和开发不确定性的来源,而非证明某种模态不可行。更广泛地说,智能体系统吞吐量和范围的增加,引发了关于假设优先级排序、溯源、独立验证、生物安全和科学培训的思考(详见补充文本 IX 的深入讨论)。

未来,我们设想扩展 Virtual Biotech 以涵盖更多药物研发管线,例如分子设计、虚拟筛选、毒性预测和临床决策智能体,将跨学科协作、速度和客观性的优势带到整个端到端流程中。Virtual Biotech 展示了从孤立的 AI 工具向能够在不同生物尺度和转化阶段进行推理的协调系统的转变。随着智能体平台的成熟,它们可能会实现一种科学组织模式,在这种模式中,假设被持续生成,针对异质证据进行压力测试,并在与人类专家的合作中得到完善。智能体系统并非取代科学家,而是可以在使推理过程更加透明和可重复的同时,扩大治疗假设探索的范围并提高其速度。

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材料与方法

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Virtual Biotech 系统架构

Virtual Biotech 是一个多智能体 AI 系统,其组织结构旨在模拟生物技术研发机构,以加速并支持治疗药物的开发与策略制定。该系统采用分层编排模型,由一名首席科学官(CSO)担任全局战略编排者,监督领域专业化的 AI 科学家智能体以及专门的研究支持智能体。

虚拟 CSO 智能体支持与用户进行多轮对话,解析查询请求,并将分析任务分派给相应的科学家智能体。 CSO 仅作为编排者运行:它负责路由查询、综合研究结果并提供战略建议,但绝不直接访问数据或执行分析。这种角色分离确保了领域专业知识被封装在科学家智能体内部,而 则维持对研究过程的全局视角。

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人类与 Virtual Biotech 的交互

Virtual Biotech 旨在实现轻量级的人机交互,其中用户的首要角色是设定意图,并通过高层级的科学问题或指令引导系统。在人类用户提交科学查询后, CSO 智能体会进行简短的澄清访谈——提出后续问题以就范围可行性达成一致——随后才启动计算分析(图 1℃)。目标明确后,后续操作均为自主完成: CSO 将任务分解并将子任务路由至科学家智能体,科学家智能体执行分析并对结果进行推理,最后由 CSO 将跨部门的结果综合为建议。与此设计一致,在本论文呈现的案例研究中,人类的参与仅限于 (i) 回应 的澄清提示,以及 (ii) 在每次迭代后提出后续问题(例如,探测假设、请求灵敏度检查或触发额外分析)。实验的构思、设计和执行仍由智能体驱动。用户可以通过检查并执行生成的代码来独立验证关键结果,从而实现人类监督。

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AI 科学家智能体

虚拟生物技术公司(Virtual Biotech)由一名虚拟首席科学官(CSO)智能体、分布在四个研究部门的八名不同科学家智能体,以及 CSO 办公室中负责监督科学方向和工作质量的两名额外智能体组成(图 1A)。每个智能体都配置了特定领域的系统提示词和 MCP 访问权限。

1) 靶点识别与优先级排序部门整合遗传因果关系、功能依赖性和细胞环境以验证靶点。统计遗传学智能体通过查询全基因组关联研究(GWAS)、用于因果基因分配的位点到基因(L2G)机器学习预测、精细映射的可信集、罕见变异负担元分析以及数量性状位点(QTL)共定位,来评估人类遗传证据,从而确定影响某个基因的遗传变异是否会影响疾病风险。功能基因组学与扰动智能体利用 CRISPR 敲除筛选和来自 Tahoe-100M 数据集的药物扰动转录组图谱,评估靶点的必要性和药理可开发性,以评价该靶点是否可以被调节。单细胞图谱智能体查询包含 1.43 亿 个协调单细胞图谱的 CELLxGENE Census,以学习细胞类型特异性的表达模式、疾病状态与健康状态之间的差异表达以及细胞间通信模式。

2) 靶点安全性部门整合通路推理、基于相互作用的影响、细胞类型特异性表达以及历史 FDA 监管安全性信号,以评估潜在的在靶和脱靶安全性问题。生物通路与蛋白质-蛋白质相互作用智能体通过通路和分子相互作用图对靶点的生物学背景进行推理,以识别在调节时可能引发安全性问题的关键细胞过程。单细胞图谱智能体通过检查 Tabula Sapiens v2 图谱中 27 种组织中发现的细胞类型特异性表达模式,对这种网络层级的评估进行补充,以识别关键细胞类型中潜在的脱靶毒性风险 (46)。FDA 安全官智能体利用来自 OpenFDA 的具有相似机制药物的不良事件报告、药物标签中的药物安全警告和黑框警告,以及小鼠敲除表型等经验性安全数据,对这些机制性评估进行补充,从而推理潜在的靶点级安全风险。

3) 模态选择部门利用结构生物学、可药性评估和临床先例,为验证后的靶点确定最佳治疗模态。靶点生物学家智能体评估限制模态选择的靶点属性,包括蛋白质家族分类、亚细胞定位以及结构可开发性预测,后者根据蛋白质结构和结合位点的可及性,评估开发小分子结合剂、治疗性抗体或其他模态类型的可能性。药理学家将此生物学评估与现有临床先例相结合,查询源自 ChEMBL 的药物数据库,以寻找共享相同靶点或机制的已批准疗法、管线化合物和化学探针。此外,他们分析同源蛋白以确定家族层级的可开发性,并评估每种模态的开发实用性,包括预计的时间表、制造需求和可能的障碍。

4) 临床官员部门通过分析监管安全数据并从先前的临床开发工作中提取见解,将临床前评估与临床先例衔接起来。临床试验员代理与 FDA 安全官员代理协同工作,通过临床先例分析来增强监管评估。它会定位针对同一基因或通路的先前试验;提取关于试验阶段、招募情况、终点和结果的信息,以确定临床验证的程度;并检查已终止的研究,以识别失败原因,包括无效性、安全顾虑或与业务相关的决策。对于肿瘤靶点,临床试验员代理可以访问临床基因组学数据,以从 cBioPortal 中确定跨肿瘤类型的预后生物标志物和生存结果。

5) 首席科学官(CSO)代理办公室:幕僚长通过盘点 MCP 工具并进行网络搜索,提供关于研究领域和数据格局的快速战略情报简报。科学评审员对 AI 科学家代理的输出进行质量保证,识别差距、缺乏支持的结论或与用户查询的不一致之处(补充文本 III)。

每个代理的系统提示词见补充文本 X。除幕僚长和科学评审员为了效率和速度而使用 Claude Haiku 4.5 外,所有呈现的代理均使用 Claude Sonnet 4.5 运行。科学家代理可以使用标准计算工具(包括文件操作和代码执行),以及以 MCP 服务器形式提供的领域特定数据访问工具(详见下文)。科学家代理被指示通过质疑假设、在互补数据集之间验证发现,并根据独立证据线的收敛情况将证据强度分类为弱或强,从而保持批判性的科学思维。

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实现与语言模型配置

智能体及其编排是使用 Claude Agent SDK 实现的,这是一个由 Anthropic 开发的用于构建 AI 平台的智能体开发框架 $(84)$。该 SDK 为多智能体科学工作流提供了多种能力:分层智能体编排(允许父智能体生成并协调具有独立执行上下文的子智能体)、与 MCP 服务器的原生集成以实现标准化的工具访问,以及对具有持久对话状态的多轮对话的内置支持。这些能力使虚拟生物技术公司(Virtual Biotech)能够实现复杂的委派模式,由首席科学官(CSO)编排者管理在保持对共享数据资源协调访问的同时自主运行的科学家智能体。智能体的行为通过结构化的系统提示词进行控制,这些提示词定义了角色身份与专业边界、可用工具与数据访问权限、分析工作流与决策框架,以及输出格式要求。我们在补充文本 II 中总结了虚拟生物技术公司的工作流算法。专门的科学工作流(如单细胞质量控制与分析)是以智能体技能(Skills)的形式实现的,并带有渐进式披露的工作流指南。

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数据与虚拟生物技术工具基础设施

虚拟生物技术(Virtual Biotech)整合了来自多个公共生物医学数据库的数据,以便在整个转化科学光谱和多个生物尺度上对药物靶点进行全面评估。Open Targets 平台(25.09 版本)作为主要的数据骨干 (33, 42)。这是一个广泛的数据库,能够对候选治疗药物靶点进行系统性的发现和评估。通过结合公开可用的数据集(包括由 Open Targets 实验和信息学研究项目产生的数据集),Open Targets 策划了支持治疗假设开发的数据。每个组件都提供了特定的证据类型,以及关于药物靶点、疾病、遗传变异、QTL 共定位、治疗化合物的作用机制、科学出版物、药物标签、FDA 报告的安全性信号、临床试验及其他相关数据的详细高分辨率信息 (33, 42)。

我们进一步将药物研发中的关键证据源等额外数据资源整合到虚拟生物技术中。单细胞图谱数据通过 MCP 工具访问和检索,这些工具利用 CELLxGENE Census API,该 API 汇总了来自 1000 多项已发表研究的协调单细胞 RNA 测序 (RNA-seq) 谱,提供了跨不同组织和疾病状态的标准化细胞类型注释 (59)。此外,我们为虚拟生物技术提供了一份 Tabula Sapiens v2 健康参考图谱的本地副本 (46)。伪批量(Pseudobulked)差异表达谱采购自 Tahoe-100M,这是一个十亿级规模的单细胞扰动图谱,涵盖了暴露于 1100 种小分子扰动的 50 个癌症细胞系 (34)。智能体对不同癌症队列中临床基因组学和结果数据的访问是通过由 cBioPortal REST API 驱动的 MCP 工具实现的 (85)。最后,临床试验信息通过利用 ClinicalTrials.gov API 的工具提供给智能体 (86)。

每个智能体的数据访问是通过 10 个 MCP 服务器介导的,每个服务器都实现为一个 FastMCP Python 实例,将特定领域的查询函数公开为可调用工具(图 1B 和补充文本 I)。MCP 在语言模型和外部数据源之间提供了一个标准化接口,支持带有类型参数和格式化响应的结构化查询 (29, 30)。每个 MCP 工具都实现为一个带有详尽文档字符串(docstrings)和类型参数签名的 Python 函数,FastMCP 会自动对其进行内省,以生成在运行时向语言模型公开的结构化工具模式,注入必要的上下文,使智能体能够在无需手动指定的情况下发现可用工具并理解其用途、所需输入和预期输出 (87)。工具不仅提供原始输出,还提供可解释的摘要和预览结果,允许智能体快速评估相关性并确定是否需要进行更深入的分析。这促进了跨不同数据源的高效多步推理和迭代工具调用。每个 MCP 服务器都提供针对频繁分析任务定制的专业工具。这些工具接受结构化输入(如基因符号、疾病标识符和各种过滤参数),并返回针对语言模型消费而优化的格式良好输出。虚拟生物技术的 MCP 工具在设计上具有可组合性,使智能体能够将多个工具调用链接在一起,以构建丰富且全面的证据概况。

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多智能体架构的优势

与单智能体方法相比,Virtual Biotech 的多智能体架构具有几个关键优势。Virtual Biotech 整合的数据源和分析工具规模极其庞大,涵盖数百种工具以及数 TB 的数据,涉及约 80,000 个靶点、4000 万 篇论文和超过 1 亿 份细胞图谱。由于上下文、时间和内存的限制,由单个智能体对这些资源进行深入分析是不可行的 (33, 34, 88)。相比之下,多智能体框架允许将这些分析分解并分布在具有独立上下文的并行智能体之间,使每个智能体能够进行彻底且专注的分析,而不会使共享上下文过载。随后,由一个协调智能体将这些智能体提供的高层摘要进行整合,以支持最终的决策。

其次,多智能体架构实现了大规模的并行工作流。例如,在提取临床试验结果时,每次提取都遵循一个多步骤工作流:给定一个输入 NCT ID,临床试验智能体首先调用 ClinicalTrials.gov API 以检索试验元数据,然后在进入三级证据级联之前,评估所有必需字段是否已充分填充。该级联过程包括使用 NCT ID 确认在 PubMed 中进行搜索,然后扩展到其他网络资源。在整个过程中,智能体审查大量信息源以理解试验设计、解读复杂的临床结果、确定终点结果、将终止原因映射到标准本体,并将所有证据整合到符合 Pydantic 模式的验证 JSON 输出中。因此,我们为每个试验分配了一个专用智能体,使其能够将完整的上下文窗口用于该项单一研究——从而深入熟悉其设计、结果和文献——而不会因为在一次对话中管理多个试验而产生干扰或导致上下文稀释。此外,这种设计实现了我们的多智能体并行化工作流,在 6 小时内系统地处理了 37,075 项 2 期和 3 期试验。相比之下,使用单个智能体处理相同数量的试验将需要约 1839 小时或 76.6 天的运行时间。因此,并行化多智能体架构实现了约 184 倍的加速,将原本需要数月之久的提取工作缩短为一次过夜运行。

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单细胞特征与临床试验结果分析

临床试验人工验证:我们从包含在智能体驱动策展过程中的 Open Targets 临床试验数据集中抽取了 100 项试验(从所有 2 期试验中随机抽取 50 项,从所有 3 期试验中随机抽取 50 项)。两名人类标注员评估了智能体在主要结果、次要结果和不良事件(AE)发生率方面的标注一致性。对于主要和次要终点,试验根据是否有足够证据支持阳性试验终点被分为两组。并非所有结果都适用于每项试验;例如,提前停止的试验不计入主要终点。对于每项试验,标注员首先审查 ClinicalTrials.gov 记录中公布的结果及任何相关出版物。如果没有可用结果,他们通过 NCT 标识符和试验名称在 Google 上搜索,以识别相关的摘要或报告。随后,标注员将这些来源与智能体提取的结果进行对比,在出现分歧时进行额外审查并记录分歧原因。两名人类标注员通过讨论模糊案例以达成共识。1 期试验未被审查,因为其成功在算法上被定义为进入 2 期。如果存在至少一项测试相同药物集且针对相同适应症、且试验开始日期在之后或同步的 2 期试验,则 1 期试验被分类为已进入 2 期。

在智能体标注与人工审查或 TDC 数据存在差异的试验中,差异仅限于本质上模糊的案例:具有多个实验组且部分组达到主要终点而其他组未达到的研究;主要终点未能达到常规统计学显著性(例如,$P = 0.06$)但具有支持性次要结果或长期结果的试验;以及无法清晰映射到简单的成功 / 失败二分结果的单臂或基于剂量的研究设计。这些边缘案例表明,将复杂的、多终点结果简化为离散类别存在本质上的模糊性,而非任何一种标注来源的系统性错误。

来自 Tabula Sapiens 的单细胞特征提取:单细胞表达特征源自 Tabula Sapiens 图谱,包含 27 种人体组织(膀胱、血液、骨髓、眼睛、脂肪、心脏、肾脏、大肠、肝脏、肺、淋巴结、乳腺、肌肉、胰腺、前列腺、唾液腺、皮肤、小肠、脾脏、胃、睾丸、胸腺、舌头、气管、子宫、血管和耳朵)。细胞类型标注基于图谱中提供的细胞本体(Cell Ontology)类别分配。对于每个目标基因,首先计算每个组织的特征,然后跨组织汇总,以获得每个基因的单个全局值。

细胞类型特异性:Tau 指数:细胞类型特异性使用 Tau 指数($\tau$)进行量化,该指数衡量基因表达被限制在特定细胞类型中的程度 (47)。对于在给定组织内的 n 种细胞类型中,在细胞类型 j 中平均表达量为 $\overline{x}_{j}$ 的基因:

$$

\tau_ {\mathrm{tissue}} = \frac {\sum_ {j = 1} ^ {n} \left(1 - \frac {\overline {{x}} _ {j}}{\ {{x}} _ {\max}}\right)}{n - 1}

$$

其中 $\{x}_{\max} = \max_{j} (\{x}_{j})$ 是该组织内所有细胞类型中的最大平均表达量。Tau 指数的范围从 0(普遍表达,在所有细胞类型中相等)到 1(完全特异性表达,仅在一种细胞类型中表达)。细胞数量少于 20 个的细胞类型被排除在 Tau 计算之外,平均表达量由对数归一化计数计算得出。对于给定的基因目标,Virtual Biotech 将所有组织的 Tau 指标汇总为该基因有表达的各组织 Tau 值的算术平均值。

表达异质性:双峰系数:群体内的表达异质性使用双峰系数(BC)进行评估,该系数用于检测是否存在截然不同的表达亚群(48, 49)。对于给定组织内 n 个表达细胞(表达量 > 0 的细胞)的基因表达向量:

$$

\mathrm{BC} _ {\mathrm{tissue}} = \frac {m _ {3} ^ {2} + 1}{m _ {4} + \frac {3 (n - 1) ^ {2}}{(n - 2) (n - 3)}}

$$

其中 $m_{3}$ 是样本偏度,$m_{4}$ 是皮尔逊峰度。双峰系数的范围从 0 到 1。计算中仅包含表达细胞,以专注于转录该基因的细胞之间的异质性。每个基因的全局双峰得分计算为各组织双峰系数的算术平均值。

单细胞图谱特征与试验结果的统计分析:我们对单细胞特征的统计分析采用了与遗传证据类似研究中的相同方法 $(39, 40)$。临床试验结果(阶段进展、试验终止、终点成功)通过单变量逻辑回归进行分析,以估计单细胞表达特征与结果概率之间的关联。在模型拟合之前,对特征进行 z-score 标准化,以便比较不同量纲的连续特征之间的效应量。模型参数通过最大似然法,使用具有二项分布族和 logit 链接的广义线性模型进行估计(statsmodels.GLM, Binomial family)。对于评估作用于多个分子靶点的药物的试验(因此每个试验产生多个 tau 和双峰特征),我们使用所有靶点中每个特征类型的最小值,因为单细胞代理假设特异性最低的靶点可能驱动整体安全性概况。对于患者层级计算的连续百分比结果(如按器官系统计算的不良事件率),我们使用了 R 语言 betareg 包 $(89)$ 中实现的 beta 回归。所得回归系数对应于预测变量增加一个标准差时,平均不良事件比例的 logit 值的变化。这些单变量分析是我们呈现的主要结果,与 Razuvayevskaya 等人 $(40)$ 和 Minikel 等人 $(39)$ 的方法一致。

除了这些结果外,我们还进行了鲁棒性分析以进一步支持我们的发现。首先,为了评估观察到的关联是否超过随机概率,我们对每个“特征-结果”组合进行了 1000 次迭代的排列检验。在每次迭代中,随机打乱结果向量,同时保留原始特征值,并重新拟合回归以获得零系数。经验双侧 P 值计算为绝对值大于或等于观察系数的零系数所占的比例。排列检验针对逻辑回归(二元结果)和 beta 回归(不良事件率)分析均运行了,且模型规范与主要分析完全相同。

接下来,为了考虑药物形式、治疗领域、试验开始年份和临床阶段可能带来的混杂影响,我们拟合了广义混合效应模型(GMMs)。对于二元结果,我们通过 R 中的 lme4::glmer 使用逻辑 GMM,并为药物类型组合和治疗领域组合设置交叉随机截距。对于不良事件率结果,我们通过 glmmTMB::glmmTMB 使用 beta 混合效应回归,采用 beta 分布族和相同的交叉随机效应结构。

为了评估单细胞表达特征是否提供了独立于遗传证据的额外信息,我们拟合了对遗传证据进行调整的双变量逻辑回归模型。对于不良事件结果,使用 R 语言的 betareg 拟合了类似的双变量 beta 回归。作为补充分析,我们将单变量分析重复应用于不含遗传证据的试验子集(75%)。参考 Razuvayevskaya 等人的方法,遗传证据被定义为一个二元指标,用于表示试验中任何“靶点-疾病”适应症对在 Open Targets 中是否有报道的直接遗传关联;Open Targets 汇总了来自全基因组关联研究(GWAS)、全表型组关联研究、基因负荷分析以及临床注释变异(ClinVar / EVA)的证据 (33, 40)。

为了对多重假设检验进行调整,我们使用了 Benjamini-Hochberg 程序将错误发现率(FDR)控制在 5% (90)。

为了实现可解释的量化,我们还通过对试验层级的分布进行 K-means 聚类 $(k=2)$,将连续的 tau 细胞类型特异性指数二值化为“细胞类型特异性”或“广泛表达”类别,并将阈值设定在两个聚类中心的中间点 $(\tau=0.69)$。

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单细胞和空间转录组学分析

质量控制与数据预处理:对原始单细胞或单核 RNA 测序计数矩阵进行质量控制过滤。保留表达基因数在 300 到 9000 之间且线粒体读取数 $\leq15\%$ 的细胞。为了减轻因采样不均导致的组成偏差,进行了供体级下采样(每个供体最多 10,000 个细胞),并按细胞类型分层以保持相对比例。使用 Scanpy (v1.9+) (91) 通过库大小归一化和 log1p 转换对基因表达进行归一化。选择高变基因 (3000) 用于下游的降维分析。

跨数据集的细胞类型注释使用细胞本体论 (Cell Ontology) (92) 统一为通用词汇表。通过分层本体遍历,将细粒度注释映射到标准化的 Level 3 本体类别。过滤出符合下游差异表达分析条件的细胞类型,要求每组条件中 $\geq3$ 个供体且每个供体 $\geq20$ 个细胞。

使用主成分分析(40 个主成分)进行降维。使用 Harmony (93) 纠正批次效应,在减轻数据集间技术差异的同时保留生物学变异。在经过 Harmony 纠正的主成分上计算均匀流形近似与投影 (UMAP) 嵌入以进行可视化。通过比较纠正前后的嵌入来评估批次混合情况。

伪体 (Pseudobulk) 差异表达:使用伪体方法进行差异表达分析。按供体和细胞类型聚合原始计数,并使用 PyDESeq2 (94) 测试差异表达。基因被定义为差异表达的条件为 FDR 调整后的 P 值 < 0.05 且 $\left / \log_{2}FC\right / > 1.0$。

细胞间通讯分析:使用 LIANA (60) 进行细胞间通讯推断,该工具计算多种配体-受体推断方法的共识得分。LIANA 的 rank\_aggregate 方法在两组之间运行了 1000 次置换。在 SCLC 中,第一组是按 B7-H3 表达量排名在前四分位数的成纤维细胞,第二组是排名在后四分位数的成纤维细胞。在 LUAD 中,B7-H3 表达量的前四分位数截止值不足以分离出 B7-H3 表达的成纤维细胞,因此第一组为 B7-H3 表达的成纤维细胞,第二组为非表达成纤维细胞。保留满足以下条件的相互作用:共表达量排名在前 $10\%$、CellPhoneDB 置换检验 $P < 0.01$,且由 $\geq 3$ 种组成方法支持。通过比较不同条件下满足上述标准的相互作用集来识别组特异性相互作用。

空间转录组数据的细胞类型反卷积:使用 NVIDIA H100 GPU (62) 上的 Cell2Location 对 10x Visium 空间转录组数据进行细胞类型反卷积。简而言之,这一已发表的工作流首先在 LUAD 单细胞图谱上训练负二项回归模型,以估计每种细胞类型的基因表达特征。随后将训练好的参考特征应用于空间数据,以推断每个点 (spot) 的细胞类型丰度,预期每个点的细胞密度为 8 个细胞。我们将目标基因 (B7-H3) 从该工作流中排除,以避免下游分析中的循环论证。参考模型训练了 250 个 epoch,空间映射模型训练了 10,000 个 epoch。细胞类型比例根据细胞丰度后验估计的前 5% 分位数计算得出。

空间免疫邻域分析:为了评估基因表达位点局部微环境中的免疫细胞组成,利用空间坐标为每个组织切片构建了k-最近邻图($k = 6$)(95)。在每个样本中,根据样本阈值将表达位点分为基因高表达组(前四分位数)和基因低表达组(后四分位数)。中间 50% 的位点被排除。表达位点少于 25 个的样本被舍弃。对于每个位点,计算其 k 个最近空间邻居中由 Cell2Location 估计的细胞类型丰度的平均值。为了在控制空间组织结构混杂因素的同时测试免疫耗竭情况,针对每种免疫细胞类型分别拟合了混合效应模型:

$$

\begin{array}{c} Y _ {i j k} \sim \beta_ {0} + \beta_ {1} \cdot \text {Gene} _ {\text {high}} + \beta_ {2} \cdot \ {UMI} _ {z} + \beta_ {3} \ \ {Fibroblast} _ {z} + \beta_ {4} \ \\ \ {Epithelial} _ {z} + \beta_ {5} \ \ {Endothelial} _ {z} + u _ {j} + v _ {j k} \end{array}

$$

其中 $Y_{ijk}$ 是样本 k 中嵌套于患者 j 的位点 i 的邻居平均免疫丰度;总 UMI 作为测序质量的代理指标,成纤维细胞、上皮细胞和内皮细胞的丰度(均在焦点位点测量)用于控制空间区室身份;$u_{j} \sim \mathcal{N}(0, \sigma_{u}^{2})$ 和 $v_{jk} \sim \mathcal{N}(0, \sigma_{v}^{2})$ 分别是患者级和样本级的随机截距,用于解释伪重复和切片间的差异。通过在递增的邻居环(邻居 7–15, 16–30)中重复分析来评估空间衰减。模型使用 lmerTest 通过限制最大似然法(REML)进行估计(96)。

生物标志物分层生存分析:为了评估 B7-H3 表达在肺腺癌(LUAD)中的预后意义,对通过 cBioPortal 访问的 TCGA PanCancer Atlas LUAD 队列进行了生存分析(63, 64)。检索了 566 名 LUAD 患者的基因表达谱和临床注释——包括诊断年龄、AJCC 病理肿瘤分期、性别和生存终点。分析仅限于具有完整的年龄、分期和性别协变量数据的患者。最终共有 477 名患者被用于分析。患者根据 B7-H3 (CD276) 的表达量被分为四个四分位数组,将前四分位数(高表达)与后四分位数(低表达)进行比较。针对总生存期(OS)、无进展生存期(PFS)、疾病特异性生存期(DSS)和无病生存期(DFS)拟合了多变量 Cox 比例风险模型,并对年龄(连续变量)、癌症分期 [晚期 (III / IV) 与早期 (I / II)] 和性别进行了调整。生存分析使用 lifelines Python 软件包完成。

转录因子活性推断:为了识别在治疗耐药性溃疡性结肠炎(UC)组织中活性持续改变的转录因子,从炎症性肠病抗 TNF(阿达木单抗)治疗的 TAURUS 纵向单细胞图谱中推断了 TF 活性评分 $74$。分析重点关注具有配对治疗前和治疗后结肠活检样本的 UC 患者($n = 20$;14 名无反应者,6 名反应者),排除了没有结局注释的患者。原始计数被标准化为每细胞 10,000 个计数并进行 log1p 转换。TF 活性使用 CollecTRI 调节子集 $75, 97$ 通过 decoupler 采用多元线性模型(MLM)进行评分,该模型对共享靶基因的 OSMR 进行联合评分,以正确划分共享的调节信号 $75$。

为了比较无反应者和反应者之间的 OSMR 活性,针对治疗后的细胞,为每个 和细胞类型拟合了线性混合效应模型:

\mathrm{TFactivity} _ {i j} \sim \beta_ {0} + \beta_ {1} \ \ { Remission\_status } _ {j} + u _ {j}

其中 $u_{j} \sim \mathcal{N}(0, \sigma_{u}^{2})$ 是样本级随机截距。模型通过 rpy2 使用 lmerTest (96) 进行拟合,并采用 Satterthwaite 自由度进行 P 值估计。P 值在每种细胞类型内部使用 Benjamini-Hochberg 程序进行校正 (90)。该筛选应用于 10 种表达 OSMR 的基质细胞类型中的 766 个 TF。

gp130 家族受体的 Shapley 方差分解分析:为了量化每个 gp130 家族 $\alpha$ 受体对下游转录因子活动的相对贡献,智能体使用了 Lindeman–Merenda–Gold (LMG) 方法 (98),该方法通过对所有可能的预测因子排序计算边际 $R^{2}$ 贡献的平均值,从而计算基于 Shapley 值的相对重要性份额。对于非响应者治疗后组织(定义为 OSMR 检测率 $\geq5\%$)中 10 种表达 的基质细胞类型,STAT1 活动通过单变量线性模型 (ULM) 进行评分,该模型使用了经过清理的 CollecTRI regulon,其中任何作为 regulon 靶点(IL6ST)出现的预测受体基因均已被移除,以防止循环论证 (75, 97)。每个样本和细胞类型的每个受体伪体 (pseudobulk) 平均表达量和 STAT1 ULM 平均活动量被计算出来(每个伪体组至少 10 个细胞)。结果(z 分数化的 STAT1 活动)被回归到 7 个 gp130 家族 $\alpha$ 受体(, IL6ST, LIFR, IL6R, IL11RA, IL27RA, CNTFR)上,并带有患者级随机截距:

$$

\mathrm {STAT1\_activity} _ {z} \sim \sum_ {r} \beta_ {r} \cdot \mathrm{Receptor} _ {r, z} + (1 / \text { Patient })

$$

其中所有预测因子在每种细胞类型内部均经过 z 分数化。LMG 份额通过穷举所有 $2^{7} = 128$ 个受体子集(每个子集在每种细胞类型中对应一个混合效应子模型),并使用 r.squaredGLMM 通过 MuMIn 提取每个子集的边际 $R^{2}$ 来计算 (99)。95% 置信区间通过集群自助法 (cluster bootstrap) 估计(在患者级进行 2000 次重采样),并使用普通最小二乘法以确保计算可行性。

大体队列中的 gp130 轴生物标志物评分验证:为了在独立患者队列中验证 gp130 冗余假设,从 Gene Expression Omnibus 获取了四个接受英夫利昔单抗治疗的 UC 临床试验队列的大体基因表达数据 (GSE12251, GSE16879, GSE23597, GSE73661)。当多个微阵列探针映射到同一个基因时,表达量被汇总为探针的平均值。gp130 轴综合评分被定义为 10 个基因(, IL6ST, LIFR, IL6R, IL11RA, IL6, IL11, OSM, LIF, STAT1)在队列内 z 分数化基线表达量的简单平均值,这些基因由智能体根据单细胞方差分解结果选择,未进行经验模型拟合。治疗非响应的预测性能通过接收者操作特征曲线下面积 (AUC) 进行评估,并与基线时的 OSMR 单独表达量以及 Arijs 等人建立的五个基因抗 TNF 响应特征 (IL13RA2, TNFRSF11B, STC1, PTGS2, IL11) 进行比较,后者使用相同的队列内 z 分数平均程序进行评分 (77)。

跨疾病 表达调查:为了确定基质 的上调是 UC 特有的还是反映了一种保守的炎症反应,我们查询了通过质量过滤的 112 种疾病的 CZ CELLxGENE Census (59)。对于每种疾病,每个供体的伪体表达量计算为 OSMR 基因的 $\log_{2}(\mathrm{CP10K}+1)$,仅包括每种细胞类型至少有 25 个细胞的供体。细胞类型使用 Cell Ontology 统一为 1 级类别 (92)。构建了疾病组和正常组织匹配的对照组,并根据研究和检测的重叠情况优先选择正常供体。差异表达使用加权线性混合效应模型进行测试:

\text { mean\_log2\_OSMR\_cp10k } \sim \beta_ {0} + \beta_ {1} \cdot \text { condition } +

$$

\beta_ {2} \cdot \log \_ d e p t h [ + \beta_ {3} \cdot a s s a y \_ g r o u p ] + (1 / d a t a s e t \_ i d)

$$

其中 condition 表示疾病组与正常组,log depth 用于控制残余的测序深度差异,assay group(在存在多种检测类型时包含)用于解释平台差异,而数据集层级的随机截距(1 / dataset_id)则用于解释研究的异质性。观测值的权重由贡献给每个伪体(pseudobulk)估计值的细胞数量决定。模型使用 lmerTest 结合 Satterthwaite 自由度进行拟合;当可用研究少于 2 项时,则改用普通加权线性模型 $96$。P 值在所有“疾病-细胞类型-基因”测试中进行了全局校正,将 FDR 控制在 5% $90$。

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致谢

作者感谢斯坦福大学 Zou 实验室的 S. He、S. Alber、W. Deng 以及其他成员对本工作提供的宝贵意见和有益讨论。资金支持:美国国立卫生研究院(NIH)(授予 H.G.Z. 的 T32-GM145402);Knight-Hennessy 奖学金(授予 H.G.Z.);美国国家科学基金会研究生研究员计划(授予 P.E. 的 DGE-2146755);斯坦福研究生奖学金(授予 P.E.)。作者贡献:H.G.Z. 和 J.Z. 构思并监督了本研究。H.G.Z. 开发、实施并优化了该框架。H.G.Z. 监督了案例研究的分析和可视化。A.B.M. 为案例研究提供了建议和指导。P.E. 设计了人类专家评估并对框架进行了基准测试。H.G.Z. 和 J.M. 设计了用户界面。H.G.Z.、P.E. 和 J.Z. 起草了手稿。所有作者对最终手稿进行了讨论、审阅和编辑。竞争利益:A.B.M. 是 PHD Biosciences 的员工。所有其他作者声明没有竞争利益。AI 使用声明:使用了一款 AI 编程工具(Claude Code)辅助代码生成和调试。所有 AI 生成的代码均由作者审阅并验证。数据、代码和材料可用性:Open Targets 平台的数据可直接访问 https: / platform.opentargets.org。CELLxGENE 数据可访问 https: / cellxgene.cziscience.com。Tabula Sapiens 数据集可访问 : / tabula-sapiens.sf.czbiohub.org / 。Visium 肺腺癌数据集可访问 : / pubmed.ncbi.nlm.nih.gov / 38782901 / 。TCGA PanCancer Atlas 肺腺癌队列通过 cBioPortal 访问(研究 ID luad\_tcga\_pan\_can\_atlas\_2018;: / www.cbioportal.org / study / summary?id=luad\_tcga\_pan\_can\_atlas\_2018)。分析的四项 UC 试验的微阵列数据可通过 GEO 登录 ID GSE12251、GSE16879、GSE23597 和 GSE73661 访问。TAURUS 数据集可访问 : / pubmed.ncbi.nlm.nih.gov / 39438660 / 。完整的案例研究文档,包括代码库、中间结果、智能体生成的报告、图表、Virtual Biotech 临床试验数据集和基准测试输出,可在 Zenodo (100) 获取。Virtual Biotech 的代码,包括可运行的命令行界面以及完整的系统提示词集和 MCP 服务器,可在以下地址找到:: / github.com / harrisongzhang / TheVirtualBiotech。本研究未产生新材料。许可信息:版权所有 © 2026 作者,保留部分权利;独家许可方为美国科学促进会(AAAS)。不对美国政府原始作品主张权利。: / www.science.org / about / science-licenses-journal-article-reuse

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补充材料

补充文本;图 S1 至 S7;表 S1 至 S4;MDAR 可重复性检查清单

2026 年 2 月 23 日提交;2026 年 5 月 25 日重新提交;2026 年 9 月 2 日接收;2026 年 9 月 17 日在线发表

10.1126 / science.aeg6779

用于糖尿病肥胖综合征无药管理的无线电催化闭环系统

Debasis Maity, Preetam Guha Ray, Peter Buchmann, Ghislaine Charpin-El Hamri, Martin Fussenegger\*

全文及作者所属机构列表:https: / doi.org / 10.1126 / science.ady8560

引言:2型糖尿病和肥胖经常共存(称为“糖尿病肥胖综合征”),影响着全球数十亿人。目前的治疗主要依赖于降低血糖或体重的药物,但这些疗法可能会产生副作用,需要终身给药,并且随着时间的推移可能会失去疗效。一种含有固体电催化剂的皮下植入物,能够以电可调的速度直接从血流中去除多余的葡萄糖,可以提供一种剂量可控、无药的治疗替代方案。

原理:电催化剂利用电能来加速化学反应。我们开发了一种植入式设备,其中包含嵌入在多孔石墨基质中的铂 (Pt) 修饰金 (Au) 纳米团簇。在无线供电时,ECHO(电催化闭环健康优化)设备选择性地将葡萄糖氧化为葡萄糖酸,这是一种能量较低的代谢产物,可很容易地通过肾脏清除。由于电刺激可以被精确控制,葡萄糖的清除速率也可以被精确调节。我们设计该植入物旨在恢复葡萄糖稳态,重塑能量代谢,并在与商业连续葡萄糖监测仪耦合时实现自主闭环控制。

结果:在生理相关条件下,该电催化剂选择性地将葡萄糖转化为葡萄糖酸,并在长期运行期间保持其活性。在患有糖尿病肥胖综合征的小鼠体内植入后,无线激活迅速将升高的血糖恢复到正常范围,重复治疗在 6 周内维持了血糖控制,且未检测到低血糖现象。

降低血糖使全身代谢转向利用储存的脂肪。接受治疗的小鼠表现出循环甘油三酯浓度和体重的降低,同时游离脂肪酸和酮体浓度增加。植入设备在 6 周的治疗期内保持功能,且治疗未产生可检测到的不良生理、炎症或行为影响。

将植入物与商业连续葡萄糖监测仪耦合实现了自主闭环运行。该系统仅在葡萄糖超过预设阈值时激活电催化剂,从而将葡萄糖维持在所需范围内。

结论:一种无线供电的电催化植入物在无需给药的情况下,直接去除了多余的血糖并促进了储存脂肪的利用。将植入物与连续葡萄糖监测相结合实现了自主闭环代谢控制,并证明了电催化作为一种无药管理糖尿病和肥胖的方法具有潜力。 □

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无线电催化控制

糖尿病肥胖综合征。ECHO 系统将连续葡萄糖监测与无线供电的电催化植入物相结合,后者将多余的葡萄糖氧化为葡萄糖酸以进行肾脏清除。在患有糖尿病肥胖综合征的小鼠中,自主闭环控制恢复了葡萄糖稳态,减轻了体重,并在不使用降糖药物的情况下促进了脂肪利用。[图表由 BioRender.com 创建。Maity, D. (2026) https: / BioRender.com / r5kl19g]

用于糖尿病肥胖综合征无药管理的无线电催化闭环系统

Debasis Maity $^{1}$ , Preetam Guha Ray $^{1}$ , Peter Buchmann $^{1}$ , Ghislaine Charpin-El Hamri $^{2}$ , Martin Fussenegger $^{1,3*}$

与生活方式相关的 2 型糖尿病及其相关的肥胖(糖尿病肥胖综合征,diabesity)影响全球 >25 亿美元 人,每年造成近 \$3 trillion 的医疗保健成本。我们开发了一种可植入的、无线供电的电催化闭环健康优化(ECHO)设备,该设备包含嵌入在石墨毡中的铂装饰金纳米团簇,能够实现血液葡萄糖向经肾脏清除的葡萄糖酸的选择性、电可调氧化。在 2 型糖尿病小鼠中,无线低功耗激活(0.75 volts, 10 milliamperes)在 1 小时内恢复了葡萄糖稳态,将代谢从葡萄糖利用转向脂质利用,减轻了体重并降低了甘油三酯,并增加了循环游离脂肪酸和酮体,且在 6 周的治疗期间未检测到低血糖或不良的生理、炎症或行为影响。将该 ECHO 设备与商业连续葡萄糖监测系统相结合,实现了对实验性糖尿病肥胖综合征的自主、智能手机控制且无药物的闭环管理。

糖尿病和肥胖是两种由遗传易感性增强的、相互关联的慢性生理生活方式疾病,与代谢能量稳态失调有关 (1–5),两者的结合被称为糖尿病肥胖综合征(diabesity)。肥胖与糖尿病之间的生理关系是双向且自我强化的,涉及代谢、激素和炎症变化的复杂相互作用 (1, 5–7)。特别是,碳水化合物触发的脂肪储存是糖尿病和肥胖发展与强化的核心驱动因素,从而形成一个恶性循环,推动了糖尿病肥胖综合征的流行,这影响了全球近 30% 的人口,且医疗保健成本高达全球国内生产总值 (GDP) 的 >1% (1–3, 5, 8–10)。由于促进糖尿病肥胖综合征的生活方式变化与福利和 GDP 增长相关,糖尿病肥胖综合征在全球范围内继续剧烈增加 (2, 3, 5, 10, 11)。

由于目前尚无治愈方法,且患者对建议的生活方式改变依从性较低,目前的糖尿病肥胖综合征策略集中在对糖尿病和肥胖进行终身药物管理 $(5, 11-13)$。鉴于手动开环干预的精度有限且缺乏实时动态给药,糖尿病管理仍然极具挑战性,导致葡萄糖代谢长期失调和持续的胰岛素给药,这可能会导致急性紧急情况和许多毁灭性的共病 $(14, 15)$。连续葡萄糖监测设备及其与胰岛素泵等药物递送系统的闭环集成极大地改善了实时血糖分析、精准胰岛素剂量和及时递送,但技术和机械问题,如传感器精度不足、传感器生物污染和信号漂移、可靠性差、缺乏个性化和灵活性有限,以及高成本和有限的可获得性,仍然是主要的限制因素 $(16-20)$。

这些挑战促使了基于设计细胞的先进概念验证疗法的开发 (21),这些细胞能够响应分子 (27–30) 或物理信号 (31–34) 来分泌调节血糖的蛋白质 (22–26)。这些细胞可以与实时原位分子血糖监测相结合,以实现闭环控制 (35, 36),这一概念在肥胖管理中也得到了探索 (31, 37–40)。例如,经工程化改造以感测食物摄入 (37) 或血脂水平 (39) 的细胞可以调节生物药物或饱腹感激素的产生,从而减少食物摄入,恢复代谢稳态,并维持健康的体重 (37–40)。尽管这些工程细胞具有前景,但包括致瘤性、免疫排斥和制造成本在内的多重障碍目前仍阻碍其临床实施 (41–44)。与此同时,

胰高血糖素样肽-1 (GLP-1) 和葡萄糖依赖性促胰岛素多肽 (GIP) 受体激动剂 [分别为司美格鲁肽 (45–47) 和替尔泊肽 (22, 23)] 已成为治疗糖尿病肥胖综合征的最新进展,通过同时解决糖尿病和肥胖问题 (48–52)。然而,高昂的成本、频繁的胃肠道不良反应,以及关于长期安全性(包括可能尚未显现的风险)的持续疑问,使得这些广泛使用的疗法在人群层面减轻糖尿病肥胖综合征负担的影响尚不确定。尽管取得了早期成功,但这些药物凸显了现代药物治疗面临的关键挑战:成本、剂量和副作用 (47, 48, 52–58)。以基于葡萄糖氧化酶的生物传感器为代表的酶催化葡萄糖氧化,是催化领域最成功的生物医学应用之一。然而,基于酶的系统可能会面临稳定性及运行寿命有限的问题,且植入会带来额外的挑战,限制了其在体内的长期使用。这些局限性促使了耐用非酶电催化方法的开发,旨在实现持续的、外部可调的闭环葡萄糖控制。

特别是电催化——在电极表面加速化学反应——近期在多个领域备受关注,例如可持续能源存储(制氢)(59, 60) 以及碳回收和升级回收($\mathrm{CO}_{2}$ 还原 (61, 62))。诸如 Pt-Ag 纳米团簇 (63)、Au 掺杂 $\mathrm{Co(OH)}_{2}$ 纳米颗粒 (64) 以及锚定在缺陷 $TiO_{2}$ 上的 Pt (65) 等电催化剂能够将葡萄糖氧化为高价值的葡萄糖酸,后者存在于水果、蜂蜜和葡萄酒中。此外,含有 Pt 和 Au 等贵金属的纳米颗粒电极结构能够紧密模拟葡萄糖氧化酶的活性并捕捉电能,从而应用于传感器和生物燃料电池 (35, 66–72)。这些进展强调了非酶电催化剂的前景,它们能为持续的葡萄糖调节提供更好的鲁棒性和可调性。先前的葡萄糖生物燃料电池研究证实,催化材料可以在体内氧化葡萄糖 (35),而经典的代谢研究表明,葡萄糖酸在全身暴露后大部分会被清除或代谢 (43)。然而,现有的非酶葡萄糖生物燃料电池持续氧化葡萄糖,无法实现外部可调的按需葡萄糖清除 (66–72)。

由于需要可控的葡萄糖清除,以及慢性药物治疗在耐受性、依从性和长期安全性方面存在的不确定性(5, 14, 15, 56, 73–80),我们开发了一种可植入、无线供电的电催化闭环健康优化(ECHO)设备。该设备包含一种复合电催化剂,由集成在石墨毡(GF)基质中的铂(Pt)修饰金(Au)纳米团簇组成(GF_Au@Pt)。这种 ECHO 设备能够在低输入功率下,将血糖特异性地、通过电调控氧化为可通过肾脏排出的葡萄糖酸。在一项针对患有 2 型糖尿病的肥胖小鼠的原理验证研究中, ECHO 植入物通过智能手机与商业连续葡萄糖监测(CGM)设备相连,在无需药物的情况下自动恢复了血糖稳态并转移了代谢能量平衡。

图 1 总结了 ECHO 系统的运行原理和代谢结果。该设备以闭环方式运行,用于检测高血糖并触发按需电催化。当 CGM 读数超过预设阈值时,智能手机启动向皮下植入物的无线功率传输,随后 GF_Au@Pt 催化剂将葡萄糖氧化为葡萄糖酸。这降低了循环葡萄糖水平并创建了一个受控的热量汇,将底物利用转向脂质分解。因此,脂肪分解增加,游离脂肪酸浓度升高,并促进肝脏酮体生成。通过在不使用外源性胰岛素的情况下将血糖维持在正常范围内,这种闭环策略将血糖控制与代谢转移相结合,从而能够对抗糖尿病肥胖综合征。

图 1. 用于糖尿病肥胖综合征电化学管理的闭环 -CGM 系统。(A) 植入式 系统调节葡萄糖的示意图。肠道吸收的饮食葡萄糖进入血液循环并由 CGM 监测。在高血糖状态下,皮下 植入物催化葡萄糖氧化为葡萄糖酸,从而降低循环葡萄糖。葡萄糖可用性的降低促进了脂肪分解,将甘油三酯转化为甘油和游离脂肪酸,后者进一步代谢为酮体并通过肾脏清除。(B) 结合 GF_Au@Pt 电催化剂的闭环 -CGM 系统的运行原理。当葡萄糖升高时(20 mM; ECHO 开启),CGM 反馈激活无线功率传输并驱动葡萄糖电催化转化为葡萄糖酸。在血糖正常时(10 mM; ECHO 关闭),无线控制器停止刺激以维持葡萄糖稳态水平。(C) 概念性治疗结果。受试者 A(治疗前)表现出葡萄糖和甘油三酯升高,而受试者 B(治疗后)在 ECHO 辅助治疗后显示出恢复的代谢平衡。[图表由 BioRender.com 创建。Maity, D. (2026) https: / BioRender.com / to7go11]

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结果

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GF_Au@Pt 电催化剂的开发与表征

利用 Pt 和 Au 分解葡萄糖的固有能力,我们合成了一种 GF_Au@ 异质电催化剂。首先在导电的高孔隙率 GF 上将 Au 纳米片(尺寸约为 150 nm)组装成球形 Au 纳米结构(尺寸约为 600 nm),然后用 点装饰这些 Au 纳米结构。我们通过在水热反应(24 小时,150℃;以及 1 小时,80℃)中使用还原剂 ($\mathrm{NaBH}_{4}$) 和络合剂(抗坏血酸),由 Au 和 GOR 盐进行化学沉积来构建该结构(图 2A)。

我们使用扫描电子显微镜 (SEM)(图 2, B 至 D)、低倍率能量色散光谱 (EDS) 映射(图 2, E 至 H)、高分辨率透射电子显微镜 (HR-TEM)(图 2I)和高倍率 EDS 映射(图 2, J 至 L)对 GF_Au@ 进行了广泛表征,这些结果确认了 GOR 装饰的 Au 纳米团簇的表面形貌(图 2, B 至 D)。Au 纳米片 (100 至 $200\mathrm{}$) 在 GF 的多孔结节框架上形成了球形结构 (500 至 $1000\mathrm{}$),为催化活性提供了充足的内部空间和巨大的表面积。在更高倍率下,球形 Au 团簇上可见 点 (<10 )(图 2I)。EDS 线扫描光谱显示碳 (C)、Au 和 GOR 的分布均匀,表明 Au@ 催化剂在 GF 上成功形成(图 2, E 至 H)。单个 Au 片(直径约 100 )的 HR-TEM 可视化和 EDS 元素映射确认了其被 GOR 点 (<10 ) 装饰(图 2, I 至 L)。Au 片提供了一个稳定、导电且高表面积的支架,支持 的沉积并促进电子传输。用纳米级 点装饰 Au 片可以在最大限度减少贵金属负载量的同时,集中高度活跃的表面基元。虽然单独的 Au 表现出有限的葡萄糖氧化活性,但 提供了主要的催化位点,两者结合,这种 Au 片 / 点架构相对于单独的 Au 显示出更高的催化效率、选择性和稳定性。

纯 GF 的高分辨率 C 1s X 射线光电子能谱 (XPS) 显示出对应于 $\mathfrak{sp}^2$ 杂化碳 (284.49 eV)、C-O 键 (285.97 eV) 和 O=C-O 基团 (289.56 ) 的特征峰,表明石墨烯框架上存在含氧官能团(图 S1A)。在引入 Au@ 纳米颗粒后,GF_Au@ 的 C 1s 能谱显示出占主导地位的 $\mathfrak{sp}^2$ 碳 (284.42 ),而含氧物种 (C-O 在 285.32 ) 的强度降低,表明在合成过程中发生了部分还原或表面改性(图 S1B)。GF_Au@ 的 Au 4f 能谱在 83.81 (Au $^{0}$ 4f $_{7 / 2}$ ) 和 87.52 (Au $^{0}$ 4f $_{5 / 2}$ ) 处显示出定义明确的双峰,确认了复合结构中存在金属金 (Au $^{0}$ )(图 2M)。 4f 能谱揭示了金属铂 ( $^{0}$ ) 和氧化铂 ( $^{2+}$ ) 物种的共存,其峰值分别归属于 $^{0}$ 4f $_{7 / 2}$ (71.13 ) 和 $^{0}$ 4f $_{5 / 2}$ (74.52 ),以及 $^{2+}$ 4f $_{7 / 2}$ (71.72 ) 和 $^{2+}$ 4f $_{5 / 2}$ (74.90 )(图 2N)。两种 氧化态的存在表明 纳米颗粒在合成过程中或之后发生了部分表面氧化。

GF_Au 和 GF_Au@ 葡萄糖氧化的电化学分析

我们首先在 21℃ 的碱性(1 M KOH)条件下,使用标准三电极装置评估了电催化葡萄糖氧化反应(GOR)。在存在和不存在 20 mM 葡萄糖的情况下,我们记录了 GF、金锚定 GF(\_Au)以及铂修饰金锚定 (\_Au@Pt)在 100 mV s $^{-1}$ 扫描速率下的线性扫描伏安法曲线(图 3A)。曲线证实,在 、\_Au 和 \_Au@Pt 存在时,在相对于 RHE(可逆氢电极)1.26 V 的电位下发生了析氧反应(OER),电流密度为 30 mA cm $^{-2}$。加入 20 mM 葡萄糖后,\_Au 和 \_Au@ 的 GOR 分别在相对于 RHE 0.7 和 0.6 V 的拐点电压处被记录到(纯 无拐点电压),这表明 在动力学上比 OER 更有利(图 3A)。值得注意的是,在没有电能且低于 0.6 V 拐点电压时,不发生 。在 0.75 V 时, GOR 的催化电流密度分别达到 25 mA cm $^{-2}$ (\_Au) 和

图 2. 石墨毡基底上金-铂纳米团簇的合成与分析。(A) 整合到石墨毡基质中、用作电控葡萄糖氧化电催化剂的铂修饰金纳米团簇的合成示意图。$C_{6}H_{8}O_{6}$,抗坏血酸;,石墨毡;\_Au,石墨毡整合金纳米团簇;\_Au@,石墨毡整合铂修饰金纳米团簇;HAuCl $_{4}$,氯金酸;H $_{2}$ PtCl $_{4}$,氯铂酸;NaBH $_{4}$,硼氢化钠;NaOH,氢氧化钠。[面板由 BioRender.com 创建。Maity, D. (2026) https: / BioRender.com / jwq27ew] (B 至 D) \_Au@ 在不同放大倍数下的扫描电子显微照片:2360× (B)、20,070× (C) 和 76,730× (D)。(E 至 H) \_Au@ 的 EDX 光谱映射图 (E),显示碳 (F)、金 (G) 和铂 (H) 的元素分布。(I 至 L) 单个 Au@ 纳米片在 600,000× (I) 和 200,000× (J) 放大倍数下的扫描透射电子显微照片,以及相应的 Au (K) 和 (L) 的 EDX 光谱映射图。(M 和 N) \_Au@ 的 XPS 光谱,显示 Au 4f (M) 和 4f (N) 区域,证实了表面组成和化学状态。a.u.,任意单位。

50 mA cm $^{-2}$ (\_Au@)。\_Au@ 的催化活性优于 \_Au,因为它在较低电压下(相对于 RHE 分别为 0.75 和 1.25 V)达到了更高的电流密度(50 mA cm $^{-2}$),证实了铂修饰在金纳米片上的协同效应以及 \_Au@ 对葡萄糖的高效氧化(图 3A)。Nyquist 图证实,由于葡萄糖吸附量更高,\_Au@ 显示出较低的电荷转移电阻,这与葡萄糖氧化速度快于 \_Au 的结果一致(图 3B)。、\_Au 和 \_Au@ 在非法拉第区域的双电层电容($C_{dl}$)值分别为 0.14, 0.27, 和 0.30 mF cm $^{-2}$(图 S1, C 至 F),证实了 \_Au@ 和 \_Au 具有比 更高的活性表面积。总体而言,\_Au@ 催化剂在各方面均优于 \_Au,并且在整个生理葡萄糖浓度范围内,葡萄糖水平与葡萄糖氧化之间存在直接相关性,且催化活性未出现饱和(图 3℃)。\_Au@ 在碱性电解质中表现出最大的 GOR 活性,同时在接近生理条件下仍保持相当的活性(图 S2)。

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基于 GF_Au@Pt 的葡萄糖氧化的性能分析与特异性

与通电 GF_Au@Pt 相关的电压下降表明反应从析氧反应(OER)转向了葡萄糖氧化反应(GOR),并且我们将葡萄糖酸鉴定为葡萄糖氧化的产物。液相色谱-质谱(LC-MS)和 ${}^{1}H-{}^{13}C$ 异核多键相关(HMBC)分析证实了葡萄糖向葡萄糖酸的选择性电化学氧化(葡萄糖 $\rightarrow$ 葡萄糖酸),支持在 ECHO 运行条件下具有较高的反应选择性(图 S3 和 S4)。这证实了基于 GF_Au@ 的葡萄糖氧化是通过以下双电子转移过程进行的:$C_{6}H_{12}O_{6}$(葡萄糖)+ 2 OH $^{-}$ $\rightarrow$ $C_{6}H_{12}O_{7}$(葡萄糖酸)+ H $_{2}$ O + 2e $^{-}$。当浸入 30 mM 葡萄糖溶液中的 GF_Au@ 在 0.75 V 和 10 mA 下通电时,葡萄糖浓度在 30 分钟内开始下降,并在 2 小时后达到 7 mM。与此同时,葡萄糖酸浓度增加至 12 mM(图 3D)。虽然葡萄糖氧化在这些体外条件下达到了稳态,但 GF_Au@ 的激活持续将葡萄糖转化为葡萄糖酸,证明了持续的电化学葡萄糖清除。在体内,约 90% 的葡萄糖酸通过肾脏清除,而较小一部分进入中间代谢。因此,我们假设 ECHO 介导的葡萄糖氧化将在降低循环葡萄糖的同时,移除其部分热量负荷 (35, 43, 81, 82)。

综合性能分析表明,电触发的 GF_Au@ 介导的葡萄糖氧化在各种条件下均具有鲁棒性,并且在测试范围内对葡萄糖浓度的依赖性很小(图 3E)。相比之下,葡萄糖氧化速率随之增加

A

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图 3. GF_Au@ 介导的电催化葡萄糖氧化。(A) GF、GF_Au 和 GF_Au@ 介导的葡萄糖氧化的线性扫描伏安法(20 mM 葡萄糖,1 M KOH,扫描速率 100 mV / s)。(B) GF、GF_Au 和 GF_Au@ 在葡萄糖(20 mM)氧化期间相对于 RHE 在 0.75 V 下记录的电化学阻抗谱。(C) GF_Au@ 催化剂的电流密度随葡萄糖浓度在 1 到 50 mM 范围内的变化。(D 至 G) GF_Au@ 介导的电催化葡萄糖氧化 [Dulbecco 磷酸盐缓冲盐水 (DPBS),10 ml,10 mA,0.75 V] 和葡萄糖酸产量对 (D) 电刺激时间、(E) 葡萄糖浓度 (DPBS, 10 ml, 10 , 0.75 V)、(F) GF_Au@ 电极表面积 (DPBS, 20 mM 葡萄糖, 10 , 10 , 1 小时, 0.75 V) 以及 (G) 样本体积 (DPBS, 10 , 2 小时, 0.75 V) 的依赖性。(H) GF_Au@ 介导的电催化葡萄糖氧化的可逆性(30 mM 葡萄糖,10 ,2 小时,0.75 V,10 ,1 cm $\times$ 1 cm 表面积)。(I) 在存在生理浓度指示代谢物的情况下,GF_Au@ 介导的电催化葡萄糖特异性的计时电流分析(0.75 V, 10 , PBS)。数据以平均值 $\pm$ SEM 表示($n = 5$ 个生物重复)。统计显著性使用双向方差分析 (ANOVA) 结合 Dunnett 多重比较检验确定。

GF_Au@Pt 工作区域(图 3F),并随着反应体积的增加而降低(图 3G)。此外,在长时间运行过程中,性能具有可逆性和稳定性(图 3H),这与 GF_Au@Pt 的材料完整性一致(图 S5)。

在所有考察的条件下,电触发的 GF_Au@Pt 激活仅氧化葡萄糖,而不针对其他糖类或代表性的电活性分子(图 3I)。线性扫描伏安法和电流分析表明,在测试条件下,GF_Au@Pt 对葡萄糖具有电化学特异性,因为在 5 到 10 倍生理浓度下测试的代谢物、蛋白质、激素、维生素和药物产生的电流响应可忽略不计,且未对葡萄糖氧化产生可测量的干扰(图 S6 和 S7)。

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GF_Au@Pt 介导的葡萄糖氧化的电可调性

在 2 型糖尿病中恢复血糖稳态以及通过重置代谢能量平衡来治疗肥胖,需要对电催化 GF_Au@Pt 的活性进行精确且动态的控制。为了全面分析 GF_Au@ 介导的电催化葡萄糖氧化的电可调性,我们将 GF_Au@ 浸入含有 $30~\mathrm{mM}$ 葡萄糖的生理盐水中,在固定电流下改变电压,同时分析葡萄糖清除动力学。GF_Au@ 介导的葡萄糖氧化的电化学起始(拐点)电压约为 0.6 V,而 0.75 V 被用作实现高效葡萄糖氧化的实际工作电压(图 3A)。随后,在激活阈值电压设定为 0.75 V 的情况下,我们记录了在改变电流时的葡萄糖氧化速率(图 3D)。结果证实,通过调节输入功率,可以将葡萄糖浓度精确调整至所需水平。在测试范围内,GF_Au@ 表现出浓度依赖性的葡萄糖氧化速率增加(图 S8)。总体而言,这些发现表明,GF_Au@ 介导的 GOR 可以通过调节 (i) GF_Au@ 的表面积、(ii) 工作时间以及 (iii) 电功率,根据需要进行微调和规模化,这表明该电催化剂可以灵活地适应不同的系统和条件。氯离子和活性氧(ROS)检测显示,在 ECHO 的 0.75 V 工作电位下没有检测到氧化剂的产生,这支持了非氧化工作窗口以及与细胞毒性测试结果一致的良好生物相容性(图 S9 和 S10)。

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GF_Au@ 介导的葡萄糖氧化的电催化闭环控制

在确定 GF_Au@ 介导的葡萄糖氧化可以通过电学调节后,我们接着探讨该反应是否可以与实时葡萄糖传感相结合,从而实现对葡萄糖清除的闭环控制。为了准备使用 GF_Au@ 介导的 GOR 对血糖进行动态闭环控制,我们首先在电催化剂运行期间通过定期添加葡萄糖来模拟餐后葡萄糖摄入。然后,为了模拟闭环控制,我们将电可调的 GF_Au@ 激活与来自商业 CGM 设备的葡萄糖水平输入数据相连接。在该系统中,CGM 实时检测模拟的餐后血糖峰值,并重复激活 GF_Au@ 电催化。该装置通过动态地开启和关闭电催化葡萄糖氧化,将葡萄糖维持在预设的 5 mM 目标值附近(图 S11)。

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构建用于可调葡萄糖氧化的无线供电 ECHO 植入物

为了实现无需药物的实时无线供电电调控血糖控制,我们将 GF_Au@Pt 电催化剂及相关的开关板电子元件组装在一个密封的 IPX7 认证防水(IEC 60529)3D 打印的美国食品药品监督管理局(FDA)许可聚酰胺外壳中 [26 mm $\times$ 14 mm $\times$ 5 mm,长 $\times$ 宽 $\times$ 高 (LWH)](图 S12)。ECHO 模块具有一个紧凑的、由聚酰胺封装的印刷电路板,可提供生物相容性的电绝缘(图 S12)。双层射频调节器可稳定无线功率传输(图 S13),而 13.56 MHz 发射器可实现高效的功率传输和同步激活,以进行闭环电催化(图 S14 和 S15)。开关板还包含一个接收线圈,用于同步来自体外电源发生器发射线圈的功率传输,其频率为 13.56 MHz 的工业、科学和医疗(ISM)频段。为了提高生物相容性,我们将含有 GF_Au@Pt 的生物电子植入物封装在一个三层结构中,该结构由 BioGlue 密封的聚纤维素袋和海藻酸盐涂层组成,且海藻酸盐层经过 EDC-NHS💡 [1-乙基-3-(3-二甲氨基丙基)碳二亚胺-N-羟基琥珀酰亚胺] 表面功能化处理。ECHO-CGM 系统将连续葡萄糖传感与无线电催化反馈相结合,通过闭环电化学控制实现自主的、具有生物相容性的葡萄糖调节(图 S16)。最终含有 GF_Au@Pt 的 ECHO 植入物在肥胖 2 型糖尿病 (db / db) 小鼠体内皮下植入 3 个月后,仍保持其电化学葡萄糖氧化活性(图 S17)。

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电催化血糖控制管理 2 型糖尿病及其相关肥胖

为了验证无药物电催化控制血糖浓度和糖尿病相关肥胖的效果,我们将 ECHO 设备植入 db / db 小鼠体内(图 S18),并测量了在 0 至 $0.9\mathrm{V}$ 应用电压(图 4A)以及 0 至 $10\mathrm{mA}$ 电流(图 4B)。我们发现,在 $0.75\{V}$ 和 $10\{mA}$ 下运行足以驱动高效的血糖氧化。在 $0.75\{V}$ 和 $10\{mA}$ 激活 ECHO 植入物后,在 60 至 $90\{min}$ 内可实现血糖正常(图 4℃),这与野生型 (WT) 小鼠的餐后血糖曲线(图 4D)相当,在糖耐量测试 (GTT) 中也观察到了同样的结果(图 4E)。这些结果表明,电催化葡萄糖清除可以在与 WT 小鼠生理性餐后血糖正常化相当的时间尺度上降低高血糖。在关闭电催化后,高血糖逐渐恢复(图 4D)。对不同时间段重复激活 控制的电催化葡萄糖氧化,证实了血糖控制的快速性和可逆性,表明 可以在实验性 2 型糖尿病中提供鲁棒、可重复且精确的血糖动态控制(图 4F)。在最佳刺激功率 $(0.75\{V}, 10\{mA})$ 和激活时间 $(60\{min / day})$ 下,高血糖波动可以被持续地减轻以达到血糖正常,并管理实验性 2 型糖尿病至少 6 周的时间(图 4, F 和 G)。血液 pH 值保持稳定且从未低于 7.35,表明碳酸氢盐缓冲系统 (37) 未受 触发的葡萄糖氧化产生的葡萄糖酸的影响,并提示不存在酮症酸中毒(图 S19)。电感耦合等离子体质谱 (ICP-MS) 和 SEM-EDX(能量色散 X 射线)分析支持 GF\_Au@Pt 电催化剂的化学和结构稳定性,在测试条件下,血清或器官组织中未检测到 Au 或 Pt(表 S1 和图 S20)。这些发现表明,海藻酸盐-聚纤维素封装有效地限制了全身金属暴露,同时也支持了 ECHO 系统的体内生物稳定性。

与侧重于单个细胞由胰岛素触发的葡萄糖摄取和代谢的经典血糖管理不同,基于 的葡萄糖电催化转化为经肾脏清除的葡萄糖酸会导致全身代谢能量的降低,这预计将有利于从基于葡萄糖的能量代谢转向基于脂肪的能量代谢,因此可能会减轻糖尿病相关肥胖。事实上,接受基于 的电催化葡萄糖氧化治疗 6 周的 db / db 小鼠不仅恢复了血糖正常,而且体重减轻了高达 10%(图 5A)。 ECHO 治疗的 2 型糖尿病 (T2D) 小鼠中胰岛素浓度的降低与血糖控制的改善一致,并可能反映了胰岛素敏感性的增强(图 5B)。此外,与未治疗的 T2D 和 WT 动物相比,这些动物表现出较低的血甘油三酯浓度(图 5℃)以及较高含量的游离脂肪酸(图 5D)和酮体(图 5, E 和 F),证实了电催化介导的从葡萄糖代谢向脂肪代谢的转变。值得注意的是, ECHO 的电催化剂保持完整,取出后的设备表现出原始性能(图 S17)。因此,电催化葡萄糖氧化可能为调节实验性糖尿病肥胖综合征中的高血糖和肥胖相关代谢特征提供一种无药物途径。在钳夹程序期间, ECHO 系统将葡萄糖维持在血糖正常范围内,支持了在测试条件下有效的控制且无低血糖证据。

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用于治疗糖尿病肥胖综合征的闭环电催化血糖氧化

与任何开环治疗干预一样,与开环无药电催化葡萄糖氧化相关的低血糖波动和过度的代谢能量耗尽无法被完全缓解。因此,我们通过将 ECHO 植入物与商业 CGM 设备接口连接,构建了一个动态闭环系统(图 S18)。该 CGM 设备实时监测组织间液葡萄糖浓度,并将数据无线传输至兼容的阅读器或智能手机,该设备经编程设定为:每当葡萄糖达到高血糖水平时,即无线激活 ECHO 植入物(图 6A 和视频 S1)。为了优化闭环控制动态并防止低血糖波动,我们在各种阈值葡萄糖浓度(5 至 15 mM 葡萄糖;图 6B)和 ECHO 激活周期(5 至 30 分钟;图 6℃)下,对闭环 - 通信和控制系统进行了分析。这一表征结果表明,闭环 - 系统可设置为上述范围内的任何葡萄糖阈值,且 5 分钟的短 激活周期足以提供稳定的葡萄糖稳态并防止低血糖波动(图 6℃ 和视频 S2)。在 ECHO 的许可使用寿命(12 天)内 (83–86),闭环 - 系统在植入 T2D 小鼠体内提供了自动、鲁棒且稳定的葡萄糖稳态(图 6D 和视频 S2)。细胞因子分析结合组织学和免疫组化分析显示,刺激组与未刺激的 T2D 队列在全身性炎症细胞因子或局部炎症细胞浸润方面没有显著差异,这证明在体内 30 天内,设备-组织界面保持了组织完整性并实现了受控的重塑(图 S21 至 S23)。

由电催化葡萄糖氧化驱动的葡萄糖消耗所导致的代谢能量损失,还诱导了向基于脂肪的能量代谢的转变,其特征为较低的血甘油三酯浓度(图 6E)、较高的血脂肪酸(图 6F)以及较高的酮体浓度(图 6, G 和 H),表明 刺激诱导了从基于葡萄糖代谢向基于脂肪代谢的转变。与此一致,高胰岛素-正常血糖钳夹研究显示,在受控的血糖条件下,经 治疗的糖尿病小鼠所需的葡萄糖输注率显著高于未刺激的糖尿病对照组(图 S24;P < 0.0001)。在测试的给药方案下,与药理学对照组相比, ECHO 电催化实现了快速降糖,且 曲线稳定,无低血糖过冲(图 S25)。该平台在 5 升规模的循环装置中进一步展示了可扩展且稳定的葡萄糖氧化,较大的 GF\_Au@Pt 电极增加了催化能力并实现了近乎完全的氧化。这些结果支持进一步的临床前开发,并证明了在与人体体积相关的灌注条件下可实现可扩展的葡萄糖氧化(图 S26)。

A

B

C

D

E

F

G

图 4. 实验性 2 型糖尿病中由 ECHO 控制的血糖水平。(A 和 B) 接受不同电压 (A) 和电流 (B) 刺激的植入 ECHO 的 T2D 小鼠的血糖概况。(C) 接受 0.75 V 和 10 mA 刺激的植入 - 的 T2D 小鼠 [T2D- (On)] 与 WT、未治疗的 T2D、未刺激的植入 - [WT+ (Off)] 以及未刺激的植入 - [T2D+ (Off)] 动物的血糖概况对比。(D) 对 T2D 小鼠使用 0.75 V 和 10 mA 进行不同时长重复刺激的 - 介导实时血糖控制。(E) 、T2D、+ (Off) 和 T2D+ (Off) 动物,以及植入 - 并接受刺激 (0.5 cm $^{2}$ , 0.75 V 和 10 mA) 的 T2D 小鼠的 GTTs。(F 和 G) 、T2D 以及每日接受一次 0.75 V 和 10 mA 刺激的植入 - T2D 小鼠的长期血糖概况。血糖水平分别在 7 天内每日监测 (F) 和 6 周内每周监测 (G)。误差棒代表平均值 ± SEM ($n = 8$ 个生物学重复)。统计显著性使用双向 ANOVA 及 Tukey 多重比较检验确定。

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以及电磁场 (116),已实现了对治疗性基因表达的远程控制 (31, 32, 117, 118)。电遗传学的最新进展还结合了材料科学,通过使用催化纳米复合材料来扩展反应空间。一个显著的例子包括一种代谢燃料电池,其中含有氧化亚铜的纳米复合材料持续催化血糖氧化,产生与血糖水平相关的直流电 (35, 108)。一个电子电源管理电路仅在高血糖期间抽取直流电,并通过光遗传学或直接方式电刺激共植入的设计细胞以产生并释放胰岛素,从而以闭环方式恢复正常血糖水平 (35, 108)。无线控制和信息交换由可穿戴设备和智能手机介导。然而,由于葡萄糖到直流电的转换是不可逆的,代谢燃料电池的纳米复合材料无法在反向模式下运行:即无法通过调节直流电输入来微调血糖浓度。

基于先前证明纳米复合材料可以将葡萄糖氧化与生物电子学相结合的工作 (35) 以及贵金属电催化剂设计的进展 (35, 119–121),我们为一种截然不同的目的设计了 GF_Au@Pt:外部供电、可逆且可调的葡萄糖氧化,而非持续的葡萄糖-电流转换。由此产生的电催化剂由高孔隙率的导电石墨毡组成,其中 Au 纳米片组装成球形纳米结构,并点缀有 Pt 点。由于其高比表面积,这种结构促进了高效的电子转移并增强了葡萄糖的可及性。花状的 Pt 点装饰 Au 框架促进了葡萄糖的吸附并改善了氧化动力学,使其整体反应性能优于传统的贵金属催化剂。这种分级结构在长时间运行中表现出极高的形貌稳定性、快速的电子转移动力学以及对葡萄糖的高特异性,并且它实现了可逆的

H

图 6. 使用与 ECHO 系统集成的商业连续葡萄糖监测设备,通过智能手机实现葡萄糖稳态的闭环控制。(A) 智能手机驱动的无线闭环 CGM-ECHO 集成系统控制 T2D 小鼠葡萄糖稳态的示意图。商业 CGM 实时连续监测葡萄糖水平,当葡萄糖水平升至预设阈值浓度以上时,启动对 ECHO 植入物的无线刺激。[该图由 BioRender.com 创建。Maity, D. (2026) https: / BioRender.com / Obj48wp] (B) 响应不同预设葡萄糖阈值浓度的葡萄糖稳态动力学。(C) 不同 刺激时间(0.5 cm $^{2}$ , 0.75 V, 10 mA)对植入 的 T2D 小鼠葡萄糖稳态动力学的影响。(D) 在 12 天的许可使用寿命期间,由集成闭环 - 设备控制的 T2D 小鼠葡萄糖稳态的自主维持。(E 至 H) - 治疗对肥胖的影响。甘油三酯 (E)、游离脂肪酸 (F)、乙酰乙酸 (G) 和 β-羟基丁酸 (H) 的浓度。动物组包括:均携带 的 WT 小鼠和 T2D 小鼠;配备闭环 - 系统但未进行刺激(Off)的 WT 小鼠和 T2D 小鼠;以及配备闭环 - 系统并进行刺激(On)的 T2D 小鼠。数据以平均值 ± SEM 表示($n = 8$ 个生物学重复)。统计显著性使用双因素方差分析(two-way ANOVA)结合 Dunnett 多重比较检验进行评估。

利用低电功率(小于或等于起搏器所需的功率),在生理范围内实现精确可调的葡萄糖氧化。最重要的是,GF\_Au@Pt 电催化剂表现出快速的电可调性,能够高效地恢复餐后血糖浓度,其动力学与在 WT 或接受胰岛素治疗的 T2D 小鼠中观察到的动力学相当,且未出现低血糖或相关的颤抖等行为。与天然生理状态或基于胰岛素的疗法(在激素触发细胞摄取葡萄糖后,身体的整体代谢能量水平保持不变)不同,电催化葡萄糖氧化产生葡萄糖酸,其中 90% 被肾脏迅速清除,导致整体系统代谢能量净减少 (35, 43, 81, 82)。值得注意的是,在此过程中我们未观察到与葡萄糖酸相关的酸中毒,表明身体的碳酸氢盐缓冲系统仍保持有效调节 (37)。这些结果表明,这种基于电催化葡萄糖酸降低净代谢能量的方法 (43, 81) 可以通过促进脂肪动员并防止进一步的脂肪积累,从而重置身体的整体代谢负荷。电催化调节血糖稳态还导致血清甘油三酯浓度降低、循环游离脂肪酸增加、酮体产生增加以及体重减轻——所有这些在食物摄入量没有检测到变化的情况下实现。这些效果与此前在针对饮食诱导肥胖管理的细胞级食欲抑制策略中观察到的结果高度一致 (39)。

在长期的糖尿病肥胖综合征(diabesity)管理过程中,该电催化植入物表现稳定,维持了其原始性能,且未出现明显的局部炎症或全身性炎症生物标志物的升高。此外,ECHO 的运行并未改变动物的进食习惯或整体行为,进一步证明了其在所测试的体内条件下的耐受性。特别是,进食行为未发生改变且未出现低血糖事件,突显了无药电催化葡萄糖调节的潜在优势,因为在这种实验设置中,它避免了全身接触降糖药物。这种无药的作用模式具有重要意义,因为目前治疗糖尿病肥胖综合征的药物疗法可能会受到副作用、耐受性、依从性、成本以及尚未解决的长期安全性问题的限制 (122)。

电催化 ECHO 设备可以与现代电子设备无缝集成,原则上可以连接到各种可穿戴设备、智能手机和基于云的物联网网络。这使得患者或医疗专业人员,或者通过能够预测日常习惯和生活方式变化的人工智能驱动算法,能够进行实时监测、在线诊断和治疗干预。作为概念验证,我们将植入 T2D 肥胖小鼠体内的 ECHO 设备与一套商业 CGM 系统进行了无线连接。CGM 系统追踪葡萄糖浓度并将数据传输至智能手机,智能手机处理数据后将指令发送回 ECHO 设备,后者随即迅速调整葡萄糖浓度以维持稳态——在无需小分子药物或生物制药且未出现低血糖事件的情况下实现了这一目标。 ECHO 许可应用的标准做法是每 12 天更换一次 (16, 83–86)。由于电催化剂在此时间尺度上没有被消耗或降解,且 ECHO 植入物显示出良好的局部组织兼容性,因此只要植入物的性能和组织兼容性在较长时间内保持稳定,配合常规的 ECHO 更换,实现更长期的无药葡萄糖和代谢能量平衡调节可能是可行的。我们认为,闭环电催化设备可以建立一个调节疾病相关代谢物的平台概念,为减少药物使用、动态控制的代谢干预提供一条潜在途径。

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材料与方法 化学试剂

氯铂酸 (H$_2$PtCl$_6$)、氯金酸 (HAuCl$_4$)、硼氢化钠 (NaBH$_4$)、抗坏血酸 (C$_6$H$_8$O$_6$)、葡萄糖 (C$_6$H$_{12}$O$_6$)、盐酸羟胺 (NH$_2$OH·HCl)、$N$-羟基琥珀酰亚胺 (NHS, C$_4$H$_5$NO$_3$)、磷酸盐缓冲生理盐水 (PBS)、$N,N'$-双(丙烯酰基)胱胺 (BAC)、聚纤维素、十二烷基硫酸钠 (SDS)、1-乙基-3-(3-二甲氨基丙基)碳二亚胺 (EDC)、2,2'-偶氮双(2-甲基丙酰胺)二盐酸盐 (AAPH) 以及牛血清白蛋白 (BSA) 均购自 Sigma-Aldrich。葡萄糖向葡萄糖酸的转化量使用比色 D-葡萄糖酸检测套件 (Sigma-Aldrich, MAK279) 进行定量。海藻酸盐购自 Buechi AG (目录号 11061528)。丙酮、炭黑、乙醇、氢氧化钾 (KOH) 和氢氧化钠 (NaOH) 来源于 ThermoFisher Scientific。铂 (Pt) 圆线 (直径 0.50 mm,密度 20.10 g / cm$^3$) 购自 Cooksongold,银墨 (目录号 186-3600) 购自 RS Components,石墨毡 (GF, 目录号 G100) 购自 Fuel Cell Store,BioGlue (目录号 BG3510-5-US) 购自 CryoLife Inc.。集成电路 (LT3092ETS8)、陶瓷电容器 (MC0402)、二极管 (Diodes Inc., 1N4148; ST Microelectronics, BAT54J) 以及电阻等其他小型电子元件购自 Digi-Key Inc.。

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电催化剂制备

石墨毡制备:将 GF 切成 5 cm $\times$ 5 cm 的正方形,用 70% (v / v) 乙醇清洗一次,在 21℃ 下干燥过夜,在 120℃ 的双蒸水 (ddH$_2$O) 中高压灭菌 24 小时以去除松散的纳米纤维并活化 表面,用 ddH$_2$O 洗涤,并在 40℃ 下真空干燥过夜。

\_Au 电催化剂的合成:通过将 10 ml HAuCl$_4$ 溶液 (10 mM) 与 10 ml NaOH 溶液 (0.1 M) 混合来合成金纳米团簇。混合物在 21℃ 下搅拌 30 分钟并超声处理 30 分钟 (82% 振幅, 20 kHz, 250 W, 5 s 开 / 关循环; Sonopuls HD4100, Bandelin Electronic GmbH),然后加入活化后的 ,随后加入 1 NaBH$_4$ (0.001 M) 和 1 抗坏血酸 (0.1 mM)。混合 5 分钟后,收集浸泡的 ,并在密封的水热高压灭菌反应器中于 150℃ 下孵育 24 小时,以完成 上片状金团簇的形成。随后将水热高压灭菌反应器在设定为 21℃ 的水浴中快速冷却——这对于维持锚定在 上的片状金团簇 (\_Au) 至关重要 (图 2℃)。收集 \_Au,用 70% (v / v) 乙醇洗涤五次,并在 50℃ 下真空干燥过夜。

\_Au@Pt 电催化剂的合成:为了在锚定于 的片状金团簇上装饰铂,我们将 \_Au 浸入 30 H$_2$PtCl$_6$ (1 mM) 中,并在 8000g 下离心 20 分钟。将 \_Au 转移至 40 抗坏血酸 (0.1 mM) 和 5 NaBH$_4$ (0.001 M) 的混合液中,在 100 rpm 的搅拌下于 80℃ 孵育 1 小时,用丙酮-ddH$_2$O 混合液 (1:10) 洗涤六次,并在 45℃ 下真空干燥 48 小时,从而获得铂装饰的片状金团簇锚定 ,即最终的 \_Au@Pt 电催化剂,准备将其放入无线供电的植入物中。

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ECHO设备

ECHO设备是按顺序组装的,包括无线供电电子元件、GF\_Au@Pt 插件以及生物相容性植入物的封装。电子元件:(i) 场发生器。我们构建了一个场发生器,用于无线供电并控制生物电子ECHO植入物。该场发生器的尺寸为 35.5 cm $\times$ 19.5 cm $\times$ 10 cm(长宽高),包含诸如使用振荡电路的频率发生器和放大晶体管输出信号的阻抗转换器等组件,这些组件驱动发射线圈的共振单元(13.56 MHz),并将电磁功率无线传输至ECHO植入物的接收线圈。(ii) 无线供电生物电子ECHO植入物。无线供电生物电子ECHO植入物外壳(26 mm $\$ 14 mm $\$ 5 ,长宽高)由3D打印(Formiga P110 3D打印机;德国Krailling,EOS GmbH)的FDA许可聚酰胺(德国Loerrach,Fabb-It 3D Druckservice)制成,其中包含接收线圈,该线圈在共振频率下收集功率发生器的电磁输出,并通过二极管将其整流为直流电。直流电激活ECHO的定制打印开关板(22 $\$ 8 $\$ 0.7 ),该开关板包含一个可编程的两端电流源(IC LT3092)用于调节设备运行,电容器(C4, C5)用于调整共振频率,电阻(R1)用于控制输出电流,以及二极管(D3, D4)用于控制阳极的输出电压,阳极中包含插入的GF\_Au@Pt电催化剂(0.5 cm $^{2}$ ),并用导电银墨水固定。为了防止任何短路,阳极和催化剂使用BioGlue进行绝缘。阴极由一根铂丝(直径 0.5 ,长度 10 )组成。电路图和电子元件列表见图 S12 至 S16 和表 S2。总体而言,根据国际保护标志标准(IEC 60529),ECHO设备的防水等级为 IPX7。(iii) ECHO植入物封装。为了提高其生物相容性,我们将ECHO植入物封装在由聚纤维素、海藻酸盐和用于表面功能化的 EDC-NHS 组成的三层结构中。我们首先将ECHO设备装入用BioGlue密封的聚纤维素膜袋中,然后将该袋浸入 0.2 (wt %) 海藻酸盐溶液中 6 小时(21℃),并在 0.1 M CaCl $_{2}$ 中浸泡 30 分钟以使其聚合,从而用海藻酸盐覆盖该袋。随后用 ddH $_{2}$ O 将覆盖海藻酸盐的ECHO袋清洗三次,并通过将其浸入含有 0.2 M EDC 和 0.05 M NHS 的 1:1 溶液中 2 小时,然后在 1 M Na $_{2}$ HPO $_{4}$ 中孵育 2 小时,最后用 ddH $_{2}$ O 清洗四次,从而对其表面进行 EDC-NHS 功能化。此过程重复三次。随后将 EDC-NHS-海藻酸盐ECHO袋浸入 0.1 M BSA 中 10 分钟,用 PBS 清洗一次,并进行 30 分钟的 UV 灭菌。最终的ECHO植入物(30 $\$ 17.5 $\$ 10 ,长宽高)在需要使用前存储于 4℃。

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GF\_Au@Pt 分析

使用扫描电子显微镜(SEM, FEI Versa 3D DualBeam)和扫描透射电子显微镜(STEM, JEOL JEM-F200 cFEG)分析 GF\_Au@Pt 的结构特性。使用 VG ESCALAB 210 系统(VG Scientific Ltd., East Grinstead, UK)进行 X 射线光电子能谱(XPS)分析。使用 FLIR E8 Pro(Teledyne FLIR LLC, USA)进行红外热成像。使用能量色散 X 射线光谱(EDS, Zeiss GeminiSEM 450)进行元素映射。使用选区电子衍射(SAED, JEM-F200(HRP))进行晶体结构表征。电化学分析,如循环伏安法(-0.2 至 0.2 V, 20 至 100 mV / s)、线性扫描伏安法(0 至 1.4 V, 100 mV / s)以及电化学阻抗谱(100 kHz 至 0.1 Hz, 100 mV 振幅),是在 CH Instruments 电化学工作站(CHI660)上完成的,使用

GF\_Au@Pt,以 RHE 为参比电极,铂为对电极,浸入 PBS(pH 7.4, 37℃ 和 1 M KOH, 21℃)中。GF\_Au@Pt 的电催化动力学记录是以 GF\_Au@Pt 为阳极、铂为阴极进行的。在电催化实验期间,使用 RND LAB 直流电源(型号:RND 320-KD3005D, 中国)提供稳定的直流电源。

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氯气测量

使用 DPD-1 测试条(目录号 486637)和 eXact EZ 光度计(目录号 486205)(ITS Europe)测量溶解氯。

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ROS 定量分析

电刺激的 DCINS 细胞用 PBS(300 $\mu$ l;目录号 14190-094, Thermo Fisher Scientific)洗涤,并在含有 25 $\mu$ mol liter $^{-1}$ 2',7'-二氯荧光素二乙酸酯(目录号 D6883, Sigma-Aldrich)的无血清 Dulbecco 改良 Eagle 培养基(DMEM; 500 $\mu$ l)中孵育 45 min (115)。细胞用 PBS(300 $\mu$ l)冲洗,并使用 Tecan Infinite 200 PRO 酶标仪通过荧光法(激发 / 发射,485 / 535 nm)对 ROS 水平进行定量分析。

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红外热成像

红外热成像(FLIR E8 Pro, Teledyne FLIR LLC, USA)检测到,在 10 ml DMEM 中以 0.75 V 和 10 mA 运行 $ 2 小时后,没有可测得的温度升高( $\pm0.1^{\circ}C$ )(图 S27)。

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分析表征

LC-MS 分析:LC-MS 测量在 Bruker Maxis 4G ESI-Q-TOF 质谱仪上进行,该仪器与高效液相色谱系统相连。分离采用 Reprospher 100 C18-Aqua 柱(2.0 mm $\times$ 125 mm,5 $\mu$ m),温度维持在 40℃。流动相由 (i) 含有 0.1% 甲酸的 H$_{2}$O 和 (ii) 含有 0.1% 甲酸的乙腈组成。梯度程序为:0 至 2 min,10% B;2 至 12 min,线性增加至 95% B;12 至 18 ,95% B;18 至 22 ,返回至 10% B。流速为 0.5 ml $^{-1}$,进样量为 1 $\mu$ l。质谱仪在正电喷雾电离 (ESI$^{+}$) 模式下运行,设置如下:毛细管电压 4500 V;雾化器压力 2.0 bar;干燥气 8 L $^{-1}$;干燥气温度 200℃;扫描范围,质荷比 75 至 700。数据使用 Bruker Compass DataAnalysis 进行处理。

核磁共振 (NMR) 光谱:NMR 光谱在 Varian 600 MHz 光谱仪($^{1}$H, 600 MHz; $^{13}$C, 151 MHz)上获取,采用梯度选择回波-反回波 HMBC 脉冲序列。D-葡萄糖在 ECHO 电池中于水相条件下电氧化 2 小时,随后将反应混合物重新溶解在 D$_{2}$O 中,在 298 K 下进行 NMR 分析。光谱采集的谱宽为 10 ppm ($^{1}$H) 和 220 ppm ($^{13}$C),使用 2048 $\times$ 512 个数据点,每次增量扫描 32 次。化学位移以残留 HDO ($\delta$ H = 4.79 ppm) 为参照。数据在 MestReNova (v14.2) 中处理,在傅里叶变换前进行正弦贝尔窗函数(sine-bell apodization)处理和零填充。

ICP-MS 分析:金 ($^{197}$Au) 和铂 ($^{195}$Pt) 使用 ICP-MS NexION 350D (PerkinElmer) 进行定量,该仪器在动力学能量判别 (KED) 模式下运行,并使用氦气作为碰撞气体。钇 [2 parts per billion (ppb)] 用作内标。外部校准采用 0.05 至 50 ppb 的标准品。检测限为 Au 0.005 ppb 和 Pt 0.010 ppb。血清样本 (0.75 ml) 使用 DigiPREP Jr. 加热模块在 100℃ 下用浓 HNO$_{3}$ (69%) 消解 55 。消解液用 Milli-Q 水稀释至 5 ml,然后在 ICP-MS 测量前在 2% HNO$_{3}$ 中进一步稀释 20 倍。

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动物实验

小鼠模型:本研究使用了两种小鼠模型:2型糖尿病(T2D)雄性 BKS(D)- $Lepr^{db}$ / JOrlRj 小鼠(6至12周龄,平均体重 $\sim$ 35至45 g,购自 Janvier Labs),雄性和雌性 BKS.Cg-Dock7m+ / +Lepr $^{db}$ J (db / db)(6至10周龄;德国 Charles River Laboratories),以及 WT 雄性和雌性 C57BL / 6JRJ WT 小鼠(6至12周龄,18至28 g,购自 Janvier Labs)。实验主要在雄性小鼠中进行,以减少与性别依赖性激素效应相关的变异性。对于图 S28 中所示的实验,在雌性 T2D 小鼠中评估了电刺激期间的血糖概况和葡萄糖耐量测试(GTTs)。其降糖效果与在雄性 T2D 小鼠中观察到的效果相当(图 4, C 和 E),且未检测到显著的性别依赖性差异。小鼠被安置在受控条件下,温度稳定( $21^{\circ} \pm 2^{\circ}\mathrm{C}$ ),环境适宜且湿度受控( $55 \pm 10\%$ )。它们维持在 12 小时的反向光暗周期中,并可不受限制地获取标准饲料和水。每个实验组由随机分配的小鼠组成( $n = 8$ )。

动物实验许可:所有实验程序均按照瑞士动物福利立法建立的伦理指南进行,并获得瑞士巴塞尔城市州兽医办公室(许可证号:2996\_34477 和 3341\_38467)以及法兰西共和国(项目号 DR2018-40v5 和 APAFIS 号 16753)的批准。实验由持有执照的研究人员在苏黎世联邦理工学院(ETH Zurich)和 / 或里昂大学技术大学研究所(Institut Universitaire de Technologie)进行:P.G.R(许可证号:LTK 5507)和 G. Charpin-El Hamri(许可证号:69266309)。

实验程序:为了准备手术干预,对小鼠的背部区域进行剃毛,并使用温和的乙醇和必达碘溶液对手术区域进行消毒。为了提供术前镇痛,在手术前于植入部位局部施用布比卡因 (0.25%) 和利多卡因 (0.5%) 的混合物。此外,在手术前 30 分钟皮下注射美洛昔康 (5 mg kg $^{-1}$ )。使用 4% 异氟烷诱导全身麻醉以确保小鼠完全麻醉,并在手术过程中使用 2% 异氟烷维持,使动物处于稳定的无意识状态,同时最大限度地减少麻醉相关并发症的可能性。ECHO 设备被手术植入皮下囊袋中,并使用临床批准的缝线 (110) 关闭切口。手术后,动物在进行 ECHO 刺激和血糖概况分析前稳定 24 小时。无线供电的 NMR 设备在 0.75 V 和 10 mA 下进行刺激,以确认催化剂与对照组相比的性能。然后,通过连续刺激 2 小时,将植入的 NMR 设备的电压 (0 至 0.9 V) 和电流 (0 至 10 mA) 参数标准化以进行血糖氧化。随后,使用优化后的电压 (0.75 V) 和电流 (10 mA) 来标准化刺激时间。为了实现闭环控制, NMR 设备通过无线方式连接到商业 CGM 系统 (FreeStyle Libre 3)(图 S16 和 S18 以及视频 S1)。连接 CGM 和 NMR 以实现生物电子闭环系统的电子电路如图 S16 所示。为了给动物配备该生物电子闭环系统, NMR 设备被植入在背侧,并且这个

随后是 24 小时的恢复期,之后在放置 CGM 设备之前,对小鼠的背腹侧区域进行剃毛和消毒。使用兼容的 CGM 阅读器(FreeStyle Libre 3 阅读器)进行连续的数据采集和监测。为了建立 和 ECHO 设备之间的闭环控制,我们对 NMR 阅读器进行了校准和编程,使其在组织间液葡萄糖处于 10 mM 或更高的高正常水平时产生振动。这些振动由一个振动传感器(SW-420 振动传感器模块;BerryBase.ch)捕捉,并通过一个 Arduino 控制器(由 ATmega328 驱动的 Arduino Nano A000005;DigiKey.ch)传递,以开启前述的电源生成器并激活 ECHO 植入物,刺激周期步长为 5 分钟,从而在没有低血糖风险的情况下安全地降低葡萄糖水平。在每个控制间隔之后,无线电频率生成器将根据连接到 阅读器振动单元的振动传感器的反馈而重新激活。建立这种无线振动通信接口是因为 NMR 的通信是私有的,无法进行开源修改。

葡萄糖耐量测试:小鼠在血糖测量前禁食 6 小时。在 GTT 中,小鼠接受葡萄糖腹腔注射(1.5 g / kg)。随后使用优化的电参数(0.75 V, 10 mA)对小鼠进行刺激,并使用 ContourNext 测试条和 ContourNext ONE 阅读器(Ascensia Diabetes Care;目录号 84191451 和 85659367)定期记录血糖曲线。对于长期分析,使用电功率(0.75V, 10 mA, 60 min)在指定间隔内刺激 ECHO 设备。刺激后测量血糖,并采集血样进行进一步分析。

血液采集与分析:血样采集于微量血清分离管(Becton Dickinson,目录号 365967)中,在 4℃ 下以 6000g 离心 10 分钟,并储存于 -80℃ 以备进一步分析。使用甘油三酯测定试剂盒(Abcam,目录号 b65336)、游离脂肪酸定量试剂盒(Sigma,目录号 MAK044)和酮体测定试剂盒(Sigma,目录号 MAK134)对血液代谢物进行分析。血清中的胰高血糖素(Mercodia,目录号 10-1271-01)和胰岛素(Mercodia,目录号 10-1249-01)使用相应的 ELISA 试剂盒进行测量。ECHO 设备的体内生物相容性通过使用相应的 ELISA 试剂盒定量分析炎症细胞因子干扰素- $\gamma$ (IFN- $\gamma$ )、白细胞介素-6 (IL-6) 和肿瘤坏死因子- $\alpha$ (TNF- $\alpha$ ) 的水平来评估 [IFN- $\gamma$ (目录号 BMS606-2), IL-6 (目录号 BMS603HS), 和 TNF- $\alpha$ (目录号 BMS607HS),均来自 Thermo Fisher Scientific]。在开环实验中,葡萄糖通过尾静脉血样测量。在闭环研究中,使用放置在植入物附近的 NMR 连续监测葡萄糖,并定期进行尾静脉采样以验证。与基于胰岛素的调节不同,ECHO 通过电极表面的直接电催化氧化来调节葡萄糖,该过程受血流和分子扩散等传输过程的控制。

树脂包埋与切片制备:样本由 Morphisto GmbH(德国美因河畔奥芬巴赫)根据协议 AF-086388 进行处理。标本用蒸馏水冲洗 1 小时以去除残留的固定剂,并使用 EXAKT 金刚石带锯(Model 312)进行切片。样本在室温下通过梯度乙醇(30% 至 99%)进行脱水,随后进行异丙醇处理和二甲苯透明化。预浸渍在 4℃ 下使用二甲苯与稳定 Technovit 9100 基础溶液(Kulzer / Morphisto GmbH)的 1:1 混合物进行,随后在添加了 Hardener I 的 Technovit 9100 中进行浸渍,最后在含有 Hardener I 和 PMMA 粉末的 Technovit 9100 中于 4℃ 下进行最终浸渍。样本被包埋在新鲜制备的 Technovit 9100 中,进行脱气(~200 mbar,10 分钟),密封以排除氧气,并在 $-4^{\circ}$ 至 $-8^{\circ}\mathrm{C}$ 下聚合 48 小时。聚合后的块状样本经过一夜脱气。研磨切片使用 EXAKT 切割、研磨和薄切技术(Donath 法),设备包括 Exakt Micro Grinder 400 CS、Diamond Band Saw 300 CP 和 402 Precision Adhesive Press。随后使用二甲苯和 2-甲氧基乙基乙酸对切片进行脱塑处理,用丙酮冲洗并重新水化。

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组织学染色与图像采集

ECHO设备切片:对重新水化的树脂包埋切片,使用Leica Multistainer ST5020自动染色系统或在$38^{\circ}$ C下使用Paragon染料进行手动苏木精-伊红(H&E)染色。切片经过脱水、用二甲苯透明处理,并使用基于二甲苯的CV Mount(Leica)封片。在$40^{\circ}$ C下干燥后,使用配备$20\times$物镜的ZEISS Axio Scan.Z1切片扫描仪在标准化采集设置下将切片数字化。

周围组织切片:包埋在石蜡块中的植入物周围组织样本使用Leica HistoCore AUTOCUT进行切片(厚度为5 $\mu$ m)(Leica Biosystems, Germany)。根据制造商的方案,使用苏木精-伊红(Roth; 目录号 9194.2)对切片进行染色。使用配备彩色摄像机的Nikon Eclipse Ti2显微镜采集染色组织的显微照片。

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免疫荧光分析

在指定终点采集ECHO设备周围的植入物周围组织,用4%多聚甲醛固定,进行石蜡包埋,并使用电动旋转微切片机(Leica HistoCore AUTOCUT, Leica Biosystems, Germany)切成5 $\mu$ m的切片。切片被贴在玻璃载玻片上,干燥,用二甲苯脱蜡,并通过梯度乙醇重新水化。使用EZ Retriever IR抗原修复系统(Biogenex; 目录号 MW015-IR),在10 mM柠檬酸盐缓冲液(pH 6.0)中进行热介导(95℃)的抗原修复。冷却后,用0.1% Triton X-100对切片进行通透化处理,并在室温下用5%正常山羊血清封闭1小时。切片在4℃下与稀释在封闭缓冲液中的兔原代抗体孵育过夜:抗CD68重组单克隆抗体(克隆 230504G10; Cat# 83014-5-RR; Thermo Fisher Scientific; 1:500)、抗TNF- $\alpha$ 多克隆抗体(Cat# BS-0078R; Thermo Fisher Scientific; 1:500)以及抗TGF- $\beta$ 1重组单克隆抗体(克隆 PD00-17; Cat# MA5-44667; Thermo Fisher Scientific; 1:500)。用PBS洗涤后,按照制造商的说明,将切片在室温下与Alexa Fluor 488偶联的山羊抗兔IgG (H+L) 交叉吸附二抗(Cat# A-11008; Thermo Fisher Scientific; 1:250)孵育1小时。使用配备彩色摄像机的Nikon Eclipse Ti2显微镜对染色样本进行成像。

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颈静脉插管与高胰岛素-正血糖钳夹实验

进行高胰岛素-正血糖钳夹实验以评估设备功效。对于导管植入,小鼠在异氟烷麻醉前接受美洛昔康(5 mg kg $^{-1}$,皮下注射)。暴露右颈静脉,并使用充满肝素盐水(50 U ml $^{-1}$)的PE-10导管(C20PU-MJV2814; Instech Laboratories, Inc., Plymouth Meeting, PA, USA)进行插管。导管向右心房推进,用丝线结扎固定,并通过皮下隧道从背侧退出,随后缝合切口。术后镇痛维持48小时。对于钳夹实验,小鼠禁食5至6小时,可自由饮水,并从尾静脉测量基础血糖。通过颈静脉导管给予胰岛素启动剂量(80 mU kg $^{-1}$),随后使用精密注射泵(Pump 11 Plus, Harvard Apparatus, Holliston, MA, USA)持续输注葡萄糖。每10 min测量一次血糖,并记录维持稳定血糖所需的葡萄糖输注率(GIR)。实验结束时,停止输注,用肝素盐水冲洗导管,动物被安乐死或在保暖条件下恢复。

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统计学

除非另有说明,所有呈现的数据均代表三次重复的两次独立实验。数据呈现的细节、生物学重复的样本量 $(n)$、统计分析以及显著性水平在图表或其相应的图注中提供。统计评估通过双向方差分析(two-way ANOVA)结合 Tukey 多重比较检验或 Dunnett 多重比较检验(如图注所述)来评估数据集之间差异的显著性。数据处理和分析使用 Microsoft Excel(版本 16.51)和 GraphPad Prism(版本 9.2.0)完成。

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致谢

我们感谢 H. Zulewski、A. P. Teixeira 和 A. Hierholzer 提供的慷慨建议。感谢 M. Pfeffer(巴塞尔大学化学系)进行的 LC-MS 分析,感谢 I. Cornu(巴塞尔大学)在 NMR 测量方面提供的协助,以及 N. Gasilova(洛桑联邦理工学院,ISIC-GE-VS, Sion)进行的 ICP-MS 分析。感谢 M.-D. Hussherr(苏黎世联邦理工学院 D-BSSE 动物设施)在执行颈静脉导管置入和手术操作方面的专业知识。资金支持:本工作得到了欧洲研究委员会高级资助(ElectroGene,编号 785800;M.F.)以及瑞士国家研究能力中心(NCCR)分子系统工程(M.F.)的部分资金支持。作者贡献:D.M. 和 M.F. 设计了该项目。D.M. 和 M.F. 分析了结果并撰写了手稿。D.M. 进行了体外工作,P.G.R. 和 G.C.-E.H. 执行了动物实验。D.M. 和 P.B. 设计了 ECHO 并制造了无线电源电路。利益冲突:作者声明没有竞争利益。数据、代码和材料可用性:支持本研究结果的所有数据均可在论文及其补充材料中获得。原始数据提供在数据 S1 中。本研究期间产生的材料,包括 GF\_Au@Pt 电催化剂和 ECHO 植入组件,可在合理要求下从通讯作者处获得。许可信息:版权 © 2026 作者,保留部分权利;独家许可方为美国科学促进会。对美国政府原始作品不主张权利。https: / www.science.org / about / science-licenses-journal-article-reuse。本研究全部或部分由欧洲研究委员会(785800)资助;根据要求,作者将根据 CC BY 公共版权许可提供作者接受的手稿(AAM)版本。

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补充材料

图 S1 至 S28;表 S1 和 S2;MDAR 可重复性检查清单;视频 S1 和 S2;数据 S1 提交日期 2025年5月8日;重新提交日期 2026年5月30日;接受日期 2026年8月31日

10.1126 / science.ady8560

BAK 和 BAX 形成多蛋白复合物以驱动 mtDNA 外流和 caspase 非依赖性细胞死亡

全文及作者所属机构列表:https: / doi.org / 10.1126 / science.aea2181

Shaoyuan Yang†, Hyungjin Kim†, Guanghong Liao, Na Ta, Ho-Chou Tu, Shriram Ramani, Chih-Yu Chen, Zih-Yu Li, Nobuhiro Tanno, James J. Hsieh, Emily H. Cheng\*

引言:线粒体在哺乳动物细胞死亡中起着关键作用。响应凋亡信号,激活型 BH3-only 蛋白激活 BAX 和 BAK,导致线粒体外膜通透化 (MOMP)、细胞色素 c 释放、凋亡小体组装以及 caspase 介导的细胞凋亡。在缺乏凋亡小体功能的细胞中, ECHO 和 ECHO 的激活反而会导致线粒体 DNA (mtDNA) 持续释放到细胞质中,激活 cGAS-STING-I 型干扰素信号传导,并引发 caspase 非依赖性细胞死亡。凋亡 caspase 级联反应通常会抑制这一先天免疫通路,使细胞凋亡在免疫学上保持沉默。鉴于凋亡小体功能受损在人类癌症中十分常见,- 激活诱导的 ECHO 外流和免疫原性细胞死亡可能为癌症治疗提供一条新途径。然而, ECHO 外流的分子和生化基础尚不明确。

基本原理:- 激活诱导的 ECHO 外流被认为与 MOMP 相关线粒体内膜 (MIM) 疝出有关。在细胞色素 c 外流后, ECHO 和 ECHO 聚集在线粒体外膜 (MOM) 形成大孔,MIM 通过这些大孔疝出并随后失去膜完整性,导致 外流。然而,只有少数疝出的 MIM 结构会失去膜完整性,这表明 外流可能还涉及一个主动的生化过程。因此,我们通过生化和遗传学研究来确定 和 ECHO 是否参与不同的蛋白复合物,从而差异化地调节细胞色素 c 和 ECHO 的外流。我们进一步在凋亡小体功能受损的人类癌细胞中研究了这一过程。

结果: ECHO 和 ECHO 在被激活型 BH3-only 蛋白激活后,组装成两个功能截然不同的线粒体复合物。负责细胞色素 c 释放的机制可能由 ECHO 或 ECHO 六聚体组成。相比之下,我们纯化了一个预先存在的 600-kD 复合物,该复合物由 、VDAC1、VDAC2、PHB1 和 PHB2 组成,可能定位于 MOM 和 MIM 之间的接触位点。BH3-only 蛋白的激活似乎会重塑该复合物,并促进细胞质 的招募以形成 释放机制,该机制直接从线粒体质体 (mitoplasts) 中释放 。这种重塑与 VDAC 通道关闭和线粒体钙离子内流增加相关。VDAC1、VDAC2 或 prohibitins 的缺失会损害 外流和 caspase 非依赖性细胞死亡,而不影响 MOMP 或 MIM 疝出。 ECHO 的耗竭也能保护细胞免于这种形式的死亡,支持了细胞质 对细胞死亡的贡献。我们将这种 - 激活诱导的 caspase 非依赖性细胞死亡命名为“baciptosis”。Baciptosis 表现出坏死形态,缺乏广泛的基因组 DNA 片段化,并伴随着

图解模型,阐明介导细胞色素 c 和 ECHO 外流的不同 - 复合物。激活型 BH3-only 蛋白激活 和 ECHO 以形成介导细胞色素 c 释放的六聚体复合物。与此同时,它们重塑一个包含 、VDAC1、VDAC2、PHB1 和 PHB2 的预先存在的 600-kD 复合物,并招募细胞质 以产生 释放机制。该模型突出了细胞色素 c 释放与 ECHO 外流在机制上的分离。

在细胞死亡前 ATP 浓度的逐渐下降。这些发现在凋亡小体缺陷的人类肾癌和肺癌细胞中得到了重复验证。

结论:我们的研究结果确定了与释放细胞色素 c 的 MOMP 机制不同的 mtDNA 释放机制。因此,mtDNA 外流并非简单的 MOMP 或 MIM 疝出的下游结果,而是涉及一个独特的、主动的生化过程。mtDNA 外流导致了 bacitosis,这是一种在凋亡小体功能受损时发生的、由 BAX-BAK 激活诱导的程序性坏死。这项工作为探索由 BAX-BAK 激活诱导的 bacitosis 作为凋亡小体缺陷癌症的潜在治疗途径提供了机制基础。□

细胞生物学

BAK 和 BAX 形成多蛋白复合物以驱动 mtDNA 外流和非 caspase 依赖性细胞死亡

Shaoyuan Yang $^{1\dagger}$ , Hyungjin Kim $^{2\dagger\ddagger}$ , Guanghong Liao $^{1}$ , Na Ta $^{1}$ , Ho-Chou Tu $^{1}$ , Shriram Ramani $^{1}$ , Chih-Yu Chen $^{1}$ , Zih-Yu Li $^{1}$ , Nobuhiro Tanno $^{1}$ , James J. Hsieh $^{2}$ , Emily H. Cheng $^{1,3,4*}$

凋亡调节因子 BAX 和 BAK 一旦被激活,会形成同源寡聚体以触发线粒体外膜通透化 (MOMP),从而激活凋亡小体和 caspase。在没有凋亡小体激活的情况下激活 - 会触发线粒体 DNA (mtDNA) 的持续外流和非 依赖性细胞死亡。然而, ECHO 外流的分子基础尚不清楚。我们纯化了一个由 、、激活剂 BH3-only 分子、电压依赖性阴离子通道 1 和 2 (VDAC1 和 VDAC2) 以及 prohibitins 组成的巨分子复合物,该复合物能使 从线粒体质体 (mitoplasts) 中释放。- 的激活导致 VDAC 关闭、线粒体钙离子内流和 ECHO 外流。VDAC1、VDAC2 或 prohibitins 的缺失可防止 - 激活诱导的 ECHO 外流和非 依赖性细胞死亡,且不影响 MOMP 或线粒体内膜疝出。这些发现支持了不同的 - 复合物对细胞色素 c 和 ECHO 外流的差异化调节。

线粒体在哺乳动物细胞死亡中起着关键作用。多种凋亡信号触发细胞色素 c 从线粒体膜间隙释放,使凋亡蛋白酶激活因子 1 (APAF1) 能够组装成七聚体凋亡小体并激活 $(1, 2)$。多结构域促凋亡蛋白 和 ECHO 使线粒体外膜 (MOM) 通透化,而抗凋亡蛋白 BCL-2、BCL-X $_{L}$ 和 MCL-1 则维持线粒体的完整性 $(3–5)$。BH3-only 分子 (BH3s) 整合上游凋亡信号,通过直接激活 和 ECHO 或使 -2、-X $_{L}$ 或 MCL-1 失活来促进凋亡 $(4–13)$。响应凋亡信号,激活剂 BH3s 直接结合 或 ECHO 以诱导其同源寡聚化,导致 MOM 通透化 (MOMP) $(4–13)$。-2 家族蛋白在正常生理和疾病过程中调节凋亡,并且是破坏蛋白质-蛋白质相互作用的抗癌药物的目标 $(14–16)$。

和 ECHO 的激活不仅触发 APAF1 介导的 ECHO 激活,还启动非 依赖性的线粒体功能障碍和细胞死亡 (4)。在缺乏 APAF1、-9 或 -3 和 -7 的细胞中激活 和 ECHO 会导致线粒体 DNA () 持续释放到细胞质中,从而激活 cGAS-STING 通路和 I 型干扰素 (IFN) 反应 (17, 18)。成像分析显示,细胞色素 $c$ 从 ECHO 或 ECHO 孔道中退出,这些孔道太小,无法通过超分辨率显微镜分辨 (19)。在细胞色素 $c$ 外流之后, ECHO 和 ECHO 聚集在 MOM 中形成大孔,线粒体内膜 (MIM) 通过这些大孔疝出,随后失去膜完整性,导致 外流 $(19)$。只有少数疝出的 MIM 失去膜完整性,且大多数与线粒体转录因子 A (TFAM) 结合的 ECHO 在此过程中仍留在线粒体内 $(19)$。在 ECHO 介导的凋亡过程中,由于 介导的快速杀伤, ECHO 外流在细胞死亡边缘瞬时发生 $(19)$。即使在凋亡过程中释放了少量 ,cGAS-STING-I 型 IFN 信号也会被 -3 介导的 cGAS 和 IRF3 切断而消除,使得凋亡在免疫学上保持沉默 $(17, 18, 20, 21)$。

由 BAX 或 BAK 激活诱导的 mtDNA 外流以及随后的免疫原性细胞死亡激活的发现,为癌症细胞死亡研究开辟了新途径,特别是考虑到凋亡小体功能受损在人类癌症中十分常见 $(22)$。然而,mtDNA 外流的分子和生化基础尚不清楚。具体而言,目前尚不明确 外流仅仅是 MOMP 及 MOMP 相关 MIM 疝出的结果,还是涉及尚未被识别的活性生化过程。此外, ECHO 的释放是否促成了非 caspase 依赖性细胞死亡也尚不清楚。鉴于神经元和心肌表达极少量的 APAF1 $(23, 24)$, ECHO 外流可能促成了与神经元和心肌细胞死亡相关的疾病的发病机制。我们利用生化和遗传学研究,鉴定并表征了一个与 BAK 和 BAX 相关的大分子复合物,该复合物在包括凋亡小体缺陷的人类癌细胞在内的多种细胞类型中,调节 外流和非 caspase 依赖性细胞死亡。

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结果

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鉴定一个 600-kD 的 BAK 相关大分子复合物

为了确定 BAK 是否通过参与不同的蛋白质复合物来调节细胞色素 c 和 mtDNA 的外流,$Bax^{- / -}^{- / -}$ 小鼠胚胎成纤维细胞 (MEFs) 被重新构建,引入 N 端蛋白 C 标签的 ,以方便对 相关复合物进行亲和纯化。我们关注 是因为它是线粒体外膜 (MOM) 的整合蛋白,而 BAX 在凋亡时从细胞质易位至线粒体 (8, 25)。为了增强对去污剂耐受的 及其相关整合膜蛋白的提取,线粒体先后使用 1% 和 2% 的 3-[(3-胆酰丙基)二甲胺基]-1-丙烷磺酸 (CHAPS) 去污剂进行提取。将 1% CHAPS 不溶且 2% CHAPS 可溶的亚组分进行抗蛋白 C 亲和色谱分析,随后进行银染和串联质谱分析。电压依赖性阴离子通道 1-3 (VDAC1-3) 异构体、腺嘌呤核苷酸转运蛋白 1 (ANT1) 和 prohibitin 2 (PHB2) 与 以近 1:1 的化学计量比共纯化 (图 1A 和表 S1)。这些蛋白质的身份通过免疫印迹得到了进一步验证 (图 1B)。线粒体基质蛋白 cyclophilin D(线粒体通透性转换孔复合物 (mPTP) 的关键调节因子 (26))和线粒体内膜 (MIM) 蛋白 ATP 合成酶 $\beta$ 作为阴性对照。 与定位于 MOM (VDAC1-3) 和 MIM (ANT1 和 PHB2) 的蛋白质相结合,表明这些组分可能在 MOM 和 MIM 的接触位点组装成一个复合物。事实上,在不连续蔗糖梯度上对线粒体亚囊泡进行分级显示,、VDAC1、VDAC2、ANT1 和 PHB2 在 MOM-MIM 接触位点具有重叠的定位 (图 1℃)。

为了进一步表征该复合物,我们对 2% CHAPS 可溶的线粒体亚组分进行了凝胶过滤色谱分析。、VDACs、ANT1 和 PHB2 在 600 kD 左右的高分子量组分中洗脱,这与这些蛋白质形成一个 600-kD 复合物的结果一致。在这些组分中未发现 Cyclophilin D、细胞色素 c 氧化酶亚单位 IV (COX IV) 和 ATP 合成酶 $\beta$,支持了该复合物的特异性 (图 1D)。为了进一步确认这些蛋白质形成了 600-kD 复合物,从凝胶过滤色谱中收集高分子量组分,并使用抗蛋白 C 抗体进行免疫沉淀。所得的银染凝胶显示出与图 1A 中未经过尺寸分级所得的模式相似 (图 1E),其身份通过免疫印迹得到了进一步确认 (图 1F)。这个 600-kD 复合物似乎存在于健康细胞中,将其与仅在被 BH3s 激活后才被检测到的寡聚化 区分开来 (8, 10)。

A

D

c

B

G

E

F

H

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图 1. BAK 存在于三种具有不同死亡调节活性的蛋白复合物中。(A) 使用 1% 和 2% CHAPS 对 $\pm$ 蛋白 C (PrC) 标签 BAK 的 $Bax^{- / -}^{- / -}$ MEFs 线粒体进行顺序提取。通过抗 PrC 亲和层析纯化 2% CHAPS 可溶亚组分,并进行银染。切下条带进行胰蛋白酶消化和液相色谱-串联质谱分析。(B) 对 $\pm$ 标签 的 $Bax^{- / -}^{- / -}$ MEFs 进行抗 免疫沉淀和免疫印迹分析。(C) 对 WT 线粒体进行低渗溶胀和超声处理,在不连续蔗糖梯度上分级为 MOM、MIM 和接触位点 (CS) 分级,并通过免疫印迹分析。FIS1 为 MOM 的标记。(D) 使用 Superdex 200 (HR 10 / 30) 凝胶过滤和免疫印迹分析 WT 的 2% 可溶线粒体亚组分。蛋白标准品表示以千道尔顿为单位的表观分子量。(E 和 F) 对 $\pm$ 标签 的 $Bax^{- / -}^{- / -}$ 的 2% 可溶线粒体亚组分进行凝胶过滤。通过抗 亲和层析纯化 600 kD 左右的分级,并通过银染 (E) 或免疫印迹 (F) 进行分析。(G) 使用 1% 和 2% 对 $\pm$ 重组 tBID 的 WT 线粒体进行顺序提取,并通过凝胶过滤色谱和免疫印迹分析。对照抗 免疫印迹 (2% 可溶) 与 (D) 中的相同。(H) 对 $\pm$ 标签 的 $Bax^{- / -}^{- / -}$ 的 1% 可溶线粒体亚组分进行凝胶过滤。通过抗 亲和层析纯化 160 kD 左右的分级,并进行银染。(I 和 J)

对 WT 的 2% 可溶线粒体亚组分进行凝胶过滤。对 tBID 处理前的 60-kD 分级以及 tBID 处理后的 160- 和 600-kD 分级进行 BMH 交联 (I),或与 $Bax^{- / -}^{- / -}$ 线粒体共同孵育,通过 ELISA 评估细胞色素 c 的释放 (J)。数据以平均值 $\pm$ 标准差 (SD) 表示($n = 3$ 次独立实验)。\*\*\*P < 0.001 (Student's t 检验)。

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BAK 存在于三种具有不同死亡调节活性的蛋白复合物中

为了研究不同 BAK 相关复合物的存在,研究人员对野生型 (WT) MEF 线粒体在体外用重组截短 BID 蛋白 (tBID) 诱导 激活前后的 1% 或 2% CHAPS 可溶亚组分进行了凝胶过滤色谱分析 (Superdex 200 HR 10 / 30)。 BAK 在三种不同的复合物中洗脱 (图 1G)。在 1% 和 2% CHAPS 可溶亚组分中, BAK 在 tBID 处理前在 60 kD 处洗脱,并在 BAK 处理后转移至 160 kD (图 1G)。我们推论,160- 复合物可能代表由 BAK 诱导的寡聚化 ,用以介导细胞色素 c 的释放,而 60- 复合物可能包含失活的 。在 BAK 处理前后, BAK 均从 2% 可溶亚组分中在 600 附近洗脱 (图 1G)。600- 复合物在 1% 可溶亚组分中的含量较低,这与其在 1% 中的较低溶解度一致。重组 蛋白主要与 600- 复合物一同洗脱 (图 1G)。

为了进一步评估 160- 复合物,对 160- 凝胶过滤组分进行了抗蛋白 C 亲和色谱分析。未检测到与 BAK 结合的明显蛋白 (图 1H)。因此,160- 复合物可能代表一个由六个 25- 单体组成的 BAK 六聚体。为了评估不同 复合物的功能意义,对 60-、160- 和 600- 组分进行了蛋白交联和细胞色素 c 释放实验。只有存在于 160- 组分中的 BAK 能被双马来酰亚胺己烷 (BMH) 交联剂交联成二聚体和三聚体 (图 1I),并能从 $Bax^{- / -}^{- / -}$ 线粒体中释放细胞色素 c (图 1J)。这些数据表明,600- 复合物在功能上与促进细胞色素 c 释放的 160- 复合物截然不同 (图 1J)。

我们接下来研究了在 $Apaf1^{- / -}$ MEFs 中通过多西环素诱导 表达后, BAK 是否形成相同的复合物。该系统能够分析 诱导的 mtDNA 外流。它还允许我们确定 BAX 是否形成了不同的复合物,以及在 BAK 表达后是否被招募到 600- 复合物中,因为在健康细胞中,大多数 BAX 不存在于线粒体中 (图 1G)。对 BAK 诱导前或诱导 6 小时后的 BAK 可诱导 $Apaf1^{- / -}$ MEFs 的 2% 可溶线粒体亚组分进行了凝胶过滤色谱分析。使用不同的 Superdex 200 (10 / 300 GL) 柱, BAK 在 BAK 诱导后同样从 60- 转移至 160- 组分,并且无论 是否表达,均一致地与 VDAC1、VDAC2、ANT1 和 PHB2 在约 600 的表观尺寸处一同洗脱 (图 2A)。与凋亡过程中从细胞质易位至线粒体一致,线粒体 [ ] 在 BAK 表达后增加,并从主要为 40 转移至 140 和 600 (图 2A)。这些发现表明,一旦被 BAK 激活,[ ] 就会被招募到 600- 复合物中。[ ] 在 BAK 缺失的细胞中, BAK 积累后仍然形成 140- 和 600- 复合物 (图 S1A),表明这些 [ ] 相关复合物的组装独立于 。我们推论,40- 复合物包含失活的 [ ],而 140- 复合物由一个类似于 160- 六聚体复合物的六聚体组成,代表了 MOMP 机制。 BAK 也被招募到了 600- 复合物中,尽管内源性过表达 的洗脱图谱与外源性添加的重组 不同 (图 2A 和 1G)。在内源性 VDAC1 被替换为 HA 标签 VDAC1 的 BAK 可诱导 $Apaf1^{- / -}$ MEFs 中,确认了 、[ ]、 和 PHB2 与血凝素 (HA)-VDAC1 的共免疫沉淀 (图 S1B)。

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VDAC1 或 VDAC2 的缺失抑制 BAX-BAK 依赖性且非 caspase 依赖性的细胞死亡

为了评估 600-kD BAK-BAX 复合物的功能,我们在 tBID 诱导的 $Apaf1^{- / -}$ MEFs 中,利用 Cas9 和单导向 RNA (sgRNAs) 靶向每个 Vdac 基因。靶向 Vdac1 或 Vdac2(而非 Vdac3)可保护 $Apaf1^{- / -}$ 细胞免于由 tBID 或由 ABT-263(navitoclax,BCL-2 和 BCL-$\mathrm{X_L}$ 的双重抑制剂)与 S63845(一种 MCL-1 抑制剂)联合抑制 BCL-2、BCL-$\mathrm{X_L}$ 和 MCL-1 所触发的细胞死亡(图 2B)(27, 28)。同时靶向 Vdac1 和 Vdac2 提供了更强的保护作用。这些发现随后在 tBID 诱导的 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ MEFs 中得到了进一步验证(图 2℃)。相比之下,在 WT 中,同时靶向 Vdac1 和 Vdac2 未能防止、甚至略微增加了细胞凋亡(图 2D)。然而,当使用泛 caspase 抑制剂 Q-VD-OPh 抑制 caspase 活性时,缺失 Vdac1 和 Vdac2 的 WT 免于 tBID 诱导的细胞死亡(图 S1C)。正如之前报道的 (4),BAX- 激活杀死 $Apaf1^{- / -}$ 的速率远低于杀死 WT 的速率(图 S1D)。在缺乏激活剂 BH3s 的情况下,ABT-263 加上 S63845 (AS) 未能激活 BAX 或 (图 S1E),这与其通过置换内源性激活剂 BH3s 来间接激活 BAX- 的机制一致 (10, 12, 29)。此外,tBID、BIM 或 PUMA 的逆转录病毒转导触发了 $Apaf1^{- / -}$ 的细胞死亡,而 VDAC1-VDAC2 的缺失抑制了这一过程(图 S1F)。遗传学研究表明,VDACs 对于 MOMP 是可有可无的 (30),且仅缺失 Vdac2 或缺失所有三种 Vdac 异构体甚至会加速 caspase 依赖性细胞凋亡 (30–32)。

与生存率数据一致,VDAC1-VDAC2 的缺失并未抑制 tBID 诱导的细胞色素 c 释放,尽管它似乎降低了基线线粒体细胞色素 c 水平(图 2E)。在 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 细胞中,通过交联仍能检测到 tBID 诱导的 BAX 或 BAK 寡聚化(图 2F)。VDAC2 不仅将 BAK 保持在失活的单体形式,还稳定其在线粒体中的定位 (31–34)。因此,在缺失 VDAC2 的情况下, BAK 变得像 BAX 一样:一旦被死亡信号激活,它便从细胞质易位至线粒体(图 2E)并形成同源寡聚体,尽管 不稳定且丰度较低(图 2F)。与 VDAC2 介导的 BAK 稳定作用一致,VDAC2(而非 VDAC1 或 VDAC3)的缺失导致 丰度降低(图 S1G)。据报道,一种小分子可结合 VDAC2 并增强其对 BAK 驱动的细胞凋亡的抑制作用 (35)。总而言之,VDAC2 似乎在负调节 依赖性细胞凋亡的同时,促进 介导的非 caspase 依赖性细胞死亡,这可能是通过与不同的 BAK 复合物(60 与 600 kD)结合实现的。

我们的研究结果表明,VDAC1-VDAC2 的缺失会抑制 $Apaf1^{- / -}$ 细胞中 tBID 诱导的死亡,且不阻断 MOMP(图 2E),这表明 BAX-BAK 依赖性、caspase 非依赖性细胞死亡并非仅仅是 MOMP 的结果。此外,MEF 细胞在缺乏细胞色素 $c$ 的情况下能够生存并增殖,且其缺乏并不影响 tBID 对 $Apaf1^{- / -}$ 细胞的杀伤(图 S1H)。我们测试了其他已知细胞死亡途径的特异性抑制剂,以研究由 BAX-BAK 激活诱导的 caspase 非依赖性细胞死亡(我们将其称为 baciptosis)(图 S1I)。这些抑制剂均未能阻止 baciptosis,从而排除了细胞焦亡(由 Q-VD-OPh 抑制)、坏死性凋亡(由蛋白激酶 RIPK1 抑制剂 necrostatin-1 和 RIPK3 抑制剂 GSK'872 抑制)、铁死亡(由 ferrostatin-1 和 deferoxamine 抑制)以及 mPTP(由 cyclosporin A 抑制)的参与。相反,通过 CRISPR-Cas9 靶向线粒体 DNA 聚合酶 gamma (Polg) 可耗尽 mtDNA,并保护 $Apaf1^{- / -}$ 细胞免受 诱导的细胞死亡(图 2G)。在用溴化乙锭处理以耗尽 mtDNA 的细胞中也观察到了类似的保护作用(图 S1J),这支持了 mtDNA 释放到细胞质中促成 baciptosis 的观点。

我们表征了 baciptosis 的形态学和生物化学特征。活细胞时间序列成像显示,表达 的 WT MEF 细胞表现出经典的凋亡特征,包括膜起泡、细胞皱缩和碎片化(视频 S1),而表达 的 $Apaf1^{- / -}$ MEF 细胞在细胞死亡前表现出显著的气球样肿胀,与坏死形态一致(视频 S2)。电子显微镜显示,WT MEF 细胞中 的表达产生了特征性的凋亡特征,包括沿核周的染色质凝聚和质膜起泡(图 S2A)。相比之下, BAK 在 $Apaf1^{- / -}$ MEF 细胞中的表达导致了坏死特征,包括质膜和细胞器破坏、自噬和线粒体自噬的诱导以及溶酶体积累(图 S2, B 和 C)。一致的是,$Apaf1^{- / -}$ 小鼠趾间蹼的发育性细胞死亡呈现坏死而非凋亡形态 (36)。这些观察结果支持将 baciptosis 分类为一种独特的程序性坏死形式。为了排除其他死亡模式,我们评估了溶酶体膜通透性,在 $Apaf1^{- / -}$ 或 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ MEF 细胞中均未检测到溶酶体破坏的证据(图 S2D)。我们还通过末端脱氧核苷酸转移酶介导的脱氧尿苷三磷酸末端标记 (TUNEL) 染色评估了基因组 DNA 的完整性。凋亡细胞显示 TUNEL 染色阳性,而 baciptotic 细胞则不显示(图 S2E)。Baciptosis 伴随着细胞死亡前 ATP 浓度的逐渐下降,而 VDAC1-VDAC2 的缺失则维持了 ATP 浓度(图 S2F)。因此,baciptotic 细胞死亡似乎在 mtDNA 释放的下游引起了灾难性的生物能量衰竭。

A

B

C

F

D

E

G

图 2. VDAC1 或 VDAC2 的缺失抑制了 BAX-BAK 依赖性的非 caspase 依赖性细胞死亡,但不抑制 caspase 依赖性细胞死亡。(A) 对 tBID 诱导的 $Apaf1^{- / -}$ MEFs 在 ± 多西环素 (1 μg / ml) 处理 6 小时后,提取 2% CHAPS 可溶性线粒体亚组分,通过 Superdex 200 (Increase 10 / 300 GL) 凝胶过滤色谱分析,随后进行免疫印迹分析。(B) 用 Cas9 和所示 sgRNAs 转导的 tBID 诱导 $Apaf1^{- / -}$ MEFs 通过免疫印迹分析。细胞经多西环素或 ABT-263 (2 μM) 加上 S63845 (10 μM) 处理,并在 48 小时通过 PI 染色和流式细胞术对细胞死亡进行定量。(C) tBID 诱导的 $Apaf1^{- / -}$ 或 $Apaf1^{- / -}$ Vdac1 $^{- / -}$ -Vdac2 $^{- / -}$ MEFs 按 (B) 中的方法处理,并在 48 小时通过 PI 染色对细胞死亡进行定量。(D) 用 Cas9 和所示 sgRNAs 转导的 tBID 诱导 WT MEFs 按 (B) 中的方法处理,并在 6 小时通过 annexin V 染色对细胞死亡进行定量。(E) tBID 诱导的 $Apaf1^{- / -}$ 或 $Apaf1^{- / -}$ -Vdac1 $^{- / -}$ -Vdac2 $^{- / -}$ MEFs 在 ± 多西环素处理所示时间后,进行亚细胞分级并通过免疫印迹分析。(F) tBID 诱导的 $Apaf1^{- / -}$ 或 $Apaf1^{- / -}$ -Vdac1 $^{- / -}$ -Vdac2 $^{- / -}$ MEFs 在 ± 多西环素 (6 小时) 处理后,用 BMH 处理并通过免疫印迹分析。星号表示分子内交联的 BAK 单体。(G) 用 Cas9 和所示 sgRNAs 转导的 tBID 诱导 $Apaf1^{- / -}$ MEFs 进行基于 qPCR 的 mtDNA 定量(左)。在多西环素处理 48 小时后,通过 PI 染色对细胞死亡进行定量(右)。(B) 至 (D) 以及 (G) 中的数据以平均值 ± 标准差 (SD) 表示($n = 3$ 次独立实验)。\* $P < 0.05$ ;

\*\*\* $P < 0.001$ ; \*\*\*\* $P < 0.0001$ ; ns,无显著差异(Student's t 检验)。

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VDAC1、VDAC2 或 prohibitins 的缺失会损害 BAX-BAK 依赖性 mtDNA 外流

由于 mtDNA 外流有助于诱发 baciptosis,而 VDAC1 和 VDAC2 的缺失会抑制这一过程,我们测试了 600-kD 的 BAK-BAX 复合物是否促进 的释放。tBID 诱导的 BAK 外流依赖于 和 (图 3A)。与细胞凋亡一样, BAK 和 BAK 在驱动 baciptosis 方面具有冗余功能(图 S3A)。在 $Apaf1^{- / -}$ 细胞中,VDAC1 和 VDAC2 的共同缺失减少了由 tBID 或 AS 诱导的 BAK 外流(图 3, B 和 C)。在 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 细胞中,逆转录转导 VDAC1 或 VDAC2(而非 VDAC3)可恢复 诱导的 BAK 外流和 baciptosis(图 3D)。与 VDAC2 在稳定 中的作用一致,在 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 细胞中重新表达 VDAC2(而非 VDAC1 或 VDAC3)可恢复 的丰度(图 3D)。因此,VDAC1 和 VDAC2(而非 VDAC3)在 - 依赖性 外流和 baciptosis 中起关键作用。

为了确定 VDAC1-VDAC2 的缺失是否影响不同 - 复合物的形成,我们在 BAK 表达前后,对来自 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 细胞的 2% CHAPS 可溶性线粒体亚组分进行了凝胶过滤色谱分析。与 VDAC2 缺失时 变得像 一样一致,在 BAK 表达前, BAK 和 BAK 仅存在于小分子量组分(40 至 60 kD)中,并在 BAK 表达后转移至 140- 至 160- 以及 600- 组分中(图 3E)。因此,凝胶过滤色谱(图 3E)和蛋白质交联(图 2F)的结果均支持,VDAC1-VDAC2 的缺失并未损害 MOMP 机制的形成。它也没有改变 、ANT1 或 PHB2 的洗脱图谱(图 3E),表明 VDAC1-VDAC2 的缺乏并未严重破坏 600- - 复合物的形成。同样,- 的缺失不影响 VDAC1、VDAC2、prohibitins 和 BAK 在 600- 复合物中的定位(图 S3B)。这些数据表明,600- 复合物的组分可能被独立地靶向至 MIM 和 MOM 之间的接触位点,而该处的特殊脂质和蛋白质微环境可能促进了它们的组装。

由于 外流需要穿过两条线粒体膜,PHB2、ANT1 或两者(与 600- - 复合物相关的 MIM 蛋白)可能参与此过程。由于 PHB2 的必需性 $(37)$,我们无法构建稳定的 Phb2 缺失细胞系。尽管如此,在 $Apaf1^{- / -}$ MEFs 中,瞬时靶向 Phb2 显著减轻了 BAK 诱导的 BAK 外流和 bacitosis(图 3, F 至 H)。相比之下,敲除 Phb2 不影响 WT MEFs 中 诱导的细胞凋亡(图 S3C)。与异二聚体 MIM 复合物中 PHB1 和 PHB2 的相互依赖性一致 (37, 38),靶向 Phb2 降低了 PHB2 和 PHB1 的丰度,但略微增加了 BAK 的丰度(图 3F)。PHB1 同样与 600- - 复合物一同洗脱,并与 BAK 共同免疫共沉淀(图 S3, D 和 E)。PHB1-PHB2 的缺失并未损害 、、VDAC1、VDAC2 或 BAK 向 600- 复合物的招募(图 S3F)。因此,prohibitins 似乎是 BAK 释放所必需的,但并非复合物组装所必需。在表达 的 $Apaf1^{- / -}$ MEFs 中,VDAC1-VDAC2 或 prohibitins 的缺失显著减轻了 IFN-$\beta$ 的积累(图 S3, G 和 H),而 IFN-$\beta$ 是 BAK 介导的 cGAS-STING-I 型 IFN 通路激活的指标。

由于 ANT1 与 ANT2 存在相互作用,且 ANT2 同样与 600-kD 复合物共同洗脱(图 S3D),因此我们对这两种异构体均进行了评估。通过慢病毒转导 Cas9 以及针对 Ant1 和 Ant2 的 sgRNA,对 tBID 诱导的 mtDNA 外流和 baciptosis 的影响极小(Fig. 3, I 和 J)。因此,尽管 ANT 蛋白和 VDAC3 存在于 600-kD 复合物中,但它们并非 BAX-BAK 依赖性 mtDNA 外流和 baciptosis 的关键介导因子,而可能仅发挥结构性或辅助性作用。尽管 VDAC 介导的线粒体钙离子内流有可能激活 mPTP,但敲除亲环蛋白 D 对 tBID 诱导的 mtDNA 外流和 baciptosis 几乎没有影响(图 S3I),这表明 mPTP 并未参与其中。使用环孢素 A 处理也得到了类似的结果(图 S1I)。VDAC1、VDAC2 和 PHB2 在 BAX-BAK 激活诱导的 mtDNA 外流和 baciptosis 中的作用在 B16-F10 小鼠黑色素瘤细胞中得到了进一步验证(图 S4)。

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凋亡小体缺陷的人类癌症中 BAX-BAK 激活诱导的 mtDNA 外流和细胞死亡的表征

鉴于人类癌症中凋亡小体失活的多种机制 (22),我们研究了在这些条件下是否会发生 baciptosis,以及该过程是否需要 VDAC1、VDAC2 和 prohibitins。我们筛选了常用的人类癌症细胞系,以寻找在 AS 诱导 BAX-BAK 激活后效应 caspase 活性最低的细胞。AS 有效地触发了 MOMP(由细胞色素 c 的释放证明),分别在 A498 肾癌、PC9 肺癌和 MDA-MB-231 乳腺癌细胞中;然而,在 A498 和 PC9 细胞中检测到的效应 caspase 活性极低,这可能是由于其 APAF1 表达量较低(图 4A 和图 S5, A 至 C)。与 caspase 激活一致,MDA-MB-231 细胞的死亡速度快于 A498 和 PC9 细胞,且只有 MDA-MB-231 细胞的细胞死亡被 Q-VD-OPh 阻断(图 4B 和图 S5D)。同时敲除 和 BAK 可保护 A498 和 PC9 细胞免受 AS 诱导的细胞死亡(图 S5E)。因此,AS 对 - 的激活在 A498 和 PC9 细胞中诱导了 baciptosis。

为了确定人类 和 BAK 在激活后是否形成上述复合物,我们分离了 AS 处理前后的 A498 细胞线粒体,并通过凝胶过滤色谱分析了 2% CHAPSS 溶解的线粒体亚组分(图 4℃)。与小鼠 类似,人类 的表观尺寸在 AS 处理后从 60 移至 160 kD,且在处理前后均与 VDAC1、VDAC2、PHB1 和 PHB2 在 \~600 kD 处共同洗脱(图 4℃)。与小鼠 一致,人类 在处理前仅以 40 的表观尺寸洗脱,处理后移至 140 和 600 (图 4℃)。BIM 在处理前主要在表观尺寸为 \~50 的组分中洗脱,但在 AS 处理后移至 600 (图 4℃)。这些结果表明,AS 将 BIM 从抗凋亡 BCL-2 家族成员中置换出来,以激活存在于 40 至 60- 和 600- 复合物中的 -,前者用于形成 MOMP 机制,后者用于形成 mtDNA 释放机制。

我们研究了 VDACs 和 prohibitins 在 A498 和 PC9 细胞中 AS 诱导的 mtDNA 外流和 bacitosis 中的作用。靶向 $VDAC1$ 或 $VDAC2$(而非 $VDAC3$)显著减轻了这两种反应(图 4, D 和 E,以及图 S5, F 和 G)。由于这些细胞无法耐受两种蛋白的同时缺失,因此无法评估 VDAC1 和 VDAC2 的同时敲除。与 MEFs 一样,VDAC2 的缺失(而非 VDAC1 或 VDAC3)降低了 BAK 的丰度(图 S5, F 和 G)。由于 prohibitins 是必需的,且人类细胞无法耐受 CRISPR-Cas9 介导的 PHB2 敲除,我们使用慢病毒短发夹 RNA (shRNAs) 瞬时敲除 PHB2。PHB2 的敲除降低了 PHB2 和 PHB1 的丰度,并显著减轻了 AS 诱导的 mtDNA 外流(图 4, F 和 G,以及图 S5, F 和 G)。然而,我们无法评估 PHB1-PHB2 缺失对 bacitosis 的影响,因为同时缺失这两种蛋白的细胞在 AS 诱导的 bacitosis 开始前就已死亡。相比之下,VDAC1 或 VDAC2 的缺失未能抑制 MDA-MB-231 细胞或 APAF1 重组 A498 细胞中 AS 诱导的凋亡(图 4, H 和 I,以及图 S5, H 至 J)。VDAC1、VDAC2 或 prohibitins 的缺失还减轻了 A498 和 PC9 细胞中 AS 诱导的 IFN- $\beta$ 表达(图 S5, K 和 L),这与其参与 - 依赖性 mtDNA 外流一致。因此,人类癌症细胞重现了小鼠的表型,证实了凋亡小体缺陷的癌症在 - 激活后可以发生 bacitosis,这一过程由 VDAC1 和 VDAC2 调节。

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图 3. VDAC1、VDAC2 或 prohibitins 的缺失会损害 BAX-BAK 依赖性的 mtDNA 外流和非 caspase 依赖性细胞死亡。(A) 转染了 Cas9 和所示 sgRNA 的 tBID 诱导型 $Apaf1^{- / -}$ MEFs 在 $\pm$ 多西环素 (doxycycline) 或 AS 处理下,分别在 48 小时进行细胞死亡定量分析,在 6 小时进行免疫印迹分析。细胞质 mtDNA 通过 qPCR 在多西环素处理后 6 小时和 AS 处理后 4 小时进行评估。(B 和 C) tBID 诱导型 $Apaf1^{- / -}$ 或 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ MEFs 处于未处理状态,或分别用多西环素 (B) 或 AS (C) 处理。细胞质 mtDNA 分别在 6 小时和 4 小时通过 qPCR 进行评估。(D) 转染了对照逆转录病毒或表达 VDAC1、VDAC2 或 VDAC3 的逆转录病毒的 tBID 诱导型 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ MEFs 在 $\pm$ 多西环素 (6 小时) 处理下,通过免疫印迹进行分析。细胞死亡在 48 小时进行定量,细胞质 mtDNA 在 6 小时进行评估。(E) 来自 $\pm$ 多西环素 (6 小时) 处理的 tBID 诱导型 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ MEFs 的 2% CHAPS 可溶性线粒体亚组分通过 Superdex 200 (Increase 10 / 300 GL) 凝胶过滤色谱分析,随后进行免疫印迹分析。(F 至 J) 转染了 Cas9 和所示 sgRNA 的 tBID 诱导型 $Apaf1^{- / -}$ MEFs 在 $\pm$ 多西环素或 AS 处理下,分别在 48 小时进行细胞死亡定量分析,在 6 小时进行免疫印迹分析 [(F) 和 (I)]。细胞质 mtDNA 通过 qPCR 在 6 小时 (G 和 J) 或 4 小时 (H) 进行评估。(A) 至 (D) 以及 (F) 至 (J) 中的数据以平均值 $\pm$ 标准差 (SD) 表示 ($n = 3$ 或 4 次独立实验)。\*P < 0.05; \*\*P < 0.01; \*\*\*P < 0.001; \*\*\*\*P < 0.0001; ns, 无显著差异 (Student's t 检验)。

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H | 图 4. VDAC1、VDAC2 或 prohibitins 的缺失会损害凋亡小体缺陷的人类癌细胞中 BAX-BAK 激活诱导的 mtDNA 外流和细胞死亡。

(A) 使用 Caspase-Glo 3 / 7 检测法定量分析了在指定时间点 ± AS 处理的指定细胞中的 Caspase 活性。(B) 在指定时间点,通过 annexin V 和 PI 染色,利用流式细胞术分析了 ± AS 和 ± Q-VD-OPh (QVD) 处理的指定细胞的细胞死亡情况。(C) 对 A498 细胞 ± AS 处理 6 小时后的 2% CHAPS 可溶性线粒体亚组分进行 Superdex 200 (Increase 10 / 300 GL) 凝胶过滤色谱分析,随后进行免疫印迹分析。(D 和 E) 分别在 12 或 6 小时后,通过 qPCR 分析了 ± AS 处理的指定 A498 (D) 或 PC9 (E) 细胞的胞质 mtDNA,并在 3 或 5 天后通过流式细胞术分析了细胞死亡情况。(F 和 G) 在 3 小时后,通过 qPCR 分析了转导指定 shRNA 的 A498 (F) 或 PC9 (G) 细胞 ± AS 处理后的胞质 mtDNA。(H) 在 24 小时后,通过流式细胞术分析了 ± AS 处理的指定 MDA-MB-231 细胞的细胞死亡情况。(I) 在 24 小时后,通过流式细胞术分析了重建 APAF1 并转导指定 sgRNA 的 A498 细胞 ± AS 处理后的细胞死亡情况。(A) 和 (B) 以及 (D) 到 (I) 中的数据以平均值 ± 标准差 (SD) 表示 (n = 3 或 4 次独立实验)。\*P < 0.05; \*\*P < 0.01; \*\*\*P < 0.001; \*\*\*\*P < 0.0001; ns,无显著差异 (Student's t 检验)。

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VDAC1 和 VDAC2 介导的 mtDNA 外流受钙调节突变的影响

线粒体中三磷酸腺苷 (ATP) 和二磷酸腺苷 (ADP) 的交换是由 VDAC 和 ANT 的协同作用介导的,它们在氧化磷酸化过程中将基质 ATP 与胞质 ADP 进行交换 $(39)$。由于 600-kD 的 BAK 相关复合物同时包含 VDACs 和 ANT,我们测试了 tBID 的招募是否会抑制这种交换。我们设计了一个 BH3 诱导系统,其中位于 BH3s 上游的 floxed 绿色荧光蛋白 (GFP) 盒阻止了它们由长末端重复 (LTR) 启动子的表达。4-羟基他莫昔芬 (4-OHT) 激活 CreERT2 以切除 GFP 盒并诱导 BH3 表达,从而导致 $Apaf1^{- / -}$ MEFs 细胞死亡(图 S6, A 至 C)。4-OHT 处理降低了 tBID 诱导细胞而非对照细胞的线粒体 导入(图 S6D)。为了确定这种损害是由 VDAC 还是 ANT 的缺陷引起的,我们测量了保留 ANT 但缺乏 的线粒体质体 (mitoplasts) 中的 BAK 摄取。尽管表达了 tBID,线粒体质体中的 BAK 摄取得到了完全恢复(图 S6D),这表明 tBID 抑制的是 BAK 介导而非 ANT 介导的 BAK 导入。BIM 或 PUMA 的过表达同样损害了线粒体 导入(图 S6E)。由于 VDAC1-VDAC2 的缺失抑制而非促进 baciptosis,激活剂 BH3 诱导的 BAK 核苷酸通道关闭不太可能是 baciptosis 的直接原因。相反, BAK 的关闭可能反映了使 mtDNA 外流成为可能所需的构象重塑。

当 对代谢物运输关闭时,它对钙变得高度通透,从而促进线粒体钙内流 (40)。VDAC1 的 E73 和 E203 与钙调节有关 (41–44)。E73 还调节 VDAC1 的构象、脂质相互作用以及己糖激酶-I 诱导的通道关闭 (42, 44)。E73 在 VDAC2 (E85) 中保守,但在 VDAC3 (Q73) 中不保守(图 S6F),这可能解释了为什么 VDAC3 不参与 BAX-BAK 依赖性的 mtDNA 外流和 bacitosis(图 2B 和 3D)。我们测试了 BAX-BAK 激活诱导的 VDAC1 和 VDAC2 关闭是否能增加线粒体钙内流。使用一种基于荧光蛋白的线粒体靶向钙指示剂 mito-G-GECO1.2 (45),我们发现 tBID 的表达增加了线粒体钙内流,而这种内流在 $Bax^{- / -}Bak^{- / -}$ 细胞中被消除(图 5A 和 BAK 图 S7A)。VDAC1 和 VDAC2 的缺失降低了 tBID 诱导的线粒体钙内流(图 5B 和 BAK 图 S7B)。同样,AS 以依赖于 VDAC1 和 VDAC2 的方式增加了线粒体钙内流(图 5℃ 和 BAK 图 S7C)。

为了确定 VDAC1 和 VDAC2 中与钙调节相关的残基是否可能导致 tBID 诱导的线粒体钙内流,我们使用以下内容重建了 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 细胞:

野生型(WT)或 VDAC1(E73Q / E203Q)和 VDAC2(E85Q / D215N)的钙调节突变体。这些突变部分损害了 VDAC1 和 VDAC2 恢复由 BAX-BAK 激活诱导的线粒体钙内流的能力(图 5D 和图 S7D)。在 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 细胞中,重建野生型而非突变型 VDAC1 和 VDAC2 可挽救 tBID 诱导的 mtDNA 外流和 baciptosis(图 5E)。突变体将 BAK 的稳定性、线粒体定位以及基线细胞色素 $c$ 水平完全恢复到与野生型 VDAC1 和 VDAC2 相同的水平,但未能促进 mtDNA 外流或 baciptosis(图 5F)。与功能缺失的研究结果一致(图 S1G),在 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 细胞中,野生型或突变型 VDAC2(而非 VDAC1)恢复了 BAK 的丰度(图 S7E)。VDAC1 和 VDAC2 的突变体仍与 600-kD 的 -BAX 复合物相关联,且未改变其他 - 复合物的形成(图 5G)。我们进一步将分析扩展到由过氧化氢或 ionomycin 触发的 BAK 外流,这些物质会增加线粒体钙浓度(46, 47)。VDAC1-VDAC2、- 或 prohibitins 的缺失减轻了由这些刺激诱导的 BAK 外流,尽管在这些条件下细胞死亡仍然发生(图 S8)。这些发现进一步支持了 VDAC1-VDAC2、- 和 prohibitins 在 BAK 外流中可能扮演的角色,且这种作用超出了 tBID 或 BH3 模拟物对 BAK 和 BAK 的经典激活。

据报道,在非死亡的小鼠胚胎成纤维细胞(MEFs)中,VDAC1 或 VDAC3 寡聚体在氧化应激下介导 从线粒体释放,这一过程独立于 和 (48)。VDAC1 的 N 端赖氨酸残基介导其与 BAK 的相互作用,而这对于 VDAC1 的寡聚化及随后的 BAK 释放是必需的(48)。因此,我们比较了 VDAC1 的 N 端赖氨酸突变和钙调节突变对 - 激活诱导的 BAK 外流的影响。在 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 细胞中,逆转录病毒转导野生型和 N 端赖氨酸突变体(K12A / R15A / K20A)的 VDAC1 均可恢复 tBID 诱导的 BAK 外流和 bacitosis(图 5H)。相比之下,VDAC1 的 E73Q / E203Q 突变体未能挽救这些表型(图 5H)。我们认为,激活蛋白 BH3 对 - 的激活与 VDAC1 和 VDAC2 的构象重塑相关,这种重塑减少了核苷酸转运,增加了线粒体钙内流,并实现了 BAK 向细胞质的释放。

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包含 tBID 的 600-kD BAK 复合物可使线粒体质体通透化从而诱导 mtDNA 外流

为了确定包含 tBID 的 600-kD BAK 复合物是否能直接使线粒体内膜(MIM)通透化,我们将来自 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}Bax^{- / -}Bak^{- / -}$ 细胞的线粒体质体,与从 $Apaf1^{- / -}$ 细胞的凝胶过滤色谱中收集的 60-( 表达前)、160-( 表达后)以及 600-( 表达前或后)组分共同孵育。 BAK 表达后的 600- 复合物表现出最高的 mtDNA 释放活性,而 表达前的 600- 复合物仅显示出极低活性(图 6A)。相比之下,源自表达 的 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 细胞的 600- 复合物未能使 MIM 通透化以释放 mtDNA(图 6A),这强调了 VDAC1 和 VDAC2 的关键作用。此外,从表达 且重组了 VDAC1 和 VDAC2 突变体( $Apaf1^{- / -}Vdac1^{\mathrm{MT}}$ $Vdac2^{\mathrm{MT}}$ )的 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 细胞中获得的 600- 复合物,表现出极低的 mtDNA 释放活性(图 6A)。这些体外实验补充了我们的细胞实验结果,并支持由 BAK、BAX、、VDAC1、VDAC2 和 prohibitins 组成的 600- 复合物即为 mtDNA 释放机制。

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VDAC1 和 VDAC2 的缺失并不妨碍 BAX-BAK 激活诱导的 MIM 疝出

鉴于有提议认为通过 BAX-BAK 大孔的 MIM 疝出介导了 mtDNA 的释放 (19),我们研究了 VDAC1 和 VDAC2 的缺失是否会损害这一过程。由于 MIM 疝出预计会降低 MOM-MIM 的共定位,因此将线粒体外膜转位酶 20 (TOMM20)-GFP 和线粒体内膜转位酶 50 (TIMM50)-mCherry 转导至

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图 5. 钙调节突变损害 BAX-BAK 激活期间 VDAC1 和 VDAC2 依赖性的线粒体钙内流和 mtDNA 外流。(A 和 B) 使用共聚焦荧光显微镜分析了表达 mito-G-GECO1.2 的指示性 tBID 诱导型 $Apaf1^{- / -}$ MEFs ± 多西环素 (4 小时)。(B) 中分析了两个独立克隆。使用 ImageJ 对荧光强度进行定量;每个点代表一个细胞。(C) 按 (A) 中的方法分析了表达 mito-G-GECO1.2 的指示性 $Apaf1^{- / -}$ MEFs ± AS (4 小时)。分析了两个独立克隆。(D) 按 (A) 中的方法分析了表达 WT VDAC1 / 2 (VDAC1 / 2 $^{\mathrm{WT}}$ ) 或钙调节 VDAC1 / 2 突变体 (VDAC1 / 2 $^{\mathrm{MT}}$ ) 以及 mito-G-GECO1.2 ± 多西环素 (4 小时) 的 tBID 诱导型 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ MEFs。(E) 分析了表达 VDAC1 / 2 $^{\mathrm{WT}}$ 或 VDAC1 / 2 $^{\mathrm{MT}}$ ± 多西环素的 tBID 诱导型 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ MEFs 在 48 小时时的细胞死亡情况,以及在 6 小时时的胞质 mtDNA 和蛋白表达情况。(F) 对指示细胞 ± 多西环素处理指示时间后进行亚细胞分级和免疫印迹分析。(G) 使用 Superdex 200 (Increase 10 / 300 GL) 凝胶过滤色谱法和免疫印迹分析了表达 VDAC1 / 2 $^{\mathrm{MT}}$ ± 多西环素 (6 小时) 的 tBID 诱导型 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ MEFs 的 2% CHAPS 可溶性线粒体亚组分。(H) 分析了表达 VDAC1 $^{\mathrm{WT}}$ 或指示 VDAC1 突变体 ± 多西环素的指示细胞在 48 小时时的细胞死亡情况,以及在 6 小时时的胞质 mtDNA 和蛋白表达情况。[(A) 至 (D)] 的统计学显著性使用 Student's t 检验评估,以确定一个样本的平均荧光强度是否超过另一个样本的 150% ($n = 3$ 次独立实验)。(E) 和 (H) 中的数据以平均值 ± 标准差 (SD) 表示 ($n = 3$ 次独立实验)。\*\* $P < 0.01$ ; \*\*\* $P < 0.001$ ; \*\*\*\* $P < 0.0001$ ; ns,无显著差异 (Student's t 检验)。

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C

D

[⚠ 低质量翻译,建议复核] 图 6. 含有 tBID 的 600-kD BAK 复合物能够使缺乏 BAX、BAK、VDAC1 和 VDAC2 的线粒体质体(mitoplasts)通透化,从而诱导 mtDNA 外流。(A) 对 tBID 诱导的 $Apaf1^{- / -}$、$Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 以及表达钙调节 VDAC1 / 2 突变体的 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ MEFs ($Apaf1^{- / -}Vdac1^{MT}Vdac2^{MT}$) ± 多西环素(6 小时)的线粒体,采用 Superdex 200 (Increase 10 / 300 GL) 凝胶过滤色谱法进行分析,如图 2A 所示。将指示分子量大小的分级组分与来自 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}Bax^{- / -}^{- / -}$ MEFs 的线粒体质体共同孵育,并通过 qPCR 评估 mtDNA 的释放。数据以平均值 ± 标准差 (SD) 表示($n = 3$ 次独立实验)。(B) 表达 TOMM20-GFP 和 TIMM50-mCherry 的 BAK 诱导 $Apaf1^{- / -}$ 和 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ MEFs ± 多西环素(2.5 小时),使用抗 TOMM20 和抗 mCherry 抗体通过免疫荧光分析(另见图 S9A)。数据以 TOMM20-GFP 和 TIMM50-mCherry 之间的 Manders 共定位系数表示($Apaf1^{- / -}$ 对照组、$Apaf1^{- / -}$ 组、$Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 对照组和 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 组的 $n$ 分别为 22, 38, 24 和 33)。(C 和 D) 经多西环素处理 3.5 小时 (C) 后指示细胞的代表性透射电子显微镜图像。红色箭头表示 MIM 疝出;插图显示放大视图。比例尺,1 μm。对 ± 多西环素处理的指示细胞中的 MIM 疝出情况进行了定量分析 (D)。每个点代表每细胞中具有内膜疝出的线粒体百分比。数据以平均值 ± 标准差 (SD) 表示($Apaf1^{- / -}$ 对照组、$Apaf1^{- / -}$ 组、$Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 对照组和 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 组的 $n$ 分别为 15, 15, 14 和 18)。(E) 由 BAK 和 BAK 调节的 caspase 依赖性和 caspase 非依赖性细胞死亡的示意模型。\* $P < 0.05$ ; \*\* $P < 0.01$ ; \*\*\*\* $P < 0.0001$ ; ns,无显著差异(Student's t 检验)。

诱导的 $Apaf1^{- / -}$ 和 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 细胞分别用于可视化 MOM 和 。 BAK 的表达导致 $Apaf1^{- / -}$ 和 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 细胞中 MOM- 共定位程度出现相当的降低(图 6B 和图 S9A),表明 VDAC1 和 VDAC2 的缺失不会损害 诱导的 BAK 疝出。电子显微镜证实了两种细胞类型中均存在相当的 BAK 疝出(图 6, C 和 D)。同样,Prohibitin 的破坏未能阻止 诱导的 MOM- 共定位降低(图 S9B),表明 prohibitins 对于 诱导的 BAK 疝出也是可有可无的。

总的来说,我们将数据解释为: BAK 疝出可能是 MOM 中 - 大孔形成的结果,而非驱动 mtDNA 外流的主动机制。与这一观点一致的是,只有少数疝出的 BAK 表现出膜完整性的丧失 (19)。 BAK 疝出在缺乏 VDAC1 和 VDAC2 的情况下可能依然存在,因为它们的缺失并不能阻止 - 寡聚化和 MOMP(图 2, E 和 F,以及 3E)。这种持续性可能解释了为什么 VDAC1-VDAC2 的缺失既不能完全阻断 mtDNA 外流,也不能在 - 激活后促进 $Apaf1^{- / -}$ 细胞的长期克隆原性存活(图 3, B 和 C,以及图 S9, C 和 D)。综上所述,我们的数据表明,含有 、VDAC1、VDAC2 和 prohibitins 的 600-kD - 复合物构成了负责大部分 mtDNA 释放的主要机制,而 疝出则在 - 激活后导致次级 mtDNA 泄漏。

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讨论

我们提供了生化证据,证明 BAK 和 BAX 在被激活蛋白 BH3-only 蛋白激活后,会组装成两种不同的线粒体蛋白复合物,分别独立介导细胞色素 c 和 mtDNA 的外流(图 6E)。释放细胞色素 c 的 MOMP 机制可能由 BAK 或 BAX 六聚体组成,这与已报道的体外研究一致 $(49, 50)$。我们将这些六聚体鉴定为释放细胞色素 c 的机制,这或许可以解释为什么这些孔洞太小,无法通过超分辨率显微镜观察到 $(19)$。相比之下,释放 mtDNA 的机制则由 BAK、BAX、激活蛋白 BH3s、VDAC1 和 VDAC2(MOM 蛋白)以及 prohibitins(MIM 蛋白)组成,并可能定位于 MOM 和 MIM 之间的接触位点。因此, MIM 外流并非简单的 MOMP 下游结果,而是一个独立且活跃的生化过程。相反,在细胞色素 c 释放后,通过 BAX 或 BAK 大孔发生的 MIM 疝出似乎是 MOMP 的结果,且独立于 VDAC1 和 VDAC2。

尽管 BAX-BAK 依赖性的 MIM 外流发生在 caspase 介导的细胞凋亡过程中,但其启动延迟,使其不太可能对快速的 caspase 驱动死亡产生贡献。相比之下, MIM 外流有助于 caspase 非依赖性的 BAX-BAK 介导死亡,因为通过敲除 $Vdac1$、$Vdac2$ 或 $Phb2$,或在 $Apaf1^{- / -}$ 细胞中耗竭 来破坏该过程,会抑制这种形式的细胞死亡。这些发现在人类癌细胞中得到了重现。低水平的 APAF1 表达会损害效应 caspase 的激活,而将 APAF1 恢复到临界阈值以上则可重新建立激活。凋亡小体缺陷的人类癌症在 BAX-BAK 激活后可发生 bacitosis,这一过程受 VDAC1 和 VDAC2 调节。这些发现表明,治疗诱导的 BAX-BAK 激活在凋亡小体缺陷型癌症中对肿瘤-免疫相互作用的影响可能比在凋亡小体完备型癌症中更大 (16)。

由于发生 baciptosis 的细胞缺乏细胞凋亡的定义性超微结构特征(图 S2B),因此需要一个新术语来描述这种独特的程序性细胞死亡形式。尽管此前被描述为 MOMP 诱导的 caspase 非依赖性细胞死亡 $(51)$,但我们的研究鉴定出一种在机制上可与 MOMP 分离的 BAK-BAX 复合物。我们将这种坏死形式的程序性细胞死亡命名为 baciptosis,以将其与铁死亡(ferroptosis)和坏死性凋亡(necroptosis)等其他形式的 caspase 非依赖性细胞死亡区分开来。耗竭 Cgas、Ifi16 或 Zbp1 并未抑制 baciptosis(图 S10, A 和 B),且 MEFs 表达的 Aim2、Nlrp3 和 Tlr9 极少。因此,baciptosis 似乎并非由经典的细胞质 DNA 感知通路介导。细胞质 促进细胞死亡的精确机制仍有待定义。

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材料与方法 细胞系

所有 MEF 细胞均经过 SV40 转化,并按照此前报道的方法进行培养 $(4)$。四环素诱导的 tBID 表达 $Apaf1^{- / -}$ MEF 细胞是通过慢病毒转导和单细胞亚克隆生成的,tBID 由多西环素 (1 $\mu$g / ml; Sigma) 诱导。BH3 诱导的 $Apaf1^{- / -}$ MEF 细胞是通过使用 MSCV-CreERT2-Neo 和 MSCV-LoxP-GFP-LoxP-BH3-pPGK-Puro 进行逆转录病毒转导,随后进行单细胞亚克隆生成的。使用 4-OHT (500 nM; Sigma) 处理后 BH3 的表达通过免疫印迹法进行了确认。为了生成 $\rho^{0}$ 细胞,$Apaf1^{- / -}$ MEF 细胞在 200 ng / ml 溴化乙锭 (Thermo Fisher Scientific) 中培养三个代次。敲除细胞系是通过 CRISPR-Cas9 介导的基因组编辑生成的,具体描述见 $(52, 53)$。简而言之,细胞经表达 Cas9 和针对目标基因的 sgRNA 的慢病毒转导,随后进行单细胞亚克隆。敲除克隆通过免疫印迹法检测目标蛋白的缺失来鉴定。在 $Apaf1^{- / -}$ MEF 细胞中删除 Vdac1 和 Vdac2 以生成 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 细胞。在 $Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 细胞中重建野生型 (WT) 或突变型 Vdac 是通过逆转录病毒转导完成的。

B16-F10 细胞 (RRID: CVCL\_0159) 获取自美国标准细胞库 (ATCC),并按照制造商的建议进行培养。MDA-MB-231 (RRID: CVCL\_0062) 和 A498 (RRID: CVCL\_1056) 细胞获取自美国国立癌症研究所发育治疗计划,并在添加了 10% 胎牛血清、1% 青霉素 / 链霉素、1% 非必需氨基酸、1% 丙酮酸钠、1% L-谷氨酰胺和 1% HEPES (Thermo Fisher Scientific) 的 RPMI 1640 中培养。PC9 细胞(人肺腺癌,男性来源;RRID: CVCL\_B260)获取自纪念斯隆-凯特琳癌症中心 (MSKCC) 的 D. Scheinberg,并按照此前描述的方法进行培养 $(54)$。所有细胞系均使用 Venor GeM 支原体检测试剂盒 (Sigma) 定期进行支原体检测。

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质粒构建、CRISPR-Cas9 介导的基因组编辑和 RNA 干扰

慢病毒四环素诱导的潮霉素抗性载体 TRE-gene of interest-pPGK-Hygro-T2A-rtTA3 是使用 NEBuilder HiFi DNA Assembly Cloning Kit (New England Biolabs) 从 pCW-Cas9、LentiCRISPRv2 和 MSCV-Hygro (Addgene) 组装而成的。缺失编码区 N 端 177 个碱基对的小鼠 Bid (tBID) 被克隆到该载体中。使用 Optimized CRISPR Design 设计的 sgRNA 被克隆到 LentiGuide-Puro 或 LentiCRISPRv2 (Addgene) 中 (55)。小鼠 Vdac1、Vdac2 和 Vdac3 被克隆到 MSCV-Hygro (Clontech) 或 MSCV-IRES-GFP (4) 中,Vdac 突变体是通过基于聚合酶链式反应 (PCR) 的定点突变生成的。mito-G-GECO1.2 是通过将来自 CMV-mito-R-GECO1 的线粒体靶向信号与来自 CMV-G-GECO1.2 (Addgene) 的 G-GECO1.2 融合 (45),并将该融合片段克隆到 pBABE-Puro (Addgene) 中生成的。小鼠 Apaf1 被克隆到 MSCV-IRES-GFP (4) 中。

所有构建体均经过序列验证。慢病毒是通过使用 Lipofectamine 2000 (Thermo Fisher Scientific) 将 pCMV-dR8.2 和 pHCMV-VSV-G 共转染至 293T 细胞中产生的,具体描述见此前报道 (52)。sgRNA 序列列于表 S2 中。针对人类 PHB2 的慢病毒 shRNA 获取自 Sigma (TRCN0000060921),针对 GFP 的慢病毒 shRNA 见此前描述 (56)。

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细胞活力与 caspase 活性分析

细胞以每孔 $8 \times 10^{4}$ 或 $1 \times 10^{5}$ 个细胞的密度接种于 12 孔板中,并在次日使用指定的试剂进行处理。使用多西环素(1 $\mu$ g / ml;Sigma)诱导 tBID 表达,或使用 ABT-263(2 $\mu$ M;Selleck Chemicals)结合 S63845(5 或 10 $\$ M;Chemietek)诱导细胞死亡。在指定条件下,细胞分别使用 Q-VDOPh(20 $\$ M;MedKoo Biosciences)、necrostatin-1(5 $\$ M;Sigma)、GSK'872(10 $\$ M;Sigma)、ferrostatin-1(20 $\$ M;Selleck Chemicals)、去铁胺(deferoxamine, 50 $\$ M;Selleck Chemicals)或环孢霉素 A(cyclosporin A, 2 $\$ M;Selleck Chemicals)进行处理。细胞死亡通过 annexin V(BioVision 或 Abcam)和 / 或碘化丙啶(PI, 2 $\$ g / ml;Sigma)染色进行定量,具体操作如前所述(56),随后使用 LSRFortessa 和 FACSDiva 软件(BD Biosciences)进行流式细胞术分析。对于 IncuCyte 分析,

细胞以每孔 8000 个细胞的密度接种于 96 孔板中,次日进行处理,使用 SYTOX Green(100 nM;Thermo Fisher Scientific)染色,并使用 IncuCyte S3 活细胞分析仪(Sartorius)监测长达 7 天。每 2 到 6 小时采集一次图像。使用 IncuCyte 基础分析软件,将 SYTOX Green 阳性汇合度相对于相差图像中的总汇合度进行归一化,以此定量细胞死亡。对于 caspase 活性分析,细胞接种于 96 孔板中,次日进行处理,并根据制造商说明使用 Caspase-Glo 3 / 7 分析系统(Promega)进行分析。

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亚细胞分级、抗体和免疫印迹分析

在 tBID 诱导后的指定时间收集细胞,并在含有 0.025% digitonin、10 mM KCl、5 mM MgCl₂、1 EDTA、1 EGTA、250 蔗糖和 20 HEPES (pH 7.2) 的 digitonin 通透化缓冲液中冰浴孵育 5 分钟,并添加完整的蛋白酶抑制剂混合物 (Roche)。通过 15,000g 离心将含有线粒体的细胞器与胞质组分分离,并在含有 1% Triton X-100 和蛋白酶抑制剂的磷酸盐缓冲盐水 (PBS) 中裂解。胞质、线粒体和全细胞裂解物通过 NuPAGE (Thermo Fisher Scientific) 或 SDS-聚丙烯酰胺凝胶电泳 (SDS-PAGE) (Bio-Rad) 进行分离,转移至聚乙烯吡咯烷酮 (PVDF) 膜 (Immobilon-P; Millipore),通过增强化学发光 (Western Lightning Plus-ECL; PerkinElmer) 进行检测,并使用 LAS-3000 系统 (Fujifilm) 或 Amersham Imager 680 (GE Healthcare) 进行成像。用于免疫印迹的一抗为:anti-BID (Cell Signaling Technology (CST), #2003, RRID:AB_10694562)、anti-BIM (Covance) (52)、-PUMA (CST, #98672, RRID:AB_3096180)、-BAX (Santa Cruz Biotechnology, #sc-493, :AB_2227995; , #2772, :AB_10695870; Proteintech, #60267-1-Ig, :AB_2848213)、-BAK (Upstate, #06-536, :AB_310159; , #12105, :AB_2716685)、-VDAC1 (Calbiochem, Porin 31HL, :AB_565262; Abcam, #ab186321 (:AB_3739918) 或 #ab16814)、-VDAC2 (Covance 针对氨基酸 212 至 228 肽段的兔多克隆抗体 (31); , #9412, :AB_10828727)、-VDAC3 (31)、-ANT1 (MitoSciences, #MSA02, :AB_478281; Abcam, #ab110322, :AB_10862212)、-ANT2 (, #14671, :AB_2798562)、-PHB1 (, #2426, :AB_823689)、-PHB2 (Upstate, #07-234)、-Cyclophilin D (Affinity BioReagents, #PA1-028, :AB_2169135)、-ATP synthase β (BD Biosciences, #612518, :AB_399819)、-COX IV (, #4844, :AB_2085427)、-TOMM20 (, #42406, :AB_2687663)、-PolG (Abcam, #ab128899, :AB_11145308)、-cytochrome c (Pharmingen, #556433, :AB_396417)、-LDHA (, #3558, :AB_2135109)、-APAF1 (, #8723, :AB_10829610; Chemicon, #06-957)、-Procaspase-9 (, #9502, :AB_2068621)、-Procaspase-3 (BD bioscience, #611048)、-FIS1 (Axxora, #ALX-210-907)、-cGAS (, #31659, :AB_2799008)、-ZBP1 (Santa Cruz Biotechnology, #sc-271483, :AB_10650130)、-IFI204 (Abcam, #ab307201, :AB_3166180)、-β-Actin (Sigma, #A1978, :AB_476692) 以及 -tubulin (Sigma, #T9026, :AB_477593)。

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线粒体 BAK 相关复合物的鉴定

按照此前所述 (4, 7, 8),从 $Bax^{- / -}Bak^{- / -}$ MEFs 或用 N 端蛋白 C 标签 BAK 重构的 $Bax^{- / -}Bak^{- / -}$ MEFs 中分离线粒体。使用含有 1% 或 2% CHAPS、142.5 KCl、2 CaCl₂、20 Tris-Cl (pH 7.4) 和无 EDTA 蛋白酶抑制剂混合物 (Roche) 的 1% 和 2% CHAPS 裂解缓冲液对线粒体进行顺序提取,随后进行超声处理。将裂解物应用于 -protein C 亲和基质 (Roche),用 10 EDTA 洗脱结合的复合物,用三氯乙酸沉淀,在 4 至 12% NuPAGE 凝胶 (Thermo Fisher Scientific) 上进行分离,并进行银染 (Silver Staining Plus Kit; Bio-Rad)。切下感兴趣的凝胶切片,用胰蛋白酶消化,并在 Taplin 质谱设施 (哈佛医学院,马萨诸塞州波士顿) 使用液相色谱-串联质谱进行分析。

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线粒体亚组分分离

线粒体外膜(MOMs)、线粒体内膜(MIMs)和接触位点的分离采用了已发表的方法并进行了微调 $(57)$。所有步骤均在 $4^{\circ}C$ 或冰上进行。线粒体在 MB 缓冲液(200 mM 蔗糖, 1 mM EGTA, 和 10 HEPES, pH 7.5)中分离,在 EB 缓冲液(125 KCl, 4 MgCl $_{2}$ , 5 KH $_{2}$ PO $_{4}$ , 和 10 HEPES, pH 7.5)中洗涤,并在 10,000g 下离心 10 分钟沉淀。沉淀物在溶胀缓冲液(20 HEPES, 0.5 EDTA, pH 7.5)中重悬 30 分钟,通过 30 针头穿刺 5 次,然后与等体积的收缩缓冲液(0.90 M 蔗糖, 20 HEPES, 0.5 EDTA, pH 7.5)共同孵育 15 分钟。样本经超声处理产生囊泡,并在 10,000g 下离心 10 分钟。上清液被铺在不连续蔗糖梯度(1.6, 1.35, 1.1, 和 0.85 M)之上,并在 Optima MAX-XP 超速离心机(Beckman Coulter)中以 35,000 rpm 离心 14 小时。收集对应于 $\sim100万美元 蔗糖(MOM)、1.2 M(接触位点)和 1.36 M(MIM)的分级部分,在 2% CHAPS 缓冲液(142.5 KCl, 2 CaCl₂, 和 20 Tris, pH 7.5)中裂解,用三氯乙酸沉淀,并通过免疫印迹法分析。

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凝胶过滤色谱、免疫共沉淀和蛋白质交联

凝胶过滤色谱在 Superdex 200 HR 10 / 30 柱(GE-Amersham)上使用 ÄKTA 纯化系统(Cytiva)进行,或在 Superdex 200 Increase 10 / 300 GL 柱(Cytiva)上使用 ÄKTA basic 10 FPLC 系统(GE-Amersham)进行,如前所述 (8)。色谱柱在含有 1% 或 2% CHAPS, 300 NaCl, 0.2 二硫苏糖醇和 20 HEPES (pH 7.5) 的缓冲液中平衡。用于校准的分子量标准为:甲状腺球蛋白(669 kD)、铁蛋白(440 kD)、过氧化氢酶(232 )、醛缩酶(158 )、结合蛋白(75 )、牛血清白蛋白(BSA, 66 )、卵白蛋白(44 )和细胞色素 c(14 )。线粒体裂解液被加载到色谱柱上,并以 0.3 ml / min 的速度洗脱。收集分级部分(0.6 ml),用三氯乙酸沉淀,通过 8 到 16% SDS-PAGE 或 4 到 12% NuPAGE 分离,并通过免疫印迹法分析。对于 N 端蛋白 C 标签 BAK 的免疫共沉淀,将指定的分级部分合并,并在 2 Ca $^{2+}$ 和无 EDTA 蛋白酶抑制剂存在下与抗蛋白 C 基质(Roche)共同孵育。免疫共沉淀物通过 4 到 12% NuPAGE 分离,并通过银染和免疫印迹法分析。对于抗 HA 免疫共沉淀,在 2% CHAPS 缓冲液(142.5 KCl, 2 CaCl $_{2}$ , 和 20 Tris-Cl, pH 7.4)中制备的裂解液与抗 HA 抗体(12CA5)共同孵育,并用蛋白 A 琼脂糖(Pierce)捕获。为了检测 BAK 或 BAX 的寡聚化,tBID 诱导细胞用多西环素处理 6 小时,然后在室温下与 5 BMH(Thermo Fisher Scientific)共同孵育 30 分钟。

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体外细胞色素 c 释放和蛋白质交联

含有 BAK 相关复合物的凝胶过滤分级部分使用 Amicon Ultra 离心过滤器(10- MWCO; Sigma)用线粒体分离缓冲液(200 甘露醇, 70 蔗糖, 1 EGTA, 和 10 HEPES, pH 7.5)进行浓缩和缓冲液交换。样本(每个复合物 1.2 ml)被稀释 >20 倍,以将 CHAPS 浓度降低至 <0.1%,并浓缩至 50 $\mu$ l。从 200 $\mu$ g 线粒体的凝胶过滤运行中回收的每个复合物,在最终体积为 100 $\mu$ l 的条件下与 $Bax^{- / -}Bak^{- / -}$ 线粒体(1 mg / ml)共同孵育。细胞色素 c 的释放通过比色酶联免疫吸附测定(ELISA, R&D Systems)进行定量,如前所述 (7),并相对于凝胶过滤缓冲液对照组进行归一化。为了检测 BAK 寡聚体,洗脱分级部分在室温下与 2.5 BMH(Thermo Fisher Scientific)共同孵育 30 分钟,用 NuPAGE 样本缓冲液淬灭,通过 4 到 12% NuPAGE 分离,并通过抗 BAK 免疫印迹法分析。

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ADP 导入测定

ADP 导入测定按照此前所述的方法 $(58)$ 进行。分离线粒体 $(4, 7, 8)$ 并将其重新悬浮于 ADP 导入缓冲液(250 mM 蔗糖, 20 mM HEPES, 10 KCl, 5 琥珀酸, 3 $KH_{2}PO_{4}$ , 1.5 $MgCl_{2}$ , 1 EGTA, 5 $\mu$ M 鱼藤酮, pH 7.2)中,浓度为 0.5 mg / ml。线粒体悬浮液 (400 $\mu$ l) 在含有或不含 50 $\$ M atractyloside (Sigma) 的条件下,补充 0.5 $\$ Ci 的 ${}^{14}C$-ADP (PerkinElmer NEN Radiochemicals),并在冰上孵育 10 min。通过加入 700 $\$ l 含有 50 $\$ M atractyloside 的 ADP 导入缓冲液来停止反应。样本洗涤两次,与闪烁液混合,并使用 LS6000 液体闪烁计数器 (Beckman Coulter) 进行分析。ANT 依赖性 ADP 摄取量计算为含有和不含 atractyloside 预孵育样本之间的计数差值。为了

分离线粒体质体 (mitoplasts),将纯化后的线粒体 (0.5 mg / ml) 在线粒体质体分离缓冲液(220 甘露醇, 70 蔗糖, 2 HEPES, pH 7.5)中用 0.15% (w / v) digitonin (Sigma) 处理,在冰上放置 10 min,然后在 10,000g 下离心 10 沉淀。

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线粒体 DNA 外流的定量

收集细胞 $(1.5 \times 10^{6})$ 并将其分为两部分。五分之一在 2000 rpm 下离心 4 沉淀,并使用 DNeasy Blood and Tissue Kit (Qiagen) 提取总 DNA。剩余的细胞经沉淀后,在 digitonin 通透化缓冲液(0.025% digitonin, 10 KCl, 5 $MgCl_{2}$ , 1 EDTA, 1 EGTA, 250 蔗糖, 20 HEPES, pH 7.2)中在冰上通透化 5 ,然后在 4℃ 下以 15,000g 离心 10 。使用 Optima MAX-XP 超速离心机 (Beckman Coulter) 在 4℃ 下将上清液以 100,000g 离心 60 。所得上清液收集为细胞质组分,并使用 QIAquick Nucleotide Removal Kit (Qiagen) 纯化 DNA。全细胞和细胞质 DNA 使用 SYBR Green Master Mix 在 ViiA 7 或 QuantStudio 3 实时 PCR 系统 (Thermo Fisher Scientific) 上通过定量 PCR (qPCR) 进行分析。核

DNA 使用小鼠 Tert 或人类 ACTB 的引物检测,mtDNA 使用 D-loop 引物检测。在细胞质组分中未检测到核 DNA,证实不存在核裂解。细胞质 mtDNA 的 Ct 值相对于全细胞 进行了归一化,并根据归一化后的细胞质 丰度计算 外流的倍数增加。qPCR 使用的引物如下:小鼠 D-loop, 5'-CATCTCGATGGTATCGGGTC-3' 和 5'-GGTGCGTCTAGACTGTGTGC-3';小鼠 Tert, 5'-CTAGCTCATGTGTCAAGACCCTCTT-3' 和 5'-GCCAGCACGTTTCTCTCGTT-3';人类 D-loop, 5'-GGATCACAGGTCTATCACCCTA-3' 和 5'-CAGCGTCTCGCAATGCTATC-3';以及人类 ACTB 5'-GGCACCCAGCACAATGAAGATC-3' 和 5'-TGAGGACCCTGGATGTGACAG-3'。

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体外线粒体质体 mtDNA 的释放

从未经处理或经多西环素处理的 tBID 诱导型 $Apaf1^{- / -}$、$Apaf1^{- / -}Vdac1^{- / -}Vdac2^{- / -}$ 以及 $Apaf1^{- / -}Vdac1^{MT}Vdac2^{MT}$ MEFs 中分离出线粒体(200 $\mu$g),随后使用 CHAPS 裂解缓冲液进行顺序提取,以获得 2% CHAPS 可溶的线粒体亚组分。该亚组分在 Superdex 200 Increase 10 / 300 GL 柱上进行分离,并收集对应于指定分子量的组分。为了分离线粒体质体,将来自 $Bax^{- / -}Bak^{- / -}Vdac1^{- / -}Vdac2^{- / -}Apaf1^{- / -}$ MEFs 的线粒体(0.5 mg / ml)在 mtDNA 释放缓冲液(142.5 mM KCl, 250 $\mu$M CaCl$_{2}$ , 20 mM Tris-Cl, pH 7.4,并添加无 EDTA 蛋白酶抑制剂混合物)中用 0.15% (w / v) digitonin (Sigma) 在冰上处理 10 分钟,然后在 10,000g 下离心 10 分钟沉淀。含有 BAK 相关复合物的凝胶过滤组分经过缓冲液交换,并使用 Amicon Ultra 离心过滤器(10 kD MWCO, Sigma)进行浓缩。样本(每个复合物 1.2 ml)用 mtDNA 释放缓冲液稀释 >20 倍,使 CHAPS 浓度降低至 <0.1%,并浓缩至 50 $\$l。每个从 200 $\$g 线粒体凝胶过滤运行中回收的 BAK 相关复合物,与来自 50 $\$g 线粒体的线粒体质体在 100 $\$l 中于 30℃ 下孵育 30 分钟。样本在 4℃ 下以 10,000g 离心 10 分钟,并使用 DNeasy Blood and Tissue Kit (Qiagen) 从沉淀中提取 DNA。上清液使用 Optima MAX-XP 超速离心机 (Beckman Coulter) 在 4℃ 下以 100,000g 离心 60 分钟,并使用 QIAquick Nucleotide Removal Kit (Qiagen) 从所得上清液中纯化 DNA。使用 ViiA 7 或 QuantStudio 3 实时 PCR 系统 (Thermo Fisher Scientific) 配合 D-loop 引物通过 qPCR 对 mtDNA 进行定量。超速离心上清液中的 mtDNA Ct 值相对于 10,000g 沉淀中的 Ct 值进行归一化,并根据相对于仅与缓冲液孵育的线粒体质体的归一化值计算 mtDNA 的释放量。

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逆转录与 qPCR

使用 TRIzol (Thermo Fisher Scientific) 从细胞中提取总 RNA。使用 SuperScript II ( ) 配合 oligo(dT) 和随机十聚体引物进行逆转录。使用 SYBR Green Master Mix ( ) 和基因特异性引物在 ViiA 7 或 QuantStudio 3 实时 PCR 系统 ( ) 上进行两次重复的 qPCR。数据相对于 $\beta$-Actin 进行归一化。qPCR 引物为:小鼠 Ifnb1, 5'-CCTTTGCCATCCAAGAGATGCTC-3' 和 5'-AGTTGAGGACATCTCCCACGTC-3';小鼠 Actb, 5'-GCCATGTACGTAGCCATCCAGGC-3' 和 5'-CTCCAGGGAGGAAGAGGATGCGGC-3';人类 IFNB1, 5'-GCTCTCCTGTTGTGCTTCTCCA-3' 和 5'-TGAGGCAGTATTCAAGCCTCCC-3';以及人类 ACTB, 5'-TCCCTGGAGAAGAGCTACGAG-3' 和 5'-AGGAAGGAAGGCTGGAAGAGTG-3'。

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线粒体钙离子的定量分析

细胞以每孔 $4.5 \times 10^{4}$ 个的密度接种于 4 孔腔室载玻片(Nunc Lab-Tek II)中,次日使用多西环素(1 $\mu$ g / ml;Sigma)或 ABT-263(2 $\mu$ M;Selleck Chemicals)加上 S63845(10 $\mu$ M;Chemietek)处理 4 小时;未处理的细胞作为对照。细胞用 4% 多聚甲醛固定,用 4',6-二脒-2-苯基吲哚(DAPI, Sigma)染色,并使用配备 40× / 1.2 数值孔径 (NA) 水浸物镜(HCX PL APO;#506341)的 Leica SP5 倒置共聚焦显微镜进行成像。每细胞的平均绿色荧光强度( $F_{0}$ )计算公式为 $F_{0} = F\_c / S$ ,其中 $F\_c$ 为每个细胞的绿色荧光总强度,S 为相应的细胞面积。核分割和细胞区域界定采用了先前描述的方法 (59),并使用 ImageJ 进行定量。对于每种条件,定量分析了 50 到 200 个细胞,相对荧光强度通过在三次独立实验中相对于对照细胞的平均值进行归一化计算。统计显著性通过 Student's t 检验进行评估,以确定一个样本的平均相对荧光强度是否超过另一个样本的 150%。

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共聚焦显微镜与共定位分析

表达 TOMM20-GFP 和 TIMM50-mCherry 的细胞被接种在 4 孔腔室载玻片(EMD Millipore)中,并在 37℃ 下用指定的试剂处理。细胞用 4% 多聚甲醛(Sigma)固定 15 分钟,用 PBS 洗涤三次,然后在室温下于含有 0.1% Triton X-100 (Sigma)、1% BSA (EMD Millipore) 和 5% 山羊血清 (Sigma) 的 PBS 透化和封闭缓冲液中孵育 1 小时。细胞与稀释在封闭缓冲液中的抗 TOMM20 (Abcam, #ab13970) 和抗 mCherry (CST, #43590S) 一抗在 4℃ 下孵育过夜。洗涤三次后,细胞与山羊抗鸡 AF488 (Invitrogen, #A-11039) 和山羊抗兔 AF594 (Thermo Fisher Scientific, #A-11012) 二抗孵育 1 小时。再次洗涤两次后,细胞用 DAPI (Sigma) 染色,并使用配备 63× / 1.4 NA Plan Apochromat 物镜的 Zeiss LSM 880 共聚焦显微镜进行成像。对于共定位分析,图像被转换为 8 位格式,进行默认的自动阈值处理,并使用 Fiji 中的 Coloc2 插件分析以计算 Manders 共定位系数 (60, 61)。

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透射电子显微镜

透射电子显微镜分析由 Weill Cornell Medicine 的显微镜核心设施完成。细胞沉淀用改良的 Karnovsky 固定液固定,随后用还原四氧化铪进行二次固定 $(62)$ 。经过梯度乙醇脱水后,样本被包埋在 Epon 类似树脂中,并使用 Leica Ultracut S 超薄切片机上的 DiATOME 金刚石刀切成 65 nm 的薄片。超薄切片按照先前描述的方法 $(63)$ 用柠檬酸铅进行对比增强,并使用在 100 kV 下运行的 JEM-1400 透射电子显微镜 (JEOL) 进行成像。数字图像由 Veleta 2K × 2K CCD 相机 (EMSIS GmbH) 采集。

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活细胞成像

细胞以每孔 $4.5 \times 10^{4}$ 个的密度接种于 4 孔腔室载玻片(Nunc Lab-Tek II)中,次日用多西环素 (1 $\mu$ g / ml) 处理

或保持未处理状态。相差活细胞成像使用由 ZEN 软件控制并配备 40× / 0.6 NA 空气物镜(LD Achroplan 40× / 0.6 Ph2; Zeiss)的 Zeiss 显微镜进行。在多西环素处理后 1 到 5 小时(对于 WT MEFs)以及处理后 36 到 41 小时(对于 $Apaf1^{- / -}$ MEFs)采集时间序列图像,以评估细胞形态和行为。

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TUNEL 染色

WT 和 $Apaf1^{- / -}$ MEFs 分别在不处理或使用多西环素(1 $\mu$g / ml)处理 3 和 40 小时,以诱导 tBID。收集细胞,在室温下用 4% 多聚甲醛固定过夜,用 PBS 洗涤,并在 4℃ 下以 1700 rpm 离心 5 分钟使之沉淀。固定后的沉淀经石蜡包埋,由 MSKCC 的分子细胞学核心设施进行 TUNEL 染色处理。切片(5 $\mu$m)被贴在玻璃载玻片上,在室温下干燥过夜,并在 60℃ 下孵育 1 小时。载玻片在二甲苯中脱蜡,通过梯度乙醇复水至水,并在 Discovery Ultra 自动染色机(Ventana Medical Systems, Roche)上进行处理。在 37℃ 下进行热修复后,载玻片用内源性生物素阻断试剂盒(Ventana Medical Systems)处理 20 分钟,并与 TdT(1000 U / ml; Roche)和生物素-dUTP(4.5 nmol / ml; Roche)共同孵育 2 小时。

信号使用链霉亲和素-HRP(Ventana Medical Systems)检测 32 分钟,并使用 Alexa Fluor 488 Tyramide SuperBoost 试剂盒(1:150; Thermo Fisher Scientific)放大 16 分钟。载玻片用 DAPI(5 $\mu$g / ml; Sigma)复染 5 分钟,用 Mowiol 4-88(Sigma)封片,并使用配备 40× / 1.3 NA 油浸物镜的 LSM 880 共聚焦显微镜(Zeiss)进行成像。

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胞质组织蛋白酶 B 活性的定量

在诱导细胞死亡之前或之后收集细胞,以 2000 rpm 离心 4 分钟使之沉淀,并在冰上使用含有 0.025% digitonin、10 mM KCl、5 mM MgCl₂、1 EDTA、1 EGTA、250 蔗糖和 20 HEPES (pH 7.2) 的 digitonin 缓冲液中通透化 5 分钟。裂解液在 4℃ 下以 15,000g 离心 10 分钟以去除细胞核、线粒体和膜结合细胞器。上清液使用 Optima MAX-XP 超速离心机(Beckman Coulter)在 4℃ 下以 100,000g 离心 60 分钟。所得上清液被收集为胞质组分,并使用组织蛋白酶 B 活性测定试剂盒(Abcam)测量组织蛋白酶 B 的活性。使用 SpectraMax M5 多功能微孔板阅读器(Molecular Devices)测量荧光,并相对于未处理的对照组进行归一化。

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细胞 ATP 水平的定量

将细胞以每孔 $2.5 \times 10^{5}$ 个细胞的密度接种于 6 孔板中,次日用指定的试剂处理或保持不处理。收集细胞并计数,每项测定使用 $1 \times 10^{4}$ 个细胞。使用 ATP 生物发光测定试剂盒 HS II(Roche)测量细胞 ATP。将荧光素酶试剂(50 $\mu$l)与 50 $\mu$l 稀释样本混合,并使用 GloMax Navigator 微孔板发光仪(Promega)测量发光强度。使用试剂盒提供的 ATP 标准品进行系列稀释,为每次实验生成标准曲线,并将信号相对于未处理的对照组进行归一化。

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致谢

由于篇幅限制,未能引用相关研究的调查人员,我们深表歉意。我们感谢纪念斯隆-凯特琳癌症中心(MSKCC)分子细胞学核心设施,特别是 Y. Romin 和 E. Chan,以及威尔康奈尔医学院显微成像与图像分析核心设施,特别是 L. Cohen-Gould 和 J. Jimenez。资金支持:本研究得到了美国国立卫生研究院(NIH)国家癌症研究所(NCI)(授予 E.H.C. 的 R01 CA252658 资助和授予 C.M.R. 的 P30 CA008748 资助)以及 Geoffrey Beene 癌症研究中心(MSKCC)(E.H.C.)的支持。作者贡献:S.Y. 和 H.K. 设计并执行了实验并分析了数据。E.H.C. 构思并设计了研究,分析并解释了数据,并监督了该项目。G.L.、N.T.、H.T.、S.R.、C.C.、Z.L. 和 N.T. 执行了部分实验。J.J.H. 分析并解释了数据。竞争利益:J.J.H. 是 ICEN Therapeutics 的联合创始人。E.H.C. 是 ICEN Therapeutics 的顾问。这些关系与本研究无关。作者声明没有其他竞争利益。数据、代码和材料可用性:所有数据均可在正文或补充材料中获得。许可信息:版权 © 2026 作者,保留部分权利;独家许可方为美国科学促进会(AAAS)。对美国政府原始作品不主张权利。https: / www.science.org / about / science-licenses-journal-article-reuse

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补充材料

图 S1 至 S11;表 S1 至 S3;视频 S1 和 S2;MDAR 可重复性检查清单 2025年 30 June 提交;2026年 10 April 重新提交;2026年 2 September 被接收

10.1126 / science.aea2181

AAAS 的会员社区是科学家和 STEM 爱好者的一个一站式目的地。这里是“科学社交之所”:一个事实至上、创意宏大,且总有理由来此聚集、分享、讨论和探索的社区。

会员社区 AAAS

研究论文

分子生物学

非编码转录控制长程基因调节的发育动力学

Philippe J. Batut $^{1,2*}$ 和 Michael S. Levine $^{1*}$

调节基因表达的基因组区域本身通常会被转录成多种非编码 RNA (ncRNAs)。然而,这种非编码转录的调节作用在很大程度上仍然未知。通过使用活体成像,我们揭示了源自不同调节元件的 ncRNAs 的顺序转录是果蝇胚胎中基因激活的基础。单等位基因共可视化发现,最佳的基因激活仅由中等水平的增强子活性实现。破坏与增强子相关的 BAK 会导致基因提前激活,这证明了 BAK 控制发育过程中基因表达的时序。我们进一步表明,增强子转录可以调节复杂调节景观中的长程相互作用。我们提出, BAK 在顺式方向上局部调节调节元件的活性,以塑造基因组组织并协调发育过程中基因表达的时间控制。

在动物基因组中,许多基因受控于巨大的调节景观,这些景观可跨越数兆碱基(megabases),且在疾病中经常遭到破坏 (1, 2, 3)。这些区域包含调节元件的集群(包括增强子),它们在发育过程中驱动特定时空模式的转录 (1, 2, 3, 4, 5)。我们和其他研究人员已经表明,基因组的空间组织在指定调节相互作用中可以起到指导作用 (6, 7),使增强子能够跨越巨大的基因组距离控制基因启动子处的转录 (1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11)。这些调节区域本身被广泛转录,产生无数的非编码 RNA () (12, 13, 14, 15, 16, 17, 18)。特别是, BAK 已成为脊椎动物 (19) 和无脊椎动物 (20, 21) 中活性增强子的标志。尽管之前的研究已经确定了许多单个 的顺式调节作用 (15, 22, 23, 24, 25),包括长链和短链的增强子相关 RNA (eRNAs) (16, 17),但目前尚不清楚这些非编码转录中有多少在功能上是相关的,而不仅仅是伪造的或机会性的 (15, 23, 26)。它如何被部署以在发育过程中调节基因表达在很大程度上也尚未被探索。最后,我们对于 如何在长程调节的背景下运作,以及它们如何利用——甚至控制——基因组组织的某些方面,了解有限。利用果蝇胚胎作为模型系统,我们结合了全基因组和活体成像方法,以确定调节元件处的非编码转录在基因表达的发育控制中的作用。

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调控元件中受发育调控的 ncRNA 转录

我们利用先前发表的 PRO-cap 数据 (20),在早期胚胎(即身体蓝图建立阶段)中进行了全基因组转录分析。该方法通过识别新生 RNA 的 5' 端,能够以单核苷酸分辨率绘制转录起始位点,非常适合检测稀有或不稳定的转录本。我们排除了蛋白质编码基因的启动子,将分析重点完全放在 ncRNA 上。我们检测到 40% 的活性增强子内部启动了非编码转录 [见补充材料 (SM),材料与方法],这与之前的报告 (20, 21) 一致(图 1, A 和 B,以及图 S1, A 至 C)。这表明其丰度远高于随机预期(图 S1C)。除增强子外,我们还分析了系留元件(tethering elements)的转录。这类调控序列影响三维 (3D) 基因组组织 (6, 7),且在功能上与增强子截然不同(图 S1, A 和 B)。我们在之前的一项研究中表明,系留元件促进了特定的长程增强子-启动子相互作用和基因激活 (6)(图 1A)。PRO-cap 分析显示,33% 的系留元件同样产生 (图 1B 和图 S1, A 至 C)。

尽管调控区域中非编码转录的普遍性已得到证实,但其功能相关性尚不明确。为了深入探讨这一问题,我们测量了 MSKCC 转录起始位点 (TSSs) 的序列保守性。通过利用 PRO-cap 的单核苷酸分辨率,我们能够检测到精确集中在增强子相关和系留元件相关 的 TSSs 上的强序列保守模式(图 1℃ 和图 S1, D 和 E)。这表明调控元件上的非编码转录承受着强烈的选择压力——暗示其在整个基因组中发挥着重要的生物学功能。

Hox 基因 *Sex combs reduced* (*Scr*) 证明了这一点,它是动物身体蓝图的主调节因子之一 (27),也是人类 *Hox5* 基因的同源基因 (28)。我们此前已经证明,*Scr* 在胚胎中受位于其启动子上游约 35 kb 处的远端增强子调控,且一个远端系留元件 (DTE) 促进了这种长程增强子-启动子相互作用 (6)。*Scr* 增强子和 DTE 在胚胎中均被转录,产生截然不同且定义明确的长 (图 1D)。为了评估它们的生物学相关性,我们重新分析了之前关于 保守性研究中多种果蝇物种的发育转录组时间序列 (29)。这些数据集是使用名为 RAMPAGE (30) 的 TSS 剖析方法生成的,结果显示这两种 在功能上已保守超过 3500 万 年。它们由具有明显序列保守性的可识别核心启动子转录而来(图 S2, A 和 B)。此外,全基因组范围内增强子相关和系留元件相关 的发育转录动态(包括 *Scr* 位点的两种 )也高度保守(图 1, E 和 F,以及图 S1, F 和 G,和图 S2, A 和 B)。值得注意的是,*Scr* eRNA 的时间转录谱在整个基因组中属于最保守的前 1%——比 *Scr* 基因本身的保守程度更高(图 1F)。这些观察结果表明,两种 *Scr* 的转录动态对发育至关重要。

为了高分辨率地表征这些动态过程,我们对 Scr 位点进行了工程化改造,以便在发育中胚胎的单细胞中可视化内源性 ncRNA 的转录(图 1G 和视频 S1 至 S3)。我们的活体成像数据揭示了一个精确有序的“启动序列”,其中增强子、系留元件和基因以稳健的时间顺序依次被激活(图 1H 和图 S3)。这些观察结果表明,不同调控元件的顺序激活可能是基因表达时间控制的基础。与增强子活性应指令性决定基因活性的预期相反,我们的定量分析显示,在增强子表现出最强活性的 45 分钟期间,Scr 基因没有检测到转录,这表明存在额外的调控层级。

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体内增强子-基因对的单细胞转录动力学

为了更好地理解增强子及其靶基因之间的定量关系,我们通过在活胚胎中顺式测量单个等位基因上的转录动力学来进行研究(图 2A 和视频 S4)。

A 拴系元件促进远程增强子-启动子相互作用

B

c

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D Scr HOX 基因座的组织结构

E 5 个物种中的发育动力学

F 发育动力学的保守性

G 转录的单细胞成像

H ncRNA 转录的活体成像

图 1. 调控元件处的非编码转录广泛存在、具有保守性且高度动态。(A) 增强子可以在较大的基因组距离上激活靶启动子的转录。系留元件(Tethering elements)本身不具备增强子活性,但能促进特定的长程增强子-启动子相互作用 (6)。(B) 对 3 至 4 小时胚胎的 PRO-cap 数据进行全基因组分析,发现在 40% 的活性基因间增强子和 33% 的系留元件中存在活性 TSS。热图显示了以识别出的 TSS 为中心、在同一基因组链上 800-bp 窗口内的 PRO-cap 信号分布(见 SM,材料与方法)。(C) 对于 (B) 中定义的类别,在以每个 TSS 为中心的 800-bp 窗口内,每个位置的平均序列保守性(phastCons 分数)。阴影包络线:SEM;灰色条:聚合 PRO-cap 信号。(D) HOX 基因 Scr(Antennapedia 复合物 ANT-C 的一部分)的 Micro-C 接触图及注释。Scr 远端调控区域包括一个早期胚胎 (EE) 增强子,以及一个远端系留元件 (DTE),后者与一个启动子近端系留元件 (TE) 形成局灶接触(Micro-C 面板中的箭头)(6)。EE 增强子包含增强子相关 ncRNA [eRNA, CR44931, \~7.4 kb(粗框代表外显子)] 的 TSS,而 DTE 包含远端系留相关 ncRNA (dtRNA, CR45559, \~0.6 kb) 的 TSS。ftz 和 Antp 是该基因座上的其他蛋白质编码基因。(E) 5 种果蝇物种(分化时间跨度约 3500 万 年)中,4 个知名发育基因和 Scr eRNA 在胚胎发育过程中的转录动力学。对每个物种在整个胚胎发育过程中以 1 小时分辨率进行转录组分析 (29);对于每个基因,5 条曲线对应 5 个物种。所有时间序列在计算上均与 D. melanogaster 参考序列对齐,以此定义时间轴(产卵后的小时数)。4 个保守的发育基因证明了时间序列之间时间对齐的准确性。(F) 全基因组所有活性启动子转录动力学保守性分数的分布 (N = 10,229 个启动子)。箭头显示了 Scr 基因的两个替代启动子、eRNA 启动子和 dtRNA 启动子的转录动力学保守性分数。(G) 内源性 Scr 基因及其 eRNA 在反式(trans)构象下的活性转录灶活体成像。图像是来自晚期囊胚期胚胎 [核周期 14 (NC14)] 4D 活体显微成像数据集的单个共聚焦 z-stack 的最大强度投影;灰色:细胞核(组蛋白 H2A);洋红色:eRNA (PP7);绿色:Scr 基因 (MS2)。图像仅为显示目的而优化(2 倍上采样和高斯平滑);定量分析是在原始 4D 数据上进行的(见 SM,材料与方法)。(H) 内源性 Scr 基因及其两个相关 ncRNA 在 NC14 间期内每个细胞核的平均转录输出量化(包络线:生物学重复间的 SEM)。每个转录本分别被内源性标记 MS2,并在不同的胚胎中进行可视化。

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eRNA 与 mRNA 转录的体内共可视化

增强子-基因对转录的时间动态

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C 增强子与基因转录之间的定量关系

图 2. 发育调节的增强子-基因对的单细胞转录动态。(A)(上)内源性 Scr 基因及其增强子相关 RNA (eRNA) 在同一等位基因(顺式配置)上的活性转录焦点(箭头)的共可视化。灰色:细胞核;紫色:Scr 基因 (PP7);青色:eRNA (MS2)。比例尺,2 $\mu$ m(2倍上采样和高斯平滑,仅用于显示)。(下)单个代表性细胞核的转录信号。两个通道分别归一化至其各自的最大值;箭头表示单个基因激活事件。(B)(上)在所有观察到的基因激活事件中,Scr 基因及其增强子 (eRNA) 的单细胞转录信号,并与基因转录的开始时间对齐(N = 12 个胚胎,n = 118 个事件;包络线:所有事件的 SEM)。由于基因转录的检测需要转录延伸通过检测盒,虚线表示基于体内延伸速度估计的基因激活时间窗(见 SM,材料与方法)。(下)增强子与基因转录信号之间的时间滞后互相关(箭头:互相关最小值;包络线:基于 1000 次自助法估计的 90% 置信区间)。(C)(上)与增强子转录开始时间对齐的单个增强子激活事件 (n = 267)。单细胞轨迹根据转录开始后 3 分钟期间达到的最小信号进行颜色编码(虚线)。(下)增强子转录(增强子激活后 3 分钟期间达到的最小信号)与随后的基因转录(增强子激活后 4 分钟期间基因转录的最大增幅)之间的关系。基因转录的时间根据延伸速度的估计进行了偏移(见 SM,材料与方法)。单细胞事件被分为增强子转录信号的 8 个分位数;点显示每个分位数的平均增强子和基因转录信号(误差棒:两个轴上的 SEM)。

这表明基因激活事件似乎并不与离散的增强子激活事件同步。相反,增强子在基因激活之前的较长时间内似乎处于强转录状态。Scr 表达的开始实际上与增强子转录的减少相一致,这由基因激活时间前后两个信号之间剧烈的负互相关所证明(图 2B)。

我们进一步定量分析了单个增强子激活事件的强度与随后基因转录增幅之间的关系。该分析揭示了增强子与基因转录之间强烈的非单调关系:在低水平时,增强子活性与基因活性正相关,但在较高水平时则呈负相关(图 2℃)。在 eRNA 和基因位于同源染色体上且呈反式配置的阴性对照中,未显示出此类相关性(图 S4)。综合这些观察结果表明,反直觉地,增强子转录可能会抑制基因激活。

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非编码转录控制基因激活的时机

我们通过在内源位点内对 eRNA TSS 进行精确的 45-bp 缺失,并利用活体成像测量其对基因转录的影响,测试了 eRNA 转录抑制 Scr 表达的可能性。此次缺失导致 Scr 转录水平增加,表明增强子的转录会削弱基因表达(图 3, A 和 B,以及图 S5, A 至 C)。 转录的缺失还导致基因的激活明显提前。相比之下,基因活动的空间模式仅有轻微改变,这表明 特异性地控制 激活的时机(图 3B 和图 S5, A 至 C)。在反式(trans)位置缺失 TSS 对基因活动和动力学的影响微乎其微,表明 严格在顺式(cis)位置控制基因激活的时机(图 S6)。

为了排除缺失 TSS 导致移除了位于 核心启动子内的 沉默子元件的可能性,我们将其替换为特性明确的异源核心启动子——来自分节基因 *even-skipped* (*eve*) 的启动子。活体转录测量量化结果显示,这不仅恢复了 转录,而且使其比野生型增加了数倍(图 3, A 和 B)。由 *eve* 驱动的 完全恢复了对 的抑制,导致 表达水平降低且启动时间延迟(图 3B 和图 S7, A 和 B)。此外,与野生型相比,由 ** 启动子增强的 转录导致 表达水平下降更明显,激活时机的延迟也更显著。

通过在 启动子内进行核苷酸替换,获得了进一步支持“ 转录控制 表达水平和时机”这一模型的证据。我们在 启动子起始子(INR)元件中替换了 5 个核苷酸,已知这会严重损害启动子活性 (31)。这种细微的替换导致了 表达的提前激活和水平增加,其效应大小与在原始

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A 增强子相关 RNA () TSS 缺失(内源位点)

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B 增强子 ncRNA 转录

基因转录

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C 基因抑制取决于 转录本长度

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D DTE相关RNA (dtRNA) TSS缺失

图 3. 来自 HOX 位点增强子和 DTE 的转录控制基因表达的动力学。(A) 在内源位点通过 CRISPR 介导的 Scr eRNA TSS(45 bp)缺失,以及用 eve 核心启动子替换 Scr eRNA TSS 的示意图。(B) 在缺失 并用 eve 核心启动子替换后,对 增强子(左)和基因(右)转录进行的活体单细胞测量。(C) 将 转录单位的主体(~7.3 kb,从 下游 37 bp 到第一个 PAS 上游 39 bp,包括内含子和两个末端外显子的部分区域)替换为源自 $\lambda$ 噬菌体基因组的序列(包含添加提前 SV40 PAS 插入和不包含插入两种情况)后,对 基因进行的活体转录测量。(D) 在 dtRNA 缺失后,对 基因进行的活体转录测量。

内源 的缺失(图 S8)。综上所述,这些结果表明, 转录的丧失导致了在缺失 启动子时观察到的 表达时间点和水平的变化。

接下来,我们试图通过研究 抑制对 序列和长度的依赖性,来深入了解其潜在机制。我们将 转录本的主体 [从 下游 37 个碱基对 (bp) 到聚腺苷酸信号 (PAS) 上游 39 bp] 替换为源自 $\lambda$ 噬菌体基因组的不相关序列。这种 7.3-kb 的序列替换维持了整体转录本长度,且旨在仅改变位于 增强子下游的序列(图 S9A)。与野生型相比,这种 ncRNA 替换导致了更强的 抑制(图 3℃ 和图 S9),从而排除了 转录暴露了影响 表达的隐蔽沉默子元件 (32) 的可能性,因为 $\lambda$ 替换完全移除了原有的 转录单位。

的抑制可能涉及 和 启动子之间对增强子招募的限量因子的竞争,而非全长 的合成。为了检验这些潜在机制,我们测试了合成报告基因和内源 位点的编辑。转基因报告实验表明,虽然启动子竞争可以轻微降低基因活性,但不足以解释在野生型胚胎中观察到的 激活时间点的长期延迟(图 S5D)。为了直接测试是否需要合成全长转录本,我们在 转录单位的 5' 区域( 下游 280 bp 处)插入了一个猿猴病毒 40 聚腺苷酸信号 (SV40 PAS)。为了排除 转录过程中暴露的未知 DNA 沉默子元件可能产生的任何影响,PAS 是在 $\lambda$ 替换的背景下插入的。$\lambda$ ncRNA 的提前终止导致 转录水平相对于单独的 $\lambda$ 替换显著增加(图 3℃),且基因激活发生的时间甚至早于野生型胚胎(图 S9)。综合来看,这些观察结果表明,仅靠 转录过程不足以实现基因活性的抑制和时间控制。相反,正常的 转录动力学需要产生全长 ncRNA,而与其原发序列无关。

为了探讨 Scr 位点的不同 ncRNA 是否具有不同的调节功能,我们删除了由 DTE 转录的 ncRNA 的 TSS(dtRNA)。与 eRNA 不同,dtRNA 的缺失并不影响 Scr 激活的时间动态,而是导致转录无法达到最大速率(图 3D 和图 S5, B 和 C)。综合这些结果表明,由增强子和 DTE 编码的 具有相反的调节功能——一个起抑制作用,另一个起激活作用——且 eRNA 特异性地决定了基因激活的时机。删除 dtRNA 或 eRNA 的 TSS 都会产生后果。两者均会导致经典的 Scr 同源异形表型——成年雄性前腿上性梳数量的变化(图 S10)。这表明顺式调节 会影响生物体的适应度。

为了确定 Scr 模型的普适性,我们还研究了一个位于 Antennapedia 基因(Antp P2)第二个启动子上游约 34 kb 处的 的潜在调节作用,该 是我们基于 RAMPAGE 和 PRO-cap 数据识别出的。该 由一个推测的系留元件(tethering element)转录,该元件与 P2 启动子形成一个弱调节环(图 S11A)。在跨越 3500 万 年进化分歧的五个物种中均观察到了该 的转录,且其在胚胎发育期间的时间活动谱高度保守(图 S11B)。对其 TSS 进行局部删除(45 bp;图 S11A)会导致 Antp 基因的转录率出现轻微但显著的增加(图 S11C)。该 似乎通过仅在其正常表达区域的前半部分定量抑制基因活性,从而调节 Antp 表达的空间模式(图 S11, C 和 D)。

我们还在其他发育控制基因的调节区域中识别出几个额外的 ,与它们相关的基因相比,这些 表现出截然不同的时空表达模式。我们再次发现,这些 在整个黑腹果蝇(Drosophila)演化支中具有高度保守性(图 S12)。这些观察结果提出了这样一种可能性: 可能被用作一种广泛的策略,用于精确控制发育控制基因的转录动态。

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增强子转录本控制系留元件活性与基因组组织

ncRNA 能够远程调节 *Scr* 基因转录的能力,促使我们研究它们与促进远程相互作用的系留元件(tethering elements)之间的关系。一个具有吸引力的假设是,远端增强子及其相关的 eRNA 可能会调节 DTE 的活性。我们通过在活胚胎中对增强子进行定向编辑,并测量 dtRNA 的转录情况来测试这一模型。此前我们已证明删除整个增强子会降低 *Scr* 的活性 (6),而此次结果显示,删除整个增强子还会导致 dtRNA 转录量剧烈下降——这证明了 DTE 的转录主要受 增强子的控制(图 4A)。相比之下,局部删除 eRNA 的转录起始位点(TSS)会导致 dtRNA 转录量大幅增加(图 4A)。这一结果表明,除了抑制 之外, 的转录还强烈抑制 的转录活性。

为了研究 调节 表达是否需要 ,我们在同一等位基因上同时删除了 和 TSS,并测量了其对基因转录的调节影响。结果显示,在 激活的时间点上存在完全的上位性(epistasis)。双突变体表现出与仅缺失 时相同的激活延迟,这表明 仅在 存在时才对 ** 产生调节影响(图 4B 和图 S13, A 和 B)。一个合理的解释可能是 仅仅是 转录所必需的,但我们通过证明删除 不会消除反而会略微增加 的转录,从而排除了这种可能性(图 S13, C 和 D)。相反,这种相互作用暗示了非编码转录与基因组组织之间存在某种相互影响。在 $\Delta , \Delta $ 双突变体中观察到的胚胎晚期合成致死现象,进一步强调了这种跨界对话(cross-talk)的生物学相关性。

为了确定 是否影响 与 ** 启动子形成调节环的能力,我们在缺失 TSS 的编辑胚胎中进行了 Micro-C 分析 (33)。尽管该位点的整体组织在很大程度上未受影响,但 的破坏导致 -启动子相互作用增加(图 4℃ 和图 S14)。在全基因组最强的 100 个环中,这是检测到的唯一显著变化,其中包括相邻 *Antp* 位点的一个 -启动子环(图 S14)。综合来看,这些结果表明 转录调节 的活性及其参与 ** 远程激活的能力。

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讨论

包含多个顺式元件和非编码RNA(ncRNA)的复杂调控区域是发育和疾病相关位点的标志,但人们对其了解仍然不足。本研究通过在活胚胎中实时可视化ncRNA的转录,揭示了此类区域的调控动态。对转录动态的单细胞定量分析揭示了ncRNA基因调控机制中出人意料的见解。

我们表明,Scr的表达时间与远端增强子及其系留元件(tethering element)的激活并不一致,相反,它们的转录呈现出一种明确的时间启动顺序。这挑战了增强子活性直接决定基因活性的观点。相反,调控元件似乎构成了一个顺式网络,支配着一个多步骤的激活过程。细胞分化的转录组研究表明,在哺乳动物细胞中,增强子转录在全局上早于基因启动子的转录 (34)。

A DTE转录受早期增强子(Early Enhancer)和eRNA的控制

B eRNA调控活性需要DTE

C eRNA TSS缺失的Micro-C分析

D 总结模型

图 4. 增强子转录控制系留元件转录和远程相互作用。(A) EE增强子和eRNA对DTE转录的调控。(左)增强子和eRNA TSS的缺失。(右)在增强子和eRNA TSS缺失后,DTE相关RNA (dtRNA) 的实时转录测量。(B) Scr eRNA与DTE之间的遗传相互作用。(左)DTE和eRNA TSS的缺失。(右)分别以及组合缺失两种元件的实时转录测量。同时破坏这两个元件会导致胚胎致死。(C) eRNA TSS缺失后Scr位点的Micro-C分析。(上)早期胚胎 (NC14) 中eRNA TSS缺失突变体的Micro-C接触图。(插图)阶段匹配的野生型胚胎的Micro-C接触图(见图 1D)。(下)在野生型和eRNA TSS缺失突变体胚胎中,Scr启动子(锚点)在整个Scr TAD范围内的相互作用谱的虚拟 4℃(圆形染色质构象捕获)定量分析。(D) 拟议模型。在发育早期,高增强子活性驱动强烈的eRNA产生。eRNA反过来 (i) 抑制远程调控环的形成,以及 (ii) 抑制增强子活性,可能是通过破坏转录凝聚体实现的。随着增强子活性逐渐减弱,eRNA介导的抑制被解除——从而实现基因激活的精确计时。

我们的工作证明,增强子转录可以延迟基因表达,以实现激活的精确计时。综合来看,这些观察结果为ncRNA在基因活性时间控制中的作用提供了证据,并表明增强子转录可能被广泛用于控制发育过程中基因活性的动态。我们的研究还表明,顺式调控ncRNA影响一系列调控结果,包括激活时间 (Scr eRNA)、表达水平 (Scr dtRNA) 和空间模式 (Antp P2)。

对 Scr 时间动态的精确控制不仅取决于增强子处的转录起始或延伸过程,还需要严格在顺式(cis)起作用的全长 eRNA 产物。这些 eRNA 具有两种调节效应(图 4D):抑制增强子活性(图 S5)以及破坏远程调节环路(图 4℃)。尽管这一过程高度依赖于转录本长度,但它并不取决于特定的 RNA 序列(图 3℃)。在分子水平上,可以设想多种不同的机制,但我们主要考虑两种非互斥的可能性。一种是高浓度的 eRNA 破坏了转录凝聚体(25, 35–40),这可能解释了在单细胞水平上观察到的增强子与基因活性之间的非单调关系(40)(图 2)。另一种可能性是 eRNAs 与转录共激活因子(以及 DNA 环路因子)相互作用,从而破坏它们与染色质的结合或调节其调节活性(15, 23)。此外,Pol II 或其他限速因子被截留在 eRNA 启动子处也可能会削弱基因激活。我们提出,顺式调节 ncRNAs 通过这些或其他机制,在共转录过程中调节底层 DNA 元件的活性,从而定量控制基因表达的时间。

我们的发现与最近的一项研究相呼应,该研究描述了在小鼠胚胎干细胞中,合成转录本通过对转录速率和转录本长度的高度依赖来实现基因抑制(41)。该研究同样支持一种依赖于 RNA 的机制,而非简单的启动子竞争模型,并突显了我们的工作与脊椎动物基因调节的相关性。值得注意的是,Scr eRNA 是一种具有高度方向性的约 7.4-kb 剪接长非编码 RNA (lncRNA)。已有研究表明,剪接可以调节 lncRNA 的染色质释放和增强子活性(42),这使得 $\lambda$ ncRNA 中内含子的缺失可能会增加新生转录本的滞留,并进一步延迟 Scr 表达的开始。

我们还提供了顺式调节 ncRNAs 与基因组组织之间关键相互作用的证据。尽管之前的研究已经表明 ncRNAs 可以影响基因组组织(43–45),但我们的工作揭示了这种机制如何被用于调节发育过程中基因活性的时间动态。在 ncRNA 与相邻结构元件之间观察到的强遗传相互作用——以及相关的胚胎致死性——表明,即使是没有明显敲除表型的 ncRNAs(26),实际上也可能发挥关键的生物学功能,这对我们理解复杂疾病的遗传架构具有重大意义。鉴于 ncRNAs 在人类基因组中的普遍存在(15),这些见解表明,非编码转录可能是远程基因调节以及在空间和时间上定量控制基因活性的核心。

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致谢

作者感谢 M. Levo 在整个项目过程中提供的无数次讨论和见解;感谢 X. Bing、X. Li、N. Treen、Levine 实验室的所有成员以及 J. Batut 提供的许多有益讨论和建议;感谢 W. Ke 和 P. Schedl 在 micro-C 分析方面提供的宝贵帮助;感谢 L. Mahal、E. Meagher 以及 Batut 实验室的其他成员在测试和验证果蝇品系方面提供的帮助,以及相关的讨论和建议;感谢 Levo 实验室提供显微镜的使用;感谢 E. Gatzogiannis 在显微成像方面提供的技术建议。我们还感谢普林斯顿基因组学核心设施(Princeton Genomics Core Facility)提供的高通量测序服务,以及 Lewis-Sigler 研究所的基因组计算组和哥伦比亚大学系统生物学 C2B2 计算组在高性能计算资源方面提供的帮助。资金支持:本工作得到了 NIH 资助 R35 GM118147 (M.S.L.) 和 NIH 资助 R35 GM162470 (P.J.B.) 的支持。作者贡献:概念化:P.J.B., M.L.;正式分析:P.J.B., M.L.;资金获取:M.L.;调查:P.J.B.;方法论:P.J.B.;项目管理:M.L.;资源:P.J.B., M.L.;软件:P.J.B.;监督:M.L.;验证:P.J.B., M.L.;可视化:P.J.B., M.L.;撰写——初稿:P.J.B., M.L.;撰写——审阅与编辑:P.J.B., M.L.。竞争利益:作者声明不存在竞争利益。数据、代码和材料可用性:MS2 / PP7 转录成像分析的源数据可通过 Zenodo (46) 获取。原始和处理后的 Micro-C 数据可通过 Gene Expression Omnibus (GEO) 获取,登录号为 GSE343884 (Scr-MS2 和 Scr-MS2,eRNAΔTSS 胚胎) 和 GSE171396 (yw 胚胎;数据此前已发表)。原始性梳计数可通过 Zenodo (47) 获取。用于 MS2 / PP7 数据初步处理和综合分析的自定义数据分析代码此前已发表,可通过 Zenodo (47) 获取。本研究中涉及的所有 DNA 构建体和果蝇品系可根据要求向 P.J.B. 索取。许可信息:版权所有 © 2026 作者,保留部分权利;独家许可方为美国科学促进会(AAAS)。对美国政府原始作品不主张权利。https: / www.science.org / about / science-licenses-journal-article-reuse

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补充材料

材料与方法;图 S1 至 S14;表 S1 和 S2;参考文献 (48–58);

视频 S1 至 S4;MDAR 可重复性检查清单

提交日期 2026 年 7 月 14 日;接收日期 2026 年 8 月 25 日;在线发表日期 2026 年 9 月 10 日

保护生物学

保护全球陆生脊椎动物物种免受未来海平面上升的影响

Zhong-Wen Jiang $^{1\dagger}$ , Heng-Bin Xiao $^{1\dagger}$ , Jeffrey O. Hanson $^{2}$ , Yiwen Zeng $^{3}$ , David S. Wilcove $^{4}$ , Mark Schuerch $^{5,6}$ , Matthew L. Kirwan $^{7}$ , Qin-Fang Yan $^{1}$ , Yaping Chen $^{1*}$ , Liang Ma $^{1*}$

海平面上升(SLR)威胁着陆地生物多样性,但其在时空维度上以及针对特定物种的影响仍不明确。通过将五种共享社会经济路径(SSPs)下的相对海平面上升预测与 34,120 种陆生脊椎动物的栖息地面积(AOH)图相结合,我们预测,暴露于海平面上升的物种数量将从 2050 年的最多 13,680 种增加到 2100 年的 15,324 种,其中包括 57 到 63% 的鸟类、47 到 52% 的哺乳动物、28 到 36% 的爬行动物以及 20 到 24% 的两栖动物。在东南亚,内陆淹没区域支撑着极高的物种丰富度。在 SSP5-8.5 路径下,面临 >10% 栖息地淹没的物种数量从 2050 年的 18 种激增至 2100 年的 109 种,其中爬行动物和已受威胁物种的占比过高。保护海平面上升避难所(即暴露物种的非淹没栖息地)至关重要,然而超过 96% 的避难所位于保护区之外,这意味着需要尽早采取国际行动。

陆生脊椎动物物种面临着来自气候变化的多方面威胁,包括气温升高 (1, 2)、极端高温事件 (3, 4) 以及长期干旱 (5, 6)。在这些威胁中,海平面上升(SLR)代表了一种被低估的危险,可能导致不可逆的栖息地丧失 (7, 8)。海平面上升已经通过淹没或退化关键栖息地,导致了种群崩溃和灭绝 (9–11)。荆棘凯岛巨鼠(Melomys rubicola)被宣布灭绝,海平面上升被确定为根本原因 (11)。海平面上升还通过潮汐淹没巢穴导致种群数量下降,正如在岸鸟物种和盐沼麻雀(Ammospiza caudacuta)中所记录的那样 (10, 12)。随着全球海平面上升率处于历史最高水平(>4 mm year $^{-1}$ ),且在未来几十年内可能增加到 10 mm year $^{-1}$ 以上 (7),上涨的海平面可能很快会迫使更多物种数量下降并走向灭绝。因此,迫切需要对海平面上升的影响进行系统性评估,以指导保护行动。

了解海平面上升对生物多样性的影响需要及时且具有空间明确性的信息 (13–15)。由于海平面上升表现出显著的空间和时间变异性 (16, 17),关于淹没何时以及何地可能发生的细致预测对于评估至关重要。这具有挑战性,因为特定地点的淹没受局部尺度因素的影响,例如垂直陆地运动(陆地沉降或抬升)(18) 以及区域海平面的动态变化(例如,由于不均匀的热胀冷缩)(19)。物种级别的栖息地数据(包括海拔范围和栖息地偏好)可以将广泛的地理分布细化为更精确的栖息地暴露估计 (20),从而使保护行动能够针对特定物种的风险量身定制。最后,识别海平面上升避难所——定义为能够支撑受影响物种的非淹没栖息地——可能提供一种尚未被充分利用的策略,以缓冲生物多样性的丧失 (21, 22)。

在这项工作中,我们对海平面上升(SLR)对陆生脊椎动物物种的影响进行了全球性的、针对具体物种的评估,并探讨了保护途径。我们利用栖息地面积(AOH)方法,通过将物种的生态需求与地形限制相结合,刻画了 34,120 种陆生脊椎动物(约占所有已知陆生脊椎动物的 90%)的分布 (20)。被世界自然保护联盟(IUCN)濒危物种红色名录认定为极危(Critically Endangered)、濒危(Endangered)和易危(Vulnerable)的物种被归类为受威胁物种。根据 IUCN 栖息地分类方案(版本 3.1;栖息地类型 9 至 15),我们排除了已灭绝、野外灭绝,或栖息地完全为人工或海洋的物种 (23)。对于同时栖息在陆地和非陆地栖息地的物种,仅考虑其陆地部分。

尽管所有 AOH 地图最初均以 100 米 $\times$ 100 米的分辨率生成,但为了计算可行性,我们按照推荐做法 (24–26),将 $AOH > 2 \text{ km}^{2}$ 的 32,919 个物种的地图聚合为 1 公里 $\times$ 1 公里的分辨率。通过将 AOH 地图与源自高精度相对 SLR 预测的淹没区域(已根据每个物种的空间分辨率进行统一,并考虑了特定区域的垂直陆地运动)进行叠加,我们确定了在五种共享社会经济路径(SSPs)下,到 2050 年和 2100 年风险最大的区域和物种。这些情景涵盖了从低到高的变暖程度:SSP1-1.9(到 2100 年相对于工业化前水平升高 +1.4℃)、SSP1-2.6(+1.8℃)、SSP2-4.5(+2.7℃)、SSP3-7.0(+3.6℃)以及 SSP5-8.5(+4.4℃)(26, 27)。物种特有的脆弱性是通过在每个物种原生分辨率下被淹没的栖息地比例来量化的,而基于丰富度的分析则在 1 公里 $\times$ 1 公里的网格上进行 (26)。最后,我们在物种的非淹没栖息地中绘制了 SLR 避难所地图。尽管之前的研究已经探讨了气候条件的改变如何影响物种的栖息地可用性 (3, 6, 28),但我们的研究强调,直接的 SLR 淹没是气候变化威胁陆生脊椎动物的另一条路径。

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海平面上升影响陆地脊椎动物多样性的地理格局

我们将政府间气候变化专门委员会第六次评估报告中的海平面预测 (16, 29) 与基于观测的、空间显式的垂直陆地运动(抬升或沉降)数据 (30, 31) 相结合。我们的分析表明,在 SSP2-4.5 情景下,全球沿海地区的相对海平面到 2050 年可能上升高达 0.57 m,到 2100 年可能上升 1.33 m。利用 12,148 个全球海岸线分段的潮汐机制 (17),我们将相对海平面上升的幅度转化为淹没面积。预计亚马逊河三角洲将经历最严重的陆地脊椎动物栖息地损失,到 2050 年将有 $>1000 \, km^2$ 的内陆地区被淹没(图 S1)。随着海平面上升的加速,面积损失热点从亚马逊河三角洲扩展到亚洲、欧洲和北美部分地区。

为了绘制海平面上升对陆地脊椎动物影响的地理格局,我们使用了三个指标:总物种丰富度、受威胁物种丰富度和稀有度加权丰富度。前两个指标分别捕捉每个淹没像素中的物种数量和受威胁物种数量,而稀有度加权丰富度——通过对每个物种 AOH 的倒数求和计算得出——则量化了每个像素对物种的相对重要性。在所有 SSP 情景和时间点中,亚马逊河三角洲均表现为受影响物种丰富度最高的地区(图 1, A 和 B)。这一格局反映了全球生物多样性枢纽——亚马逊盆地中广泛的海平面上升诱导面积损失 (32)。东南亚、中美洲和非洲东南部的海岸线在受影响物种丰富度方面得分也很高,反映了它们作为全球生物多样性热点的地位 (33, 34)。

海平面上升对岛屿密集地区的陆地脊椎动物影响尤为严重(图 1, C 和 D),这些地区的物种通常地理分布范围较小 (35)。岛屿拥有许多特有种 (13, 33),且其海岸线与内部的比例使得更大份额的内陆地区暴露在上涨的潮汐中。因此,即使是适度海平面上升导致的轻微栖息地损失,也会增加岛屿物种的灭绝风险。稀有度加权丰富度最高的淹没区域集中在东南亚、琉球群岛和加勒比群岛(图 1, C 和 D),这支持了岛屿物种将率先承受海平面上升冲击的预测 (7, 13, 15, 36)。与之前的研究 (14) 不同,尽管亚马逊河三角洲支持极高的物种丰富度,且预计将因海平面上升而损失大片内陆地区,但其稀有度加权丰富度较低(图 1, C 和 D),表明它并不属于分布范围受限的特有种受影响最严重的地区。

图 1. 在 SSP2-4.5 情景下,海平面上升(SLR)对陆生脊椎动物物种影响的空间格局。(A 和 B) 到 2050 年 (A) 和 2100 年 (B) 暴露于 SLR 的物种丰富度(定义为给定区域内存在的物种数量)。(C 和 D) 到 2050 年 (C) 和 2100 年 (D) 暴露于 的稀有度加权丰富度。该指标代表了一个区域对所有其所支撑物种的累积重要性,计算方式为该区域内发现的所有物种总栖息地倒数之和。(E 和 F) 在预测的 NIH 下,到 2050 年 (E) 和 2100 年 (F) 的受威胁物种丰富度。该指标表示在给定的淹没区域内,目前根据 IUCN 威胁状态被分类为受威胁的物种数量。暴露于 的物种定义为:栖息地被淹没面积至少为 $1\mathrm{km}^2$,或者对于总 $\mathrm{AOH} \leq 2\mathrm{km}^2$ 的物种,淹没面积 $\geq 0.01\mathrm{}^2$。本图显示了中等 情景 (SSP2-4.5) 的结果。其他 SSP 的结果和特定分类群的模式见图 S10 至 S33。结果保留了原始的 1--by-1- 分辨率,但为了全球可见度,在不改变地理坐标的情况下放大了绘制的点。

东南亚及其周边岛屿在所有三项指标中均显示为令人担忧的区域(图 1),其淹没区域拥有大量受威胁物种(图 1, E 和 F)。在 SSP2-4.5 情景下,马来半岛、婆罗洲和苏门答腊的淹没像素所支撑的受威胁物种数量平均几乎是世界其他地区的三倍,该比例从 2050 年的 2.82 增加到 2100 年的 2.87 ($W = 5.83亿$ , $P < 0.001$;具体分类群模式见补充文本 1.1)。因此,尽管东南亚预测的淹没面积小于亚马逊河三角洲和北美南部(图 S1),但其卓越的生物多样性(包括许多分布范围受限和受威胁的物种)使其极易受到 的影响(图 1, C 至 F)。本研究中确定的某些极易受 影响的区域,如婆罗洲和菲律宾群岛,在使用物种-面积关系 (15) 时被低估了。

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物种特有的海平面上升(SLR)暴露度与脆弱性

我们评估了四个陆生脊椎动物类群以及六种 IUCN 威胁状态(极危、濒危、易危、近危、无危和数据缺乏)下,物种特有的 SLR 暴露度和脆弱性。我们首先使用绝对栖息地损失阈值来识别暴露于 SLR 的物种:淹没面积 $\geq1~km^{2}$ 的 AOH,或对于总 AOH $\leq2~km^{2}$ 的物种,淹没面积 $\geq0.01~km^{2}$。我们这样做是因为小型栖息地碎片往往对物种和遗传多样性有不成比例的贡献 (37),且许多物种在关键生命阶段 (38) 依赖于易受 SLR 影响的小型栖息地 (10)。随后,物种特有的脆弱性被量化为每个物种 AOH 被淹没的比例。绝对阈值可防止分布范围较大的物种在数学上稀释广泛分布物种的栖息地损失 (39),而比例淹没则使脆弱性标准化 (40)。

在中间情景 SSP2-4.5 下,到 2050 年有 13,511 种陆生脊椎动物暴露于 SLR,到 2100 年这一数字增加到 14,831 种(图 2)。在所有 SSP 情景中,暴露物种的数量在 2050 年为 13,308 至 13,680 种,在 2100 年为 14,325 至 15,324 种。其中包括 20% 至 24% 的两栖类(2050 年为 1540 至 1587 种;2100 年为 1683 至 1844 种)、28% 至 36% 的爬行类(2050 年为 2779 至 2900 种;2100 年为 3129 至 3551 种)、57% 至 63% 的鸟类(2050 年为 6225 至 6356 种;2100 年为 6559 至 6835 种)以及 47% 至 52% 的哺乳类(2050 年为 2764 至 2837 种;2100 年为 2954 至 3094 种)。尽管预测 SLR 对鸟类和哺乳类的影响比例高于两栖类或爬行类,但后两组受影响的物种,尤其是爬行类,其平均比例栖息地损失将几乎是鸟类和哺乳类的两倍(图 2 和图 S2)。

因 SLR 而损失大量栖息地的物种可能需要保护干预。为了识别此类物种,我们采用了 10% 的栖息地损失阈值,因为此类栖息地损失可能与遗传多样性的降低相关,而遗传多样性的恢复可能需要数千年时间 (41)。在 SSP5-8.5 情景下,预计到 2050 年有 18 种物种将损失 $>10\%$ 的 AOH,到 2100 年这一数字将增加到 109 种,其中包括 13 种两栖类、58 种爬行类、27 种鸟类和 11 种哺乳类。其中,预计有 32 种物种将损失 $>20\%$ 的 AOH(图 S2 和表 S1)。在 SSP5-8.5 情景下,预计到 2100 年,蠕蜥 (Amphisbaena littoralis)、卡塔利娜chuckwalla (Sauromalus klauberi) 和 Restinga 蟾蜍 (Melanophryniscus setiba) 将损失 $\sim50\%$ 的栖息地(表 S1)。虽然鸟类在 SLR 下的总栖息地损失较低,但当分别分析繁殖地、非繁殖地和常驻栖息地时,迁徙物种的关键脆弱性便显现出来。例如,尽管在 SSP5-8.5 下, ferruginous duck (Aythya nyroca) 的总栖息地淹没比例仍 $<1\%$,但在 SSP2-4.5 下,其常驻栖息地的淹没比例从 2050 年的 17% 增加到 2100 年的 38%(表 S1)。

被 IUCN 认定为受威胁的陆生脊椎动物物种可能会受到 SLR 的不成比例影响,其平均栖息地损失比例估计是无危物种的 5 倍,在不同 SLR 情景中范围为 2 到 10 倍 (W = 5.34亿, P < 0.001)。这与预测的岛屿限制物种的损失一致 (15),表明受威胁物种对 SLR 的不成比例脆弱性并不局限于岛屿生态系统,而是全球陆生脊椎动物普遍存在的现象。

图 2. 在 SSP2-4.5 情景下,不同物种对海平面上升(SLR)影响的特异性脆弱性。(A 和 B) 展示了四个陆生脊椎动物类群 (A) 和六种 IUCN 威胁状态 (B) 中,每个物种被 SLR 淹没的实际分布范围(AOH)比例($P_{\text{inundated}}$)的分布情况,分别对应 2050 年(左列)和 2100 年(右列)的 SLR。 (A) 中从上到下呈现的四个陆生脊椎动物类群依次为两栖类、爬行类、鸟类和哺乳类。同样,(B) 中从上到下显示的六种 IUCN 威胁状态是指极危 (CR)、濒危 (EN)、易危 (VU)、近危 (NT)、无危 (LC) 和数据缺乏 (DD)。红色虚线标志着 1% 的栖息地被淹没,平均值代表该类群估计的栖息地淹没平均比例($P_{\text{inundated}}$),$n$ 表示该类群中的物种数量。$P_{\text{inundated}} > 1\%$ 的物种被纳入避难所分析。其他 SSPs 的结果见图 S34 至 S37。请注意,$x$ 轴经过 $\log_{10}$ 转换以适应高度偏斜的数据分布,且轴刻度标签显示未转换的比例值以方便解读。动物剪影图像来源于 PhyloPic (https: / www.phylopic.org / )。

栖息地淹没与总 AOH 呈负相关,表明分布范围狭窄的物种比例损失更大。这种关系在爬行类以及被分类为数据缺乏、濒危或极危的物种中尤为强烈(图 S3 和 S4)。

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SLR 避难所

随着海平面上升(SLR),受淹没影响的物种预计将退缩到其剩余的未淹没栖息地中 (42, 43)。我们在预计因 而损失 $>1\%$ AOH 的物种(以下称为受影响物种)的未淹没 AOH 中识别了 SLR 避难所,该阈值在保护框架中被广泛采用 (26, 44, 45)。 SLR 避难所被定义为前 10% 的未淹没像素,这与定义避难所常用的 10% 阈值一致 (45, 46),并使用三个互补的指标进行排名 (26):所支持的受影响物种总数、所支持的受影响受威胁物种数量,以及所支持物种的栖息地淹没比例总和(图 S5)。第三个指标突出了支持那些因 而栖息地损失更严重物种的未淹没像素。

我们为 2050 年识别的 SLR 避难所中,仅有 0.5% 位于现有的保护区内(表 S2)。尽管各国已承诺根据昆明-蒙特利尔全球生物多样性框架(GBF)的目标 3,在 2030 年前保护 30% 的陆地面积 (47),但仍需取得实质性进展 (48)。在大多数国家,避难所的保护区覆盖率也很低。在 SSP2-4.5 情景下,缅甸、斐济、马达加斯加和巴西的 SLR 避难所覆盖率均 $<1\%$。相反,新西兰、古巴、日本和西班牙在几乎所有 情景下的覆盖率均 $>30\%$。通过将当前的国家保护区覆盖率与国家层面的未保护避难所比例进行比较(图 S6)(26),我们的分析表明,缅甸、越南和印度尼西亚等国家可以通过增加对 SLR 避难所的保护,在保护生物多样性免受 影响的同时,向 30% 的保护区覆盖率目标迈进(图 S6)。

预计的 SLR 避难所在时间上呈现出动态的空间模式。由于 避难所是基于物种剩余的未淹没栖息地定义的,随着 影响到更多物种,最初识别的避难所可能会扩大,新的避难所也可能会出现。在 SSP2-4.5 情景下,到 2050 年仅缅甸和澳大利亚拥有 避难所,到 2100 年这一数字将增加到 26 个国家(图 3A,深红色,以及图 S7)。避难所的地理模式在四个分类群之间有所不同,详细分析见补充文本 1.2。基于 避难所总面积的国家排名在低至中度 情景(SSP1-1.9 和 SSP1-2.6)中相对一致,但在更严重的情景(SSP2-4.5 到 SSP5-8.5)下有所不同。例如,预计到 2100 年,在中国低至中度情景下的 SLR 避难所面积相对较小,但在最坏情况情景(SSP3-7.0 和 SSP5-8.5;图 S7)下,中国位列避难所面积最大的国家之列。这些特定于时间和情景的预测可以通过分阶段的避难所策略来指导保护区的扩张和土地利用规划——优先保护到 2050 年出现的避难所,同时制定计划并为随着 加剧而逐渐变得重要的区域分配资源。

图 3. SSP2-4.5 情景下全球 避难所的空间模式。(A 和 B) 深红色表示根据预测的 SLR 在 2050 年 (A) 和 2100 年 (B) 在全球范围内识别的 SLR 避难所位置。 SLR 避难所是指在三个指标中同时排名前 10% 的未淹没区域:所支持物种的栖息地淹没比例总和(记作 P)、所支持的受影响受威胁物种数量 (T) 以及所支持的受影响物种总数 (R)。该分析针对所有至少有 1% AOH 因 而损失的物种进行。其他 SSP 的结果和特定分类群的模式见图 S37 至 S61。

许多海平面上升(SLR)避难所,包括那些位于东南亚和南美洲中西部的避难所,在空间上与公认的全球生物多样性热点地区(34, 49)以及陆地保护优先区域(50)相一致,但许多避难所则分布在这些区域之外。例如,中国东部沿海和俄罗斯北部海岸线在很大程度上被忽视,未被列为保护优先区,但预测显示这些地区拥有在严重海平面上升情景下会扩大的 SLR 避难所(图 3 和图 S7)。同样,尽管预计泰国将拥有广泛的 SLR 避难所(图 3)且与生物多样性热点地区重叠(34, 49),但其被指定的保护优先级仍然较低(50)。总之,这些发现凸显了通过保护 SLR 避难所来实现全球生物多样性框架(GBF)目标的潜力,同时也揭示了传统保护优先级与新兴的气候驱动脆弱性之间的不匹配。

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影响

我们的研究结果揭示了气候变化对全球生物多样性的多维度影响,并指出了有针对性保护的关键位置。到 2100 年,约 45% 的所有研究物种可能会受到海平面上升(SLR)的影响,然而在 IUCN 红色名录中,仅有 $5.9\%$ 的受影响物种被标记为面临气候相关威胁(补充文本 1.3)。这些发现对于帮助各国实现昆明-蒙特利尔全球生物多样性框架(GBF)目标具有重要意义。首先,在大多数国家,SLR 避难所的保护区覆盖率较低,这表明在目标 3 下的保护区扩张应提高对 SLR 避难所的覆盖。其次,目标 1 下的综合规划应考虑 的影响,以避免失去那些对生物多样性将变得日益重要的区域。第三,对于预计将因 而失去大部分栖息地的物种,为了在目标 4, 下防止灭绝,战略性的栖息地修复和迁地保护可能是必要的,先前的恢复工作已证明了这一点 (51-54)。总体而言,在目标 8 下最大限度地减少 的影响并增强其韧性——以及应对其他气候变化影响——对于实现 GBF 下的多个政策目标至关重要 (47)。

的影响在空间上和物种之间具有高度的异质性。在受 威胁的地区——例如亚马逊地区(那里的青蛙还面临着日益严重的干旱 (6))、加勒比海等岛屿系统以及美国南部——陆生脊椎动物预计还将面临更高的过热风险 (3, 28)。在分类群中,爬行动物可能对气候变化尤为脆弱,本研究以及此前针对岛屿的研究 (13) 所识别的 SLR 诱导的栖息地丧失,以及它们对极端高温事件的高暴露度 (3) 证明了这一点。与之前的评估 (15) 相比,我们的评估表明,到 2100 年,因 而失去全部栖息地的物种数量可能较少。例如,在 SSP5-8.5, 情景下,预计只有 3 个物种将失去约一半的栖息地,而在全球统一 1 米 情景下,预测有 37 个物种将失去所有栖息地,且其灭绝推论是基于广义面积损失-物种损失比例假设 (15)。这种差异部分是因为我们的研究考虑了 SLR 的空间动态变化。即使在 SSP5-8.5, 情景下,到 2100. 预计的全球平均相对 SLR 为 $\$0.80 \pm 0.22$ 米,尽管局部数值可能达到 $1.54$ 米。此外,我们通过将预测的淹没区域与单个 AOH(分布范围)地图相交,直接估算了特定物种的栖息地暴露情况。虽然很少有物种可能因 而失去所有栖息地,但许多物种可能会失去足够的栖息地,从而影响其长期生存。

将高精度的相对海平面上升(SLR)预测与物种特有的 AOH 数据相结合,可为生物多样性风险评估和保护规划提供更细致的见解。然而,细粒度的物种级分析仍受限于底层数据产品的不确定性。例如,用于评估淹没区域的数字高程模型产生于十年前 (55)。尽管它提供了垂直不确定性较低且全球一致的可靠地形,但单一的地形快照无法反映沿海景观不断变化的特性。另一个局限性是我们评估的是全分布范围的物种级影响,而许多保护规划是在国家尺度上进行的,或侧重于亚种和种群 (56–58)。例如,尽管从物种层面看,老虎(Panthera tigris)受 SLR 的影响似乎极小,其栖息地淹没比例 $<0.05\%$,但预计孟加拉亚种(P. t. tigris)将在几十年内失去近一半的栖息地 (59)。我们排除了完全的海洋物种,对于依赖海岸的物种,仅考虑 AOH 地图所捕捉的陆地栖息地组成部分。然而,包括 Scolopacidae 科和 Charadriidae 科的迁徙涉禽在内的许多物种,依赖潮间带进行觅食和繁殖 (10, 60, 61);因此,本研究未能捕捉到它们面对 SLR 的全部暴露情况。此外,我们的研究仅关注渐进式 ,未考虑日益增加的盐雾 (62)、增强的风暴潮 (63, 64) 以及加剧的飓风 (64),这些因素可以将盐水带到更远的内陆,并在常规潮汐淹没之前破坏陆生脊椎动物的栖息地。因此,我们的研究代表了 SLR 对陆生脊椎动物影响的一个保守估计。

需要尽早采取协调一致的国际行动,以减轻 对生物多样性的影响。这对于低收入和中等收入国家尤为重要,因为有限的资金能力和紧迫的发展需求使得延迟保护的成本日益增加 (21, 22, 52, 65–68)。由于许多国家在保护 避难所方面可能资金有限(补充文本 1.4),提供资金和技术援助的国际政策可能有助于保护 避难所。此类努力应考虑国家财富的差异和当地的社会文化背景 (69)。虽然沿海防洪屏障对于保护人类发展至关重要 (70),但它们不太可能完全减轻

生物多样性框架”(联合国环境规划署,报告 CBD / COP / DEC / 15 / 4, 2022);https: / www.cbd.int / doc / decisions / cop-15 / cop-15-dec-04-en.pdf。

对陆生脊椎动物的影响。我们的敏感性分析表明,这些屏障可以降低某些内陆物种的预计暴露程度,但其效果在空间上有所不同,且随时间而减弱(补充文本 1.5 以及图 S8 和 S9),并可能加剧海岸挤压或破坏生态连通性 (17, 71, 72)。因此, SLR 避难所在整个 21 世纪支持受 影响的物种方面可能会发挥重要作用。由于许多避难所位于生物多样性热点地区 (34) 或保护优先区 (50, 73) 之外,它们在保护规划中可能会被忽视。系统性的保护规划可以基于我们的发现,在考虑不同 情景下的栖息地动态和不确定性的同时,确定保护 避难所的优先区域 (74)。我们的研究结果强调了保护 避难所对于在 GBF 目标 8 下建立韧性并维护生物多样性的重要性,从而有助于实现更广泛的生物多样性目标。

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致谢

我们感谢 C. Mi 提供的评论以及 R. Liu 在数据准备方面提供的帮助。资金支持:本研究得到了中国教育部基础学科交叉突破计划 JYB2025XDXM902 (Z.-W.J., L.M., Y.C., 和 H.-B.X.);中国国家自然科学基金 32330067 (Z.-W.J. 和 L.M.);中国国家自然科学基金 32501390 (Z.-W.J.);中国国家自然科学基金 32570593 (L.M.);中山大学中央高校基本科研业务费 24hytd014 (L.M.);中国国家自然科学基金 42501094 (Y.C.);中山大学中央高校基本科研业务费 24hytd012-2 (Y.C.);加拿大自然科学与工程研究委员会 (NSERC) (J.O.H.);以及加拿大环境与气候变化部 (ECCC) (J.O.H.) 的支持。作者贡献:

概念化:Z.-W.J., L.M., H.-B.X., Y.C.;数据整理:Z.-W.J., J.O.H., M.S.;资金获取:L.M., Y.C., Z.-W.J., H.-B.X.;调查:Z.-W.J., L.M., H.-B.X., Y.C., Q.-F.Y.;方法论:Z.-W.J., L.M., H.-B.X., Y.C., J.O.H., Y.Z.;项目管理:Z.-W.J., L.M., Y.C.;监督:L.M., Y.C.;可视化:Z.-W.J., H.-B.X.;初稿撰写:Z.-W.J., L.M., H.-B.X., Y.C.;审阅与编辑:Z.-W.J., L.M., H.-B.X., Y.C., J.O.H., Y.Z., D.S.W., M.S., M.L.K., Q.-F.Y.。竞争利益:作者声明不存在竞争利益。数据、代码和材料可用性:到 2100 年的全球海平面预测获取自 Zenodo (https: / zenodo.org / records / 6382554) (29)。数字高程模型源自 NASA 航天飞机雷达地形任务 (SRTM) 数据集 (https: / srtm.csi.cgiar.org) (55)。哺乳动物和鸟类的 AOH 地图可在 Dryad (https: / datadryad.org / dataset / doi:10.5061 / dryad.02v6wwq48) (75) 获取,而两栖动物和爬行动物的地图是使用 "aoh" R 软件包 (76) 基于 IUCN 红色名录 (https: / www.iucnredlist.org / resources / spatial-data-download) (23) 的分布范围数据生成的。本文产生的所有数据和代码均可在 Dryad (77) 获取。本研究未创建新材料。许可信息:版权所有 © 2026 作者,保留部分权利;独家许可方为美国科学促进会。不对美国政府原始作品主张权利。https: / www.science.org / about / science-licenses-journal-article-reuse

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补充材料

材料与方法;补充文本;图 S1 至 S62;表 S1 和 S2;

参考文献 (78–111);MDAR 可重复性检查清单

2025 年 11 月 2 日提交;2026 年 3 月 21 日重新提交;2026 年 8 月 26 日接收;2026 年 10 月 8 日在线发表

天然产物

植物和细菌中胍基异戊烯基转移酶的天然产物生物合成

Dominik Kolling $^{1,2}$ , Katharina Konzok $^{3}$ , Daghan Taser $^{4}$ , Tom Jentsch $^{4}$ , Svenja Schwoerer $^{4}$ , Henry Struwe $^{4}$ , Arne Bültemeier $^{5,6}$ , Jonas Freiberg $^{7}$ , Claus-Peter Witte $^{7}$ , Jakob Franke $^{5,6}$ , Andriy Luzhetskyy $^{2,8}$ , Andreas Kirschning $^{4,9}$ , Sophia Rudorf $^{3*}$ , Jesko Koehnke $^{1*}$

胍几乎完全以共振稳定阳离子的形式存在,这使得其直接的酶促功能化具有挑战性。我们鉴定出蓝细菌酶 NosH,该酶可催化异戊烯基直接转移至游离胍。结构和机制分析揭示,通过一种独特的催化架构,由两个天冬氨酸夹钳激活胍并与异戊烯基供体结合。在这些特征的指导下,我们在细菌和植物中鉴定出一个庞大的胍基异戊烯基转移酶家族。植物酶在体外产生了如 galegine 等胍类生物碱,且在烟草(Nicotiana benthamiana)中异源表达一种植物同源蛋白可在植体内产生 galegine,从而为植物特有代谢提供了直接的酶促联系。

在生理条件下,胍(Gua, 1)是自然界中最强的碱之一,几乎完全以共轭稳定阳离子的形式存在。胍在生命的不同分支中都是一种重要的生物代谢物 (1)。有机胍衍生物是治疗心血管疾病、感染和 II 型糖尿病药物的核心 (2–7)。胍存在于哺乳动物的尿液中,而包括蓝细菌在内的细菌利用游离胍作为氮源 (8–11)。

在特有代谢中,初级代谢物被重新利用以构建复杂的天然产物。特别是植物,会产生含有胍的生物碱,如 galegine (2) (12–14),这启发了二甲双胍 (3) 的开发,后者是全球使用最广泛的抗糖尿病药物(图 1A)(15, 16)。然而,尽管在药理学上具有超过一个世纪的相关性,但 galegine 以及植物代谢物 pterogynine (4) 和 nitensidine (5) 中胍掺入的生物合成来源仍然是一个谜。

源自胍的天然产物在细菌中也被发现,包括 gromomycin (6)、cybastacine (7) 和 zillamycin (8)(图 1A 和图 S1)(17–20)。在如 saxitoxin (S48) 和 stylissadine (S49) 等研究充分的毒素的生物合成中,脒转移酶降解精氨酸,并仅转移其胍基的一部分 (21–24)。在 autumnalamide A (S63) 或 argicyclamide A (S64) 等天然产物中,ABBA-fold 异戊烯基转移酶将异戊烯基链附加到精氨酸或亚精胺(agmatine)的胍基上,从而调节溶解度、稳定性和生物活性(图 S1)(25–27)。然而,这些已知的胍基异戊烯基转移酶作用于嵌入在较大天然产物骨架中的胍基。尚未证明异戊烯基可直接转移至游离胍,且除了降解之外,尚未建立游离胍酶促功能化的机制。

在此,我们鉴定并表征了 NosH,这是一种蓝细菌胍基异戊烯基转移酶,可催化游离胍的直接异戊烯基化。结构分析揭示了一种独特的活性位点架构,该架构通过一个疏水沟槽激活胍并容纳多种异戊烯基供体。在这些结构特征(而非仅凭序列一致性)的指导下,我们在植物和细菌中发现了一个庞大的胍基异戊烯基转移酶家族,并证明了选定的植物酶在体外和植体内产生 galegine 的能力。

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NosH 催化游离胍的直接异戊烯化

最近发现的一类名为 gromomycins 的含胍次级代谢产物揭示了独立于脒转移酶运行的生物合成机制(图 S2 和表 S1)(17)。对相应生物合成基因簇 (BGC) 的分析表明,其编码的酶 GroH 通过一种涉及精氨酸修饰及随后环化的异常反应机制,催化精氨酸与异戊烯供体六异戊烯基二磷酸 (HePP; S6) 形成 gromomycin 中间体六异戊烯基 / C$_{30}$-胍 (zillamycin; 8)。然而,GroH 的活性是从代谢组学数据中推断出来的,尚未通过体外生化重组得到证实,部分原因是生化表征受限于酶的溶解度较低。

为了克服这些限制,我们在来自 *Nostoc flagelliforme* CCNUN1 的相关推测萜类 BCG 中鉴定出一种蓝藻同源酶 NosH(图 1B,图 S3,以及表 S2 和 S3)。重组表达的 NosH 仅显示出极少量的 FPP (9) 与 L-精氨酸 (Arg, 10) 或精胺 (Agm, 11) 转化为 C$_{15}$-异戊烯化衍生物 (12 和 13) 的转化率,这促使我们考虑游离胍是否可以作为底物(图 S4)。这一假设得到了 NosH 相关 BGC 附近存在与胍代谢相关基因的支持,以及最近在 *N. flagelliforme* CCNUN1 中证明的一种由胍特异性核糖开关控制的分解代谢途径的支持(图 S5 和表 S4)(11)。

NosH 催化了游离胍与 FPP (9) 之间的一项 $Mg^{2+}$ 依赖性反应,产生法尼基胍 (14, $[M+H]^{+}_{obs.}=264.2427$ Da, $[M+H]^{+}_{calc.}=264.2434$ Da, $\Delta ppm-2.65$ ),该结果随后通过核磁共振 (NMR) 分析得到了进一步确认(图 1℃,图 S6 至 S10,以及表 S5)。在初始速率条件下,使用纯化的 14 作为定量外部标准进行的时间进程实验得出,胍的 $K_{M}$ 为 $1.00\pm0.39$ mM,$k_{cat}$ 为 $2.59\pm0.18$ min$^{-1}$(图 1D 和图 S11)。

接下来,我们使用链长递增的类异戊二烯二磷酸考察了 NosH 的异戊烯供体范围:异戊烯基二磷酸 (IPP; S1)、二甲基烯丙基二磷酸 (DMAPP; S2)、香叶基二磷酸 (GPP; S3)、香叶基香叶基二磷酸 (GGPP; S4)、五异戊烯基二磷酸 (PePP; S5) 和 HePP (S6)。NosH 要求供体链长至少为 $C_{10}$,且可接受至少高达 $C_{30}$ 的供体,从而产生相应的胍基化多异戊烯基 15-17 和 zillamycin (8)(图 1E 和图 S12 至 S15)。这种广泛的供体耐受性将 NosH 与典型的 ABBA 折叠异戊烯转移酶区分开来,后者仅限于短链供体 ($C_{5}$ 至 $C_{10}$) (28)。计算机模拟提出 NosH 类蛋白参与胍基修饰途径 (20),且蓝藻同源酶 ScAer3 能将 DMAPP 转移至精胺的胍基 (11),但尚未报道其对游离胍的活性 (29)。

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NosH 催化游离胍异戊烯化的结构基础

为了确定胍异戊烯化的结构基础,我们测定了 NosH 的 apo 结构和配体结合结构(图 S16 至 S22 和表 S6)。NosH 形成一个同源二聚的 $\alpha4-\alpha4$ 桶状结构,该结构在结构上与 I 类萜烯合酶相关,且与 ABBA 折叠异戊烯转移酶不同 (30, 31)。与典型的 I 类酶不同,NosH 包含一个反向的 DDxxD 基序(残基 176 至 183,NDFIDYADD),它以一种独特的几何构型协调 $Mg^{2+}$ 和异戊烯二磷酸。活性位点将一个双天冬氨酸胍结合夹(Asp140 和 Asp172)与一个疏水通道相结合,该通道在异戊烯供体结合时开启成一个沟槽,这与生化实验中观察到的 $C_{10}$ 至 $C_{30}$ 的宽供体范围一致。

A

B

C

D

E

图 1. NosH 催化游离胍的异戊烯化。(A) 含有异戊烯化胍基的代表性细菌和植物天然产物,以及受天然产物启发的合成药物二甲双胍 (3)。(B) 来自 Streptomyces sp. Je 1-332 的 gromomycin 生物合成基因簇 (BGCs) 以及来自 Nostoc flagelliforme CCNUN1 且包含 NosH 的相关基因簇。(C) NosH 与法尼基二磷酸 (FPP; 9) 以及胍 (1)、L-精氨酸 (Arg; 10) 或 凝胺 (Agm; 11) 的体外反应。提取离子色谱图 (EICs) 显示形成了法尼基胍 (14) 以及痕量的法尼基 L-Arg (12) 和 Agm (13)。(D) 使用 $1\mu \mathrm{M}$ 或 $0.1\mu \mathrm{M}$ NosH 的胍异戊烯化时间曲线,以及使用 FPP 和不同胍底物浓度的 Michaelis-Menten 分析。数据代表独立生化反应的平均值 $\pm$ 标准差 ( $n = 3$ )。(E) 使用不同链长的类异戊二烯二磷酸测试 NosH 的异戊烯供体范围。$\mathrm{C}_{10}$ 至 $\mathrm{C}_{30}$ 的供体均被接受,从而实现了 zillamycin (8) 生物合成的体外重建。部分图表使用 BioRender 创建。

分辨率为 2.10-Å 的三元结构(包含胍、$Mg^{2+}$ 和不可水解的 FPP 类似物法尼基 S-硫代二磷酸 [(FSPP)18])捕捉到了活性位点中的反应伙伴(图 2, A 和 B,以及图 S23 和 S24)。胍由 Asp140 和 Asp172 锚定,而 FSPP 的二磷酸通过 $Mg^{2+}$ 与反向 DDxxD 基序相互作用而协调,其异戊烯链占据疏水沟槽。与 apo 结构和 FSPP 结合结构的比较表明,胍的结合破坏了 Arg137-Asp176 盐桥,并使 Arg137 向胍结合位点重新定位。在三元复合物中,Arg137 位于胍和 FSPP C-1 碳之间,两者相距 4.7 Å。这些结构定义了底物结合的几何构型,并确定了 Asp140 / Asp172 夹和

Arg137 构象开关是连接胍识别与异戊烯供体定位的关键特征。

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NosH 机制与底物识别

在结构数据的指导下,我们进行了定向诱变以探究 NosH 的催化机制(图 S25 和 S26)。我们首先检查了胍结合残基 Asp140 和 Asp172。保守的 Asp140Asn 突变使周转率降低了约 15%(本节中所有数值均将突变体活性与野生型 进行比较),而 Asp140Ala 则使活性完全丧失。由于胍是由两个 Asp 残基结合的一价阳离子,预计其中一个 Asp 残基主要参与氢键结合,而另一个形成盐桥;我们的数据表明 Asp140 承担前者角色。Asp140 与 Glu52 形成氢键,这种相互作用在 Asp140Asn 变体中得以保留,可能对其残余活性有所贡献。Glu52 本身是可有可无的,因为 Glu52Gln 和 Glu52Ala 保留了近乎完整的活性(分别为 88% 和 99%)。相比之下,Asp172 上的负电荷被证明是不可或缺的:Asp172Asn 和 Asp172Ala 没有活性,而保守的 Asp172Glu 变体保留了 93% 的活性,这与同源物之间的序列变异一致。

A

图 2. 三元复合物定义了 BGC 中的底物结合。(A) 与不可水解的 FPP 类似物法尼基 S-硫代二磷酸 (FSPP; 18)、胍 (1) 和 $Mg^{2+}$ 的三元复合物。FSPP 的二磷酸基团由 $Mg^{2+}$ 稳定,而异戊烯基链结合在疏水槽中并通过疏水相互作用参与结合。18 的 $F_{O}-F_{C}$ 电子密度图显示为等值面网格,等值线设为 $3\sigma$。(B) 活性位点的放大图。胍由 Asp140 和 Asp172 协调,而 Arg137 重新定位在胍与 FSPP 的 C-1 原子之间。虚线代表盐桥和氢键;距离以 Å 为单位。

Arg137 成为一个关键残基(图 S27)。在结合胍的结构中,其胍基位于底物附近,而在结合 FSPP 的复合物中,Arg137 与 Asp176 形成盐桥,从而使异戊烯类供体能够对齐以进行异戊烯基转移。在三元复合物中,Arg137 向胍方向重新定向,取代了异戊烯基 C-1 碳。因此,我们提出 Arg137 在两种状态之间切换:一种定位在胍附近,另一种与 Asp176 结合。Arg137 带正电的侧链可能会降低胍底物的 $pK_{a}$,并促进 Asp172 对胍的激活。与 Asp176 的盐桥可能会防止与 FPP 结合产生空间干扰。仍能降低胍底物 $pK_{a}$ 的突变体(Arg137Lys 和 Arg137Met)保留了活性,而具有短侧链(Arg137Ala)或大体积侧链(Arg137Leu)的突变体则受损。Arg137-Asp176 相互作用的重要性得到了 Asp176Asn(几乎没有活性)和 Asp176Glu(保留 67% 活性)的进一步支持。因此,我们提出 Arg137 和 Asp172 促进胍的去质子化及其转化为异戊烯基转移的亲核试剂(图 3A 和图 S28)。质子是直接传递给二磷酸基团还是通过 Asp176 传递,目前尚未解决。

的同源物 AgdT 和 AgdS 此前在计算机模拟中被注释为蓝藻 aeruginoside (S15) 和 microguanidine (S16 和 S17) BGCs 的组成部分,尽管其功能尚未得到验证 (20)。最近表征的 ScAer3 将 DMAPP 转移至精胺,但据报道并不使用游离胍,现在可以将其视为更广泛的 BGC 类胍异戊烯基转移酶谱系的一部分 (29)。 BGC 与这些使用精胺 / 精氨酸的酶之间的主要区别在于残基 Asn175,后者在这些酶中对应于 Asp(图 S29)。 BGC 中该残基的突变(Asn175Asp,以下简称为 $\mathrm{}^{\mathrm{RP}}$)扩大了底物特异性,使其除了胍之外还能接受精胺和精氨酸(图 3B 和图 S30、S31)。

为了阐明这一变化,我们确定了 NosH $^{RP}$ 与 Arg (10) 复合物的 1.85-Å 晶体结构(图 3℃ 和图 S32)。胍基在 NosH 活性位点中占据与游离胍相同的位置,而 Arg 的其余部分则采取两种替代构象:在一种构象中,Arg 的羧基与来自结晶条件的 Ca $^{2+}$ 离子配位,并且会与异戊烯基供体发生碰撞,这表明该状态是结晶的人为产物。在第二种构象中,$\alpha$-氨基与 Asp175 形成盐桥,并且与 FPP 的结合相兼容。因此,该结构为 Asn175Asp 如何在不改变反应性胍基位置的情况下实现对扩展的含胍底物的识别提供了理论依据。

$^{RP}$ 还能容纳更长的异戊烯类链且无明显长度限制,能以极高的转化率产生衍生物 12, 13, 19, 20 以及 S65 至 S70(图 S33 至 S37)。其效率的提升使我们能够检测额外的精氨酸类似物(图 3D 和图 S38 至 S41)。胍基乙酸 (21) 和胍基丁酸 (S73) 被转化为其法尼基化产物 (22 和 S74),其产率超过了精氨酸。L-同精氨酸 (23) 和 L-精氨酸 O-甲基酯 (25) 同样被接受(产生 24 和 26),而胍基本身的修饰,例如 L-canavanine (27, S77, S78) 中的修饰,则是有害的,这可能是由于静电特性的改变或空间位阻所致。 $^{RP}$ 对 L- 和 D-精氨酸 (10 和 28) 均能进行异戊烯基化,尽管 L-形式更受青睐(图 S41)。

最后, BGC 异戊烯类结合槽的结构表明其与非天然 FPP 类似物 (32–35) 具有兼容性。 BGC 和 $^{RP}$ 接受了五种测试的合成 FPP 衍生物中的三种 (30 至 32, S7 和 S8),产生了异戊烯基化产物 33 至 35 以及相应的 L-精氨酸和精胺衍生物 S83 至 S86(图 3E 和图 S42 至 S46)。带有改变的双键位置或大体积取代基的底物不被接受,这与活性位点的空间和几何约束一致。其中一个被接受的类似物具有一个末端烯丙基,提供了一个化学可寻址的柄,突显了 BGC 衍生酶在选择性胍基功能化方面的潜力。

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植物中 NosH 同源物的结构引导发现

植物中含有胍基的天然产物(如 galegine (2))的出现,引发了人们对自然界在细菌之外是否也采用了类 NosH 胍基异戊烯基转移酶的疑问(图 S47)。针对植物酶数据库的标准 BLAST 搜索在最高匹配项中识别出了我们将其分类为推测性胍基异戊烯基转移酶的蛋白质;然而,它们与 FSPP 的序列一致性通常低于 30%,这使得仅凭序列相似性难以进行可靠的功能分配。因此,我们利用结构洞察,将 FSPP 活性位点的三维架构定义为酶发现的高级描述符,并开展了由 Chai-1 生成的结构模型 (36) 支持的结构引导、基于基序(motif)的搜索。具体而言,对 FSPP 晶体结构的仔细分析识别出一个诊断性的 R / KxxD 基序,以及一个处于固定间距的第二个酸性残基 (R / KxxD / Ex $_{31}$ D / E),作为胍基配位的特征。这一刻意设定的严格复合基序作为候选识别的主要序列级过滤器,使我们能够排除具有相关折叠但缺乏 -胍基识别架构的酶,例如 I 类萜烯环化酶。

A

B

C

D

E

图 3. 的机制与底物重编程。(A) 拟议的催化机制。Asp140 / Asp172 夹钳对胍基进行定位并激活,使其对 FPP (9) 的 C-1 位进行亲核攻击,同时伴随焦磷酸的离去和质子化。精确的质子转移路径尚未明确。(B) 将 Asn175 替换为 Asp $(\mathrm{}^{\mathrm{RP}})$ 扩大了受体特异性,使其除了游离胍之外,还能利用精氨酸和精胺。(C) $\{}^{\{RP}}$-L-精氨酸复合物(蓝色表面)与 -胍复合物(绿色棒状模型)的叠加。与 FPP 结合兼容的 L-精氨酸构象以橙色显示;另一种 $\{Ca^{2+}}$ 配位构象以黑色棒状模型显示。活性位点残基的构象差异由箭头指示,距离以 Å 表示。(D) $\{}^{\{RP}}$ 对精氨酸衍生物的受体范围。L-精氨酸和 D-精氨酸 (10 和 28) 均被接受,且偏好 L-对映异构体,而对胍基的修饰则会损害转化。(E) 使用 FPP 衍生物 30–32, S7 和 S8 对 FSPP 和 $\{}^{\{RP}}$ 进行测试。底物 30–32 被接受,而 S7 和 S8 则未被接受。

全面的生物信息学分析显示,类 正同源物不仅存在于植物中,还存在于多种细菌和藻类谱系中,包括放线菌门 (Actinomycetota)、$\gamma$-变形菌纲 (Gammaproteobacteria)、蓝细菌门 (Cyanobacteriota)、绿藻门 (Chlorophyta) 和囊泡藻门 (Alveolata)(图 S48)。将结构相似性搜索与基于基序的过滤相结合,在不同分类群中找回了 1000 多个推测性的胍基异戊烯基转移酶,这证明了结构特征可以找回那些通过常规序列搜索无法可靠注释的进化远缘酶。

系统发育分析揭示了截然不同的细菌和植物分支,每个分支都与特定的基因组背景相关,且与特化代谢中的作用一致(图 S48)。在蓝细菌门(Cyanobacteriota)和放线菌门(Actinomycetota)中,NosH 正交同源物被嵌入在推测的萜类、aeruginoguanidines、microguanidines 和微囊藻毒素(microcystine)的生物合成基因簇(BCGs)中(S47),以及包含编码非核糖体肽合成酶(NRPS)、聚酮合酶(PKS)和核糖体合成及翻译后修饰肽(RiPPs)基因的隐蔽或杂合簇中(图 S49 至 S61 和表 S7 至 S12)(20, 37, 38)。这些数据表明,NosH 样蛋白在更复杂的环境(如肽类)中也可能作用于胍基,尽管还需要进一步的实验来验证这一假设。在植物中,我们在分析的每个基因组中都发现了一个 NosH 正交同源物,并在 100 多个家族中鉴定出 600 多个候选蛋白,其中豆科(Fabaceae,82 个蛋白)、禾本科(Poaceae,70 个)和十字花科(Brassicaceae,49 个)代表性最强(图 S62)。序列比对显示,对 NosH 催化至关重要的残基(Glu52, Asp59, Leu106, Arg / Lys137, Asp140, Asp / Glu172;NosH 编号)具有高度保守性,而协调胍基的 Asp140 和 Asp / Glu172 残基之间的间距则有所不同(14 到 85 aa;中位数为 32 aa)(图 4A 和图 S63)。植物正交同源物最常在 Arg137 位置携带 Lys,偶尔在 Asp172 位置携带 Glu(图 S64)。所有植物正交同源物在相当于 NosH

A

图 4. 植物胍基异戊烯基转移酶的结构引导发现与验证。(A) 细菌和植物正交同源物中催化和镁结合残基的保守性。(B) 选定用于异源表达和生化表征的植物和藻类正交同源物。(C) 使用胍(i 和 ii)、精胺(agmatine, iii)或 L-精氨酸(L-arginine, iv)作为底物,对四种 NosH 正交同源物的代表性反应进行 LC-MS 分析。提取离子色谱图(EICs)显示了指示的异戊烯基化产物的形成。(D) 胍类生物碱 galegine (2) 和 pterogynine (4) 的拟议且经实验支持的合成路径。左面板总结了拟议的生物合成关系;右面板显示了本研究中经实验支持的转化,包括在烟草(Nicotiana benthamiana)中表达 CofH-Iso1 后异源产生 galegine。部分图表使用 BioRender 创建。

Asn175 位置携带 Asp,这表明该残基可能会在系统发育树中调节底物偏好(图 S65)。

与细菌同源物相比,植物酶表现出更大的结构多样性,并由多种剪接形式代表,每个基因最多预测有 14 个变体。其中一些由 NosH 样核心和额外的 $\alpha$-螺旋结构域组成,而另一些则似乎嵌入在较大的蛋白质中(图 S62 和 S66)。植物 NosH 同源物中一个高度保守的 $\alpha$-螺旋部分对应于一个经常与泛素结合蛋白相关的折叠类(图 S67)。为了测试催化活性,我们选择了 8 个同源物在 $E.$ coli 中进行异源表达和生化表征(表 S13 和 S14)。其中 6 种蛋白质成功表达并纯化:分别来自大麻(Cannabis sativa, CanH)、莱茵衣藻(Chlamydomonas reinhardtii, CamH)、debaryana 土栖衣藻(Edaphochlamys debaryana, EdaH)、小立轴藓(Physcomitrium patens, PhyH)以及阿拉比卡咖啡(Coffea arabica, CofH-Iso1 和 CofH-Iso2,两种剪接异构体)(图 4B)。这 6 种蛋白质在 $\mathrm{Mg}^{2+}$ 存在下均显示出胍基异戊烯转移酶活性(图 4℃ 和图 S68 至 S77)。它们接受游离胍 (1)、L-精氨酸 (10) 和精胺 (Agm, 11) 作为底物,但优先利用二甲基烯丙基焦磷酸 () 作为异戊烯供体;不接受更长链的多异戊烯基二磷酸。这一限制与预测的结构差异一致,因为植物同源物拥有一个结合口袋,而非 NosH 中发现的疏水通道(图 S78)。

这些酶的生化相关性由其在体外产生多种胍类生物碱的能力所强调,包括二甲基烯丙基胍(galegine; 2)、pterogynine (4) 和 pterogynidine (36)。我们进一步观察到植物和藻类 NosH 同源物在产物概况上的差异:藻类酶 CamH 和 EdaH 使用双异戊烯基化衍生物作为底物进行额外的异戊烯基化步骤,从而产生一种额外的三异戊烯基化代谢物 (37)(图 S68 和 S69)。经表征的同源物进一步接受 L-精氨酸和精胺作为二甲基烯丙基-异戊烯基化的底物,在体外产生植物代谢物 sphaerophysin (38) 和化合物 39。由于基因组数据有限且同位素标记研究含糊,galegine (2) 的生物合成长期以来一直处于推测阶段 (12, 39)。在烟草(Nicotiana benthamiana)中异源表达 NosH 同源物 CofH-Iso1 导致了植物体内 galegine (2) 的产生(图 S79)。NosH 样酶的鉴定和生化验证现在为药理相关胍类生物碱提供了直接的酶促联系,并确立了游离胍的异戊烯基化是植物特有代谢中一种保守的生化策略(图 4D,图 S80 和表 S15)。

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讨论

我们的研究证明,游离胍的直接异戊烯化是植物和细菌代谢中的一个保守特征。将结构分析与基于基序(motif)的注释相结合,揭示了一种由双天冬氨酸胍夹钳、R / KxxD... D / E 间距以及疏水异戊烯结合槽组成的活性位点架构,这使得能够检测到那些仅凭序列相似性无法可靠确定的进化远端同源物。这说明了保守的催化架构如何引导跨进化远端谱系的发现,这些谱系共同的催化逻辑在结构层面而非序列层面得以保留。

胍异戊烯转移酶在细菌和植物中广泛分布,经常以包含泛素结合折叠或其他调节架构的多结构域蛋白形式出现。尽管这些额外结构域的功能尚不清楚,但它们与胍异戊烯转移酶核心的重复关联表明,它们在更广泛的生物合成、调节或识别过程中发挥作用。一个可能的例子是河豚毒素的生物合成,其中一种多异戊烯化胍被认为是前体,且 NosH 在体外能产生相应的化合物 (40)。植物 NosH 样酶在体外能产生诸如 galegine (2)、pterogynine (4) 和 sphaerophysine (38) 等胍类生物碱,而其在 *N. benthamiana* 中的异源表达则产生了 galegine。这些观察结果将胍异戊烯化的相关性扩展到了细菌代谢之外,并支持 样酶在植物胍类生物碱生物合成中具有更广泛的作用(图 4D 以及图 S79 和 S80)。

从机制上讲, FPP 是一种具有 I 类萜烯环化酶相关折叠的胍异戊烯转移酶,但其催化逻辑与脄基转移酶或 ABBA 型异戊烯转移酶截然不同。双天冬氨酸夹钳和基于 Arg137 的构象开关实现了胍的激活和底物定位。这种架构支持广泛的底物耐受性,而 $^{RP}$ -Arg 结构则解释了 Asn175Asp 替换如何通过为延伸的胍基底物提供额外的相互作用,在不改变反应性胍基位置的情况下扩大底物范围。

除了生物学重要性外, FPP 还为生物催化提供了机遇。 FPP 和 $^{RP}$ 在温和的水相条件下催化烷基化胍的选择性形成,并接受带有化学可寻址手柄的非天然异戊烯供体。这为化学生物学和材料化学相关的胍基功能化构建块提供了一条酶促路径,在这些领域中,胍基功能化的表面、涂层和薄膜表现出抗菌、抗污和膜相互作用特性 (41–44)。更广泛地说, FPP 说明了结构明确的活性位点基序如何揭示远端酶同源物以及序列注释无法触及的隐秘代谢物的生物合成逻辑。

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致谢

我们感谢 ESRF 束线 ID-30B 的使用以及当地联系人的支持。我们要特别感谢 DESY P11 束线的 J. Hakanpää 和 S. Chatziefthymiou 在数据采集过程中提供的卓越帮助。作者进一步感谢 A. Palusczak 在进行 LC-MS 测量方面的帮助,以及 J. Zapp 在 NMR 结构鉴定方面的帮助。我们对 P. Stallforth、S. E. O'Connor、J. Hartig 和 R. G. da Silva 在有益讨论和稿件校对方面所做的贡献表示感谢。资金支持:本工作得到了以下支持:欧洲研究委员会(ERC CoG 101002326);zukunft.niedersachsen(下萨克森州科学与文化部的资助计划);大众基金会。K.K. 得到了 Claussen-Simon-Stiftung 的 Dissertation Plus 奖学金支持。作者贡献:D.K. 和 J.K. 构思了研究想法。D.K. 和 J.K. 提出了假设并设计了实验。D.K. 进行了蛋白质纯化、体外生化反应、动力学实验、蛋白质结晶和蛋白质结构鉴定。K.K. 和 S.R. 设计并执行了生物信息学分析。D.K. 进行了基因组挖掘和生物合成基因簇鉴定。D.T.、T.J. 和 S.S. 进行了 NosH 底物、参考化合物和 FSPP 的有机合成。H.S. 为生化转化提供了 FPP 衍生物。A.B. 和 Jo.F. 进行了本氏烟草(Nicotiana benthamiana)实验。D.K.、J.K.、K.K.、S.R.、A.L.、Ja.F.、C-P.W. 和 A.K. 分析并讨论了结果。D.K.、J.K.、K.K. 和 S.R. 准备了稿件。竞争利益:作者声明没有竞争利益。数据、代码和材料可用性:本研究中确定的晶体结构坐标已提交至蛋白质数据库,条目 ID 如下:NosH-apo (pdb\_00009tgv), -gua (pdb\_00009tgx), -FSPP-Mg $^{2+}$ (\_00009tgz), -Gua-FSPP-Mg $^{2+}$ (\_00009th3), $^{RP}$ -Arg (\_000031ka)。本研究过程中未产生新代码。所有化学材料的方法和表征可根据方法部分重现。关于质粒等生物材料和原始数据的请求应发送至 J. Koehnke。材料无需材料转移协议(MTAs)即可提供。图表和正文中的表格数据可见 data S57。许可信息:版权所有 © 2026 作者,保留部分权利;独家许可方为美国科学促进会(AAAS)。不对美国政府的原始作品主张权利。https: / www.science.org / about / science-licenses-journal-article-reuse。本研究全部或部分由欧洲研究委员会(ERC CoG 101002326)资助;根据要求,作者将根据 CC BY 公共版权许可提供作者接受的稿件(AAM)版本。

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补充材料

材料与方法;图 S1 至 S84;表 S1 至 S19;数据 S1 至 S57;

MDAR 可重复性检查清单;参考文献 (45–92)

2026 年 2 月 5 日提交;2026 年 8 月 26 日接收

固体物理学

蜂窝状反铁磁体中声子霍尔效应的热力学起源

Qingkai Meng $^{1,2\dagger}$ , Xiaokang Li $^{1*}\dagger$ , Jie Liu $^{1}$ , Lingxiao Zhao $^{3}$ , Chao Dong $^{1}$ , Zengwei Zhu $^{1*}$ , Liang Li $^{1*}$ , Kamran Behnia $^{4*}$

多种绝缘体中由声子产生的热霍尔效应的底层机制尚未被确定。在这项工作中,我们报道了在三硫化镍磷 ($\mathrm{NiPS}_3$) 中存在显著的热霍尔电导,$\mathrm{NiPS}_3$ 是一种具有之字形(zigzag)反铁磁序的蜂窝层范德华堆叠材料。纵向 ($\kappa_{aa}$) 和横向 ($\kappa_{ab}$) 热电导在同一温度下达到峰值,且在该峰值处的热霍尔角符合此前确定的界限。$\kappa_{ab}$ 的幅度对沿 $b$ 轴的磁化强度幅度极其敏感,但与声子平均自由程不相关,这指向了一种内在起源。

电霍尔效应的热模拟被称为热霍尔效应(THE)。它指的是在垂直磁场存在的情况下,由纵向热流产生横向温度差的现象。长期以来,由于声子缺乏电荷和自旋,被认为无法对 THE 做出贡献 (1)。然而,2005 年在一种顺磁绝缘体 ($\{Tb}_{3}\{Ga}_{3}\{O}_{12}$) 中发现的 THE 证明了这一假设是错误的 (2)。大量实验 (3–20) 报道了在多种绝缘体中可检测到 THE,包括三种非磁性固体 (10, 18, 20)。这些实验观察激发了许多关于晶格振动(声子)如何与磁场耦合的理论研究 (1, 21–31)。

$\{NiPS}_3$ 是一种层状反铁磁体,其中 Ni 原子形成蜂窝层,这些层沿 $c$ 轴以侧移方式堆叠,并通过范德华相互作用耦合(图 1A)(32, 33)。其之字形反铁磁序可以用一个哈密顿量来描述,该哈密顿量包含第一和第三邻居之间的铁磁交换,以及第二邻居之间较弱的反铁磁交换 (34, 35)。它具有 $1.8\{eV}$ 的能隙 (33),属于 $MPX_3$(其中 $M = \{Fe}$ , Mn 或 Ni,$X = \{S}$ 或 Se)范德华磁体家族。对块体材料的剥离表明,$\{NiPS}_3$ 的磁序在单层极限下被完全且突然地抑制。这暗示了层间耦合对磁序的重要性 (36)。与 Zhang-Rice 单态-三态跃迁相关的自旋-轨道纠缠激子的发现 (37),增强了人们将该家族作为研究多体相干性和耦合平台的兴趣 (38-41)。最近,红外光谱和拉曼光谱检测到了 $\{FePSe}_3$ 中磁振子与光学声子能带之间的杂化 (38, 40, 41)。

在这项工作中,我们报道了在 $\{NiPS}_3$(一种范德华蜂窝反铁磁体)中观察到 THE。纵向和横向热电导在同一温度下达到峰值,且最大热霍尔角与在其他绝缘体中发现的数值相当。值得注意的是,我们发现横向热响应与面内磁各向异性之间存在强相关性。结合这种磁性固体中存在的磁振子-声子能带交叉,该观察结果支持一种可能由磁振子-声子杂化驱动的内在声子 THE。

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测量热传输

本研究中使用的 $\text{NiPS}_3$ 单晶是通过化学气相传输法生长而成的,使用 $\text{I}_2$ 作为传输剂 [更多详情请参阅补充材料 (42)]。磁化强度的温度依赖性如图 1B 所示。尼尔温度(Néel temperature)为 155 K,易轴沿 $a$ 轴,这与之前的研究一致 (32, 35, 37)。如图 1℃ 所示,在 4.2 K 下,高达 55 T 的磁场依赖性磁化强度未显示出任何相变。鉴于 Ni 原子的磁矩 (1.05 $\mu_B$) (32),在此磁场下,塞曼能(Zeeman energy)为 3.2 meV。磁有序的持续性与通过非弹性中子散射量化的最大交换参数 ($J_3 = 6.9$ meV) 一致 (34, 35)。

我们使用图 1D 所示的一加热器三热电偶法同时测量了纵向和横向热传输 (42)。图 2A 显示了 $\kappa_{aa}$ 在 $0\mathrm{T}$ 和 $14\mathrm{T}$ 下的温度依赖性,两者几乎完全重合。在尼尔温度处未检测到强异常,这表明声子是唯一的载热子。$\kappa_{aa}(T)$ 在 $\$274\{W K}^{-1}\{m}^{-1}$ 处达到峰值,该值高于大多数磁性绝缘体,略低于 $\{Cu}_3\{TeO}_6$ (14),且远低于在黑磷 (18) 等非磁性绝缘体中观察到的声子热导率 [或金刚石,其峰值超过 $10^{4}\{W K}^{-1}\{m}^{-1}$ (43)],证实了磁振子在载热中的作用微乎其微。

图 2B 显示了在三个典型温度下,热霍尔电导 $\kappa_{ab}$ 随磁场变化的依赖性(最高至 14 T)。磁场依赖性始终呈线性,但绝对值从 305 K 时的 2.6 mW K$^{-1}$ m$^{-1}$ 大幅增加到 33 K 时的 910 mW K$^{-1}$ m$^{-1}$(符号保持为负)。这远大于 $\kappa_{aa}$ 的增强幅度,这意味着定义为两者之比的热霍尔角在冷却时也会增加。

图 2℃ 显示了在 $14\{T}$ 下 $\kappa_{aa}$(除以因子 $-160$)和 $\kappa_{ab}$ 的温度依赖性。$\kappa_{ab}$ 在 $T_N$ 处没有出现任何跳跃,并在 $\$25\{K}$ 和 $14\{T}$ 时达到峰值,获得 $-1636\{mW K}^{-1}\{m}^{-1}$ 的显著大值。正如先前研究 (10, 18) 所观察到的,$\kappa_{aa}(T)$ 和 $\kappa_{ab}(T)$ 在同一温度下达到峰值。此外,定义为 $\kappa_{ab}$ 与 $\kappa_{aa}$ 之比再除以磁场的热霍尔角,在该温度下达到 $\$4\times 10^{-4}\{T}^{-1}$ 的峰值。该值保持在 $10^{-4}$ 到 $10^{-3}\{T}^{-1}$ 的狭窄范围内,大多数报道的最大热霍尔角均处于此范围(图 S9)(18)。

这些材料在峰值温度下的声子平均自由程在 10 nm 到 100 $\mu\{m}$ 之间变化 (18)。相比之下,从实验测得的最大霍尔角中提取的热长度 ($\lambda_{tha}$) 尺度 $\lambda_{tha} = \sqrt{\frac{\hbar}{eB} \times \kappa_{ab} / \kappa_{aa}}$ 显示出极小的变化 (18);因此,它可能与另外两个相关的长度尺度相关——原子间距离和峰值温度下的声子波长——这两者与声子平均自由程不同,在这些绝缘固体中没有显著变化 (18)。

声子热霍尔效应(THE)(1, 2I–3I)的拟议理论机制大致可分为外在机制和内在机制。大多数外在情景涉及声子平均自由程。例如,根据最近的一项理论提案(28),纵向和横向热导率可以简单地表示为 $\kappa_{aa} \sim Cv^{2}\tau \propto \ell$ 和 $\kappa_{ab} \sim Cv^{2}\tau^{2}\tau_{0}^{-1} \propto \ell^{2}$。这里,C、v、$\tau$、$\ (=v\tau)$ 和 $\tau_{0}^{-1}$ 分别是声子比热、声速、平均散射时间、平均自由程和时间反演奇 skew 散射率。这两个方程意味着 $\kappa_{aa} \ \$、$\kappa_{ab} \ \^{2}$ 以及 $\kappa_{ab} / \kappa_{aa} \ \$,这与实验结果相反,实验发现 $\kappa_{ab} / \kappa_{aa}$ 不依赖于 $\$。

A

B

C

D

图 1. 晶格结构、磁化强度和热传输装置。(A) $\text{NiPS}_3$ 的晶格结构(空间群为 $C2 / m$)。侧视图(上方)显示了层状结构。每层由 $\text{NiS}_6$ 八面体的蜂窝晶格组成。在 Néel 温度以下,沿 $a$ 轴的磁矩形成铁磁锯齿链,且链之间呈反铁磁有序(磁空间群为 $P_{C}2_1 / m$)(35,37)。(B) 在 7 T 下,三种不同方向的磁化强度随温度的变化关系。曲线在 155 K 处开始分叉,表明发生了反铁磁相变,这与之前的文献一致(32)。(C) 在 4.2 K 下,高达 55 T 的高场磁化强度。没有出现相变,表明存在强健的反铁磁交换相互作用。(D) 同时测量纵向 $[\nabla T_a = -(T_3 - T_2) / I]$ 和横向 $[\nabla T_b = -(T_2 - T_1) / w]$ 温度梯度的装置。磁场沿 $c^*$ 轴方向。

A

B

C

图 2. $\text{NiPS}_3$ 的纵向和横向热导率。(A) 在 0 T 和 14 T 磁场下,纵向热导率 ($\kappa_{aa}$) 随温度的变化关系。两条曲线在整个温度区域内重合,峰值在 25 K 附近。(B) 在三个不同温度下,横向热导率 ($\kappa_{ab}$) 随磁场变化的关系,磁场扫描至 14 T。在热霍尔测量中,热流沿 a (x) 轴,横向温度梯度沿 b (y) 轴。(C) 随温度变化的 $\kappa_{aa}$(除以 -160)与 $\kappa_{ab}$ 的对比。

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$\text{NiPS}_3$ 中 THE 的样品依赖性

通过对 5 个 $\text{NiPS}_3$ 晶体进行研究,我们发现纵向热导率的值非常相似,而热霍尔响应具有样品依赖性,且与磁化强度的各向异性以及孪晶(twinning)的存在相关。结果如图 3 所示。5 个不同样品在 7 T 下磁化强度 $M$ 的温度依赖性如图 3, A 和 B 所示。虽然 $M_a$ 在不同样品之间几乎没有变化,但 $M_b$ 在各向异性最强和最弱的样品之间显示出 $\approx$ $ 30\% 的样品差异。我们的数据与另外两组报告的结果一致(图 S12)。磁化强度的样品依赖性可以基于孪晶的存在来理解 (44, 45)。沿 $a$ 轴和沿 $b$ 轴磁化强度之间的差异因少数畴(minority domains)的存在而减弱。一个合理的推测是,较弱的磁各向异性反映了样品中更高的孪晶密度 [详见“孪晶”部分 (42)]。样品 1, 具有最高的磁各向异性,最接近完美的无孪晶样品;样品 3 是由三种可能的晶畴数量几乎相等而表征的。扭矩磁力计对磁各向异性特别敏感,在两个代表性样品中进一步支持了这一解释(图 3℃)。磁自由能的角度依赖性显示出一种在两个高对称轴处消失的双峰振荡。在 $\frac{M_b}{M_a}$ 较大的样品(样品 4)中,其振幅更大。图 3, D 和 E 显示了 5 个不同样品中 $\kappa_{aa}$ 和 $\kappa_{ab}$ 的温度依赖性。$\kappa_{aa}$ 曲线全部重合。$\kappa_{bb}$ 和比热也是这种情况(图 S5 和 S7)。尽管声子平均自由程相同,但横向响应 $\kappa_{ab}$ 具有很强的样品依赖性。样品 1 的峰值振幅约为样品 3 的 $ 10 倍。

热霍尔电导振幅与磁化强度分量之间的相关性(图 3E,插图)让人联想到将霍尔响应与热力学性质联系起来的 Streda 公式 (46, 47)。与这种相关性形成鲜明对比的是,纵向热导率和声子平均自由程是各向同性的,且与 $\kappa_{ab}$ 或 $M_b / M_a$ 不相关。

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讨论与展望

$\mathrm{NiPS}_3$ 并非首个具有可变幅度的热霍尔效应(THE)案例。在 $\mathrm{SrTiO_3}$ 中,用极少量的 Ca 原子替换 Sr 原子会强烈地抑制 $\kappa_{xy}$ (16)。在 $\mathrm{Sr}_2\mathrm{IrO}_4$ (48) 中,用 Rh 替换 Ir 最初会放大 $\kappa_{xy}$,随后在磁序被破坏时将其抑制。然而,在这两种情况下,热霍尔角的幅度剧烈变化都伴随着纵向热导率的变化以及基态的改变。而在本案例中,我们观察到热霍尔响应有 10 倍的变化,但纵向输运没有变化。随之而来的磁响应变化意味着,热霍尔响应的变化是由自旋晶格与晶体晶格之间的重新排列驱动的。

将 $NiPS_{3}$ 与 $\alpha-RuCl_{3}$ 进行比较同样具有启发意义。两者都是具有蜂窝晶格的范德华层,在零温下具有之字形(zigzag)反铁磁序。然而,与前者相反,人们怀疑后者中存在显著的 Kitaev 项。在这种背景下,值得注意的是,$NiPS_{3}$ 的纵向和横向热导率均比 $\alpha-RuCl_{3}$ 大一百倍(图 S10)。这一观察结果表明,在 $\alpha-RuCl_{3}$ 中,用连续的不相干磁激发 (4.9) 替换 $NiPS_{3}$ 中定义明确的磁振子,会导致声子平均自由程受到严重抑制。尽管如此,这两种固体的热霍尔角大致相等。决定该角度的因素既不随声子平均自由程而缩放,也不太依赖于与声子耦合的磁激发。

在理论上,已知简并的手征声子位于蜂窝晶格的布里渊区中心 (50)。$NiPS_{3}$ 中的磁序打破了反演中心对称性,从而消除了这种简并。最近,拉曼散射和红外电导率报道了 $NiPS_{3}$ 的姐妹化合物 $FePSe_{3}$ 中磁振子与光学声子之间的杂化 (38, 40, 41)。然而,热量是由声学声子携带的。此前已有研究建议后者与磁振子之间存在耦合 (51–53)。假设磁振子模式和声子模式在某一点相交(图 4A)。在这种情况下,即使是极微小的耦合也会消除简并,打开能隙,并产生两种杂化模式。较低的模式具有携带热量并在有限磁场下产生奇响应的能力。我们注意到,在 Petit 等人 (54) 的研究中,非弹性中子散射为第一个 THE 绝缘体 $Tb_{3}Ga_{5}O_{12}$ (2) 中声子模式与磁模式之间的混合提供了光谱证据。

基于这些考虑,我们将计算出的 $NiPS_{3}$ 声子谱 (55) 与从非弹性中子散射测量中提取的磁振子谱 (45) 进行了比较。磁有序在核布里渊区之上产生了一个新的布里渊区 (35, 45)。磁布里渊区在蜂窝晶格的六边形上投影为矩形(图 4B)。由于这种区域折叠,核布里渊区的一个边界点位于磁布里渊区的中心。这一关键特性允许磁振子与声学声子混合。图 4℃ 展示了沿 $\Gamma-M$ 方向磁振子和声学声子的能带色散。可以看出,磁振子能带和声子能带在布里渊区的 $\Gamma$ 点和 M 点附近有多个交点。这些交点在动量空间中沿 $b^{*}$ 发生,而在实空间中,其幅度

研究发现,沿 b 轴的磁化强度决定了 $\kappa_{ab}$ 的幅值。在 M 点附近,三个声学声子分支与磁振子能带相交,最低的交点出现在 3.7 meV 的能量处。该能量处的有限耦合将开启一个能隙。Yang 等人 (27) 认为,独立于微观细节,一种内在的 THE 表现出简单的行为,即 $\kappa_{xy} / T \propto \exp(-T / T^{*})$。$T^{*}$ 代表 Berry 相为有限且常数的能量窗口宽度 (8, 9, 19, 27)。图 4D 显示,我们针对孪晶最少样本(样本 1)的数据呈现出这种行为。拟合结果得出 $T^{*} = 12$ K。这个 1-meV 的能量量级与磁振子-声子交点之间的距离显著接近(图 4℃)。

这一图景与 $\kappa_{ab}$ 对孪晶的极高敏感性相兼容。单层 $NiPS_{3}$ 是由 $NiS_{6}$ 八面体组成的蜂窝网络,其 $C_{3}$ 对称轴($c^{*}$ 轴)垂直于 ab 平面。锯齿形磁序破坏了这些蜂窝层的三倍对称性(图 4E)。在体晶体中,这些层沿可能的 c 轴之一堆叠,而这些轴都相对于 $c^{*}$ 轴倾斜(图 4F)。因此,晶体学堆叠和磁序各自以其独特的方式破坏三倍对称性。锯齿序倾向于三个 a 轴之一,而堆叠倾向于三个 c 轴之一。结果是,两个 $b^{*}$ 轴(一个由晶体堆叠决定,另一个由磁序决定)的相对方向在三个畴中旋转了 $120^{\circ}$(图 4F)。这可以解释随着少数畴比例增加而导致的 $\kappa_{ab}$ 的大幅衰减 (42)。

我们发现,具有锯齿形磁序的蜂窝晶格 $NiPS_{3}$ 具有由磁各向异性决定幅值的声子 THE。结合磁振子-声学声子能带交点,这一观察结果指向了一个内在起源,以及磁振子-声子杂化可能扮演的角色。我们的结果对于关于 $\alpha$-RuCl$_{3}$(另一种具有锯齿形磁序的蜂窝晶格)中 THE 起源的激烈争论具有启示意义。它们提出了一个开放性问题,即磁振子-声子杂化在其他磁性量子材料中产生声子 Berry 曲率的重要性。

A

B

T (K)

$\theta (^{\circ})$

Fig. 3. $NiPS_{3}$ 中热传输、面内磁化强度和转矩的样本依赖性。(A 和 B) 五个不同样本 (1 到 5) 在 B / a (A) 和 B / b (B) 情况下的面内磁化强度。$M_{a}$ 没有检测到变化,但 $M_{b}$ 变化了约 30%。(C) 两个样本 (4 和 5) 在 30 K 和 5 T 时转矩的角度依赖性。$M_{b}$ 较高的样本(样本 4)具有更大的转矩响应。(D) 不同样本中纵向热导率 $\kappa_{aa}$ 的温度依赖性。曲线重合。(插图) 五个样本中峰值 $\kappa_{aa}$ 随面内磁各向异性 ($M_{b} / M_{a}$) 的变化曲线。(E) 五个样本中热霍尔电导 $\kappa_{ab}$ 的温度依赖性。与 $\kappa_{aa}$ 不同,$\kappa_{ab}$ 具有强烈的样本依赖性。(插图) $\kappa_{ab}$ 峰值与 $M_{b} / M_{a}$ 之间的相关性。

C

E

F

D

图 4. magnon-phonon 杂化与堆叠孪晶。(A) magnon-phonon 能带杂化的示意图 (51)。(B) 磁布里渊区(红色)与晶体布里渊区(黑色)的边界 (56)。$\Gamma - Z - M$ 沿 $b^{*}$ 方向。(C) $\text{NiPS}_{3}$ 的计算声子谱(绿色)(55) 与实验推导的 magnon 谱 (35, 45)。在 M 点附近约 4 meV 处存在 magnon-phonon 交点。(D) 样品 1 中 $\kappa_{ab} / TB$ 随温度变化的半对数图。$\kappa_{ab} / TB$ 在 $\approx 30$ K 处达到峰值。在此温度之上,它遵循 $\exp(-T / T^{*})$,其中 $T^{*} = 12$ K。(E) $\text{NiPS}_{3}$ 的磁结构,沿 $c^{*}$ 轴(上)和 $b$ 轴(下)观察 (32, 35)。黑线代表晶胞边界。(F) 具有不同堆叠方向的主畴(橙色块)和次级畴(蓝色和红色块)。每个畴沿三个可能的轴($c_{1}, c_{2}$ 或 $c_{3}$)之一堆叠。红色箭头 ($b_{\mathrm{mag}}^{*}$) 代表由磁序决定的垂直于 $a$ 轴的 $b^{*}$ 轴。橙色箭头 ($b_{\mathrm{lattice}}^{*}$) 代表由堆叠决定的垂直于 $c$ 轴的 $b^{*}$ 轴。这两个轴之间的夹角在三个畴中旋转 $120^{\circ}$。

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致谢

我们感谢 B. Fauqué、G. Grissonnanche、R. Valenti,特别是 A. Wildes 提供的有益讨论。资金支持:本研究得到了中国国家重点研发计划(项目号 2022YFA1403500, 2023YFA1609600, 和 2024YFA1611200)、国家自然科学基金(项目号 12304065, 12674058, 12474043, 52588101, 51821005, 12004123, 51861135104, 和 11574097)、中央高校基本科研业务费专项资金、湖北省自然科学基金(项目号 2025AFA072)以及蔡元培中法项目(项目号 51258NK)的支持。作者贡献:X.L.、Z.Z. 和 K.B. 构思并设计了本研究。L.Z. 提供了本研究中使用的样品。Q.M. 和 X.L. 进行了热传输和磁化测量。L.L. 开发了脉冲高磁场设施和磁化测量站。C.D. 在脉冲磁场下测量了高场磁化。J.L. 进行了磁转矩测量。Q.M.、X.L.、Z.Z.、L.L. 和 K.B. 分析了数据。Q.M.、X.L.、Z.Z. 和 K.B. 在所有作者的协助下撰写了手稿。竞争利益:作者声明不存在竞争利益。数据、代码和材料可用性:所有数据均可在正文、补充材料和 Zenodo (57) 中获得。所有化合物和材料的合成与表征详情见材料与方法部分。许可信息:版权所有 © 2026 作者,保留部分权利;独家许可方为美国科学促进会(AAAS)。对美国政府原始作品不主张权利。https: / www.science.org / about / science-licenses-journal-article-reuse

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补充材料

材料与方法;补充文本;图 S1 至 S13;参考文献 (58–64)

提交日期 2024年9月16日;接收日期 2026年8月19日

机器学习

利用语言模型进行顺序诊断

Harsha Nori\*†, Mayank Daswani†, Christopher Kelly†, Scott Lundberg†, Marco Tulio Ribeiro†, Marc Wilson†, Xiaoxuan Liu, Viknesh Sounderajah, Jonathan M. Carlson, Matthew P. Lungren, Bay Gross, Peter Hames, Mustafa Suleyman, Dominic King, Eric Horvitz\*

我们探索了前沿语言模型在顺序诊断(sequential diagnosis)中的能力,这是一种能够捕捉临床推理迭代特性的诊断范式。在给定简短的临床表现后,临床医生有选择性地获取信息以达成诊断,从而能够评估诊断的准确性和检查成本。我们开发了一个交互式基准测试和一个人工智能(AI)系统,该系统模拟了一个医生小组,能够不断修正鉴别诊断并选择具有成本效益的检查。利用该基准测试,该系统在《新英格兰医学杂志》的临床病理讨论病例中达到了 83.2% 的准确率,在 MIMIC-IV-ED 急诊科入院病例中达到了 80.3% 的准确率,优于全科医生(分别为 36.1 和 46.8%)。尽管这些结果是在受控的基准设置中获得的,但它们凸显了语言模型在支持更准确、更低成本诊断方面的潜力。

临床诊断是一个信息收集与推理的顺序过程,而非对完整病例的一次性分析。医生从有限的信息开始,制定初步的鉴别诊断,然后选择要询问的问题和要开具的检查,在权衡每项检查的预期诊断收益与其成本、患者负担以及延迟之间。随着结果的返回,他们不断修正鉴别诊断,并判断现有证据是否足以做出诊断或采取治疗行动,或者是否需要进一步的检查。这种假设细化与战略性信息收集的交替进行,是临床诊断的核心。

语言模型(LMs)具有极具前景的医学推理能力,在执业医师资格考试和结构化诊断案例分析中取得了顶尖分数 $(1-7)$。目前对语言模型的评估尚未将诊断测试为一种主动的、顺序的信息收集过程,即同时考虑诊断准确性和诊断检查成本。相反,基准测试通常在完整指定的病例上评估语言模型,将主诉、现病史、体格检查结果和诊断测试结果打包在单个提示词中。通过将诊断压缩为一次推理步骤,静态基准测试无法衡量系统是否提出了正确的问题、是否避免了无差别的检查、是否随着证据的积累而更新鉴别诊断,或者是否能识别出何时已达到足够的确定性以结束检查。因此,它们可能会夸大诊断能力,同时掩盖诸如不恰当的检查或过早结案等失效模式。

我们推出了顺序诊断基准(Sequential Diagnosis Benchmark, SDBench),该基准将来自《新英格兰医学杂志》的 304 例临床病理讨论病例(CPC cases)(8) 以及来自 MIMIC-IV-ED 的 325 例从急诊室到入院的就诊记录(ED cases)(9) 转化为交互式的分步就诊过程。CPC 病例和 ED 病例共同涵盖了广泛的临床表现和记录风格,最终诊断范围从常见疾病到罕见疾病不等。每个病例以简短的临床摘要开始,诊断者 [可以是人工智能(AI)代理或医生] 可以据此提出问题、开具诊断检查或做出最终诊断(图 1)。性能评估分为两个维度:诊断准确率(对照参考诊断进行衡量)以及所开具检查的累计预估成本。该框架不仅评估诊断准确率,还评估高效识别并获取信息证据的能力,以及确定何时已达到足够的诊断确定性以结束就诊的能力。

我们使用 SDBench 来评估诊断编排器(Diagnostic Orchestrator, DxO),这是一个与模型无关的编排器,它通过模拟一个具有互补角色的临床专家小组来执行顺序诊断,在每一步中融入具有成本意识的检查管理,并在多次独立运行中汇总诊断结果。在 SDBench 中,在受控的纯文本条件下,与参与评估的个体全科医生相比,DxO 在预估成本-准确率帕累托前沿(Pareto frontier,即没有任何一种评估方法能同时实现更高准确率且更低成本的运行点)中处于更高的区域。这些比较并未证明其优于专科医生、多学科团队或现实世界的临床实践。然而,它们表明,在大语言模型(LM)对迭代工作流的编排下,可以在旨在评估顺序诊断的基准测试中改善可衡量的成本-准确率权衡,并证明这些方法可以被利用来支持临床医生。

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结果

SDBench 将每个 CPC 和 ED 病例呈现为一个基于文本的顺序交互过程,始于一段简短的临床病例摘要。在每一步中,担任诊断代理(Diagnostic agent)角色的医生或 AI 系统可以询问病史或体检结果、开具诊断检查,或提交最终诊断(图 1)。SDBench 的关键组成部分和流程如图 2. 所示。一个门控代理(Gatekeeper agent)负责调解所有基于底层病例记录的信息请求,仅返回通过指定问题或检查在临床上可获取的信息。当请求的结果在源记录中缺失时,门控代理会生成诊断中立的合成结果,以避免通过提示数据缺失来提供关于最终诊断的线索。最终诊断由一个评审代理(Judge agent)进行裁定,该代理使用由医生编写的五级临床评分标准和参考诊断,其中 4 或 5 分(指管理方案不会因此改变的诊断)被视为正确(补充材料,材料与方法)。

测试成本是通过请求的检查项目,利用基于当前医疗程序术语(CPT)的定价(源自一个大型医疗系统的收费清单 (10))来估算的,其中病史询问和体检问题被视为固定医生就诊成本的一部分。该框架允许在诊断准确率和累计测试成本这两个维度上,对参与的医生、基准 LM 以及 DxO 变体进行直接比较(补充材料,材料与方法)。

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临床病理讨论会研究

我们发现,搭载 GPT-5 的 DxO 建立了一个新的帕累托前沿(Pareto frontier),在任何成本或准确率水平上均优于参与的医生(图 3)。在没有预算限制的 DxO 配置下,其表现出显著的有效性,在平均成本为 $5431. 时达到了 83.2% 的准确率。DxO 的结构化推理能够响应特定的预算限制,随着测试成本的逐步降低,准确率略有下降,在平均成本为 $2241 时达到 80.9% 的准确率,在 $1303. 时达到 79.6%。在光谱的另一端,采用旨在实现卓越诊断的配置时,准确率在成本为 $8945. 时跃升至 84.5%。这种权衡是通过平衡请求的问题数量与检查数量来实现的(补充文本)。

我们招募了活跃的初级保健医生、医院医生和急诊医生(包括内科专家、急诊和

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诊断代理

详细说明喉咙痛、扁桃体周围肿胀和出血开始的时间、进展情况,以及任何相关症状,如发烧、吞咽困难、声音变化、耳痛或呼吸问题?

入院前七周:出现喉咙痛。在第一周内,疼痛持续存在。四天后,酸痛加剧,导致无法入睡。入院前 31 天,注意到右侧喉咙疼痛和肿胀,有食物“卡住”的感觉,并伴有疲劳;无发烧、头痛、呼吸道、胃肠道症状或皮疹……

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让我们收集一些病史。

涵盖既往病史、用药史、恶性肿瘤体征、HIV / HPV 病史、牙科问题、出血史、妊娠情况、初步实验室检查(例如 FBC、凝血功能,以及包括颈部 MRI 在内的影像学检查……

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鼻咽癌?

测试请求:右侧扁桃体周围肿块的超声引导下粗针穿刺活检(大孔径),送检常规 H&E 染色、免疫组化(CD31, D2-40, CD34, ERG, GLUT-1, pan-cytokeratin, CD45, CD20, CD3, Ki-67)

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不是。肺泡状横纹肌肉瘤?

肿瘤细胞核质比高,且可见频繁的有丝分裂象。

免疫组化:CD31:阴性 D2-40:阴性 CD34:ERG:GLUT-1:泛细胞角蛋白 (Pan-cytokeratin):CD45:CD20:CD3:Ki-67:60% 核阳性

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组织学 (H&E):浸润性圆细胞

检测请求:免疫组化:Desmin, Myogenin, MyoD1(用于评估横纹肌源性分化)

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让我们排除胚胎性横纹肌肉瘤

对扁桃体周围活检标本的免疫组化分析显示,肿瘤细胞对 desmin 和 MyoD1 呈弥漫性阳性,对 myogenin 呈多灶性阳性。

检测请求:肿瘤组织 FOXO1 (13q14) 分离 FISH 检测

荧光原位杂交(使用针对 FOXO1 (13q14) 位点的分离探针)未检测到任何 FOXO1 重排

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诊断者的最终诊断

“右侧扁桃体周围区域胚胎性横纹肌肉瘤”

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NEJM 标准答案诊断

“咽部胚胎性横纹肌肉瘤”

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评判员对比

5 / 5 - 同一种疾病;候选者补充了正确的具体位置。

图 1. DxO 解决顺序诊断推理问题的示例。初始病例信息:一名 29 岁女性因喉咙痛、扁桃体周围肿胀和出血入院。症状在抗微生物治疗后未减轻。

图 2. SDBench 中的编排。通过门控代理 (Gatekeeper)、诊断代理 (Diagnostic) 和评判代理 (Judge) 之间的协调,将 CPC 或 ED 病例语料库转化为一组顺序诊断挑战。在运行时,门控代理调解诊断代理的信息请求,决定是否以及如何回答诊断代理关于患者病史、检查结果和检测结果的问题。评判代理评估诊断代理的最终诊断是否与原始病例中报告的标准答案一致。

(急诊科医生)以评估人类在该基准测试上的表现。在针对 CPC 病例(在开发期间从工程工作中预留的 56 个病例)的医生研究中,参与者平均完成了 36.4 个(闭卷)和 34.8 个(开卷)病例,在 56 个病例中总共提供了 764 个(闭卷)和 662 个(开卷)人类诊断。平均而言,医生每例病例花费 11.9(闭卷)和 18.1(开卷)分钟,提出 6.1(闭卷)和 8.4(开卷)个问题,并请求 7.1(闭卷)和 12.1(开卷)项检测,导致平均成本为 \$3049(闭卷)和 \$4725(开卷)。他们的平均诊断准确率为 22.3%(闭卷)和 36.1%(开卷)。与闭卷测试相比,在开卷 CPC 研究中提供搜索和参考工具增加了提问数量和订购检测的数量,并

增加了医生每例病例花费的总时间,以及每例病例检测的平均成本。尽管如此,即使是诊断准确率最高(51.8%)的医生,在准确率和成本方面都被超越了。我们发现医生将提问和检测紧凑地交替进行,在订购第一项检测前平均提出 5.6 个问题。相比之下,搭载 GPT-5 的 DxO 在相同病例中订购第一项检测前平均提出了 25.5 个问题,这表明其采取了不同的策略,即在启动诊断检测之前进行广泛的结构化病史采集。

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急诊医学研究

CPC病例由学术临床医生策划,而急诊(ED)病例则由当代的电子健康记录(EHR)笔记组成,这些笔记反映了常规工作流程和更具代表性的病例组合。在没有预算限制的情况下,DxO 在每个 ED 病例上的平均诊断准确率达到 80.3%,平均成本为 \$4979(图 4)。在有预算限制的情况下,DxO 的准确率在成本为 \$2634 时达到 73.2%,在成本为 \$2037 时达到 69.5%。正如预期的那样,全科医生在 病例上的熟练程度高于 CPC 病例,平均准确率为 46.8%(相比之下,后者为 36.1%)。医生在 病例上的平均检测成本为 \$3400。诊断表现最好的个体医生实现了 62.5% 的平均准确率,平均成本为 \$3332(40 个病例)。

与 CPC 病例一样, 倾向于比参与研究的医生询问更多的问题并开出更少的检测单,尤其是在预算受限的情况下。虽然医生的表现根据是 还是 病例而有显著差异,但 在这两个数据集上的准确率相当。

图 3. 病例的性能和帕累托前沿(Pareto frontiers)。点表示基于 GPT-5 的 、基准语言模型(LMs)以及参与研究的医生在《新英格兰医学杂志》临床病理讨论会病例上的平均诊断准确率和平均累计医疗成本(仅测试集;图例)。参与医生的表现分为闭卷(红色 +)和开卷(灰色 x)挑战,每种设置的平均表现由粗体 + 和 x 表示。

现代语言模型以及利用这些模型的 在处理长尾、非典型模式时似乎比参与的临床医生更一致。与语言模型在 病例和 病例中整体维持的性能相反,临床医生的诊断准确率在以罕见复杂性为特征的 病例中骤降。

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模型能力与错误研究

我们在图 3( 病例)和图 4( 病例)中展示了使用 GPT-5 的 CPC 的性能。我们将 CPC 在 CPC 和 CPC 病例上的性能与使用极简提示词(见补充文本)的商业语言模型进行了比较,测试了来自多种供应商的多个模型系列和规模。在所有测试的模型中, CPC 的编排将 CPC 病例和 CPC 病例的诊断准确率分别平均提高了 4.4 和 7.9 个百分点(见补充文本)。

我们研究并比较了 、基准模型和参与医生的诊断错误(见补充文本)。我们使用两个独立的前沿语言模型对失败案例进行分类,随后进行了人工验证。 CPC 的错误通常涉及在错误的特异性级别上选择一个临床上相近的答案,而非无关疾病。 CPC 相对于基准模型的优势集中在依赖于更好病史采集的诊断中,例如罕见接触史和旅行相关感染。对于此类病例,更深入的询问能挖掘出在广泛的检测组合中不易发现的鉴别线索。当医生出错时,其诊断结果往往比 AI 的错误结果更偏离参考诊断。

最初开发时,GPT-4.1 是当时最强的模型。随后我们使用 GPT-5 对该方法进行了评估,并在发表前,在不修改提示词或编排的情况下,使用 GPT-5.5 重复了完整的评估套件(见补充文本)。

继续定义帕累托前沿,且其相对于基准提示词的准确率优势在 GPT-5.5 中有所增加,这表明模型能力的提升并不一定会削弱精心编排所带来的益处。

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讨论

SDBench 是一个基准测试,它将 304 例《新英格兰医学杂志》的临床病例讨论(CPC)案例和 325 例 MIMIC-IV-ED 案例转化为交互式的、多轮的诊断挑战。与静态医学基准不同,SDBench 要求决定询问什么、测试什么以及何时做出诊断,且每项决定都会产生成本。在该基准测试的背景下,我们提出了 DxO,这是一种执行顺序诊断工作流的方法,通过模拟临床专家小组来决定请求哪些问题或测试。我们证明,DxO 在提高诊断准确率的同时降低了累计测试成本,从而为准确率和成本建立了新的帕累托前沿(Pareto frontier)。尽管 最初是利用 CPC 案例开发的,但在独立的急诊(ED)案例以及新发布的语言模型(LMs)中,它依然保持了帕累托主导地位。

我们发现, CPC 在诊断准确率方面显著优于执业全科医生,且通常产生的累计测试成本更低。这些发现或许并不令人惊讶,因为 CPC 案例是基于其教学价值而筛选的,且通常包含专家的反思和结论。我们预计,当将 CPC 与专家级专科医生或根据每个案例内容选定的多学科专家团队进行比较时,性能差距将会缩小。我们原以为 CPC 在 ED 挑战中的优势会较小,因为这些挑战源自常规急诊科案例,因此完全属于全科医生和急诊临床医生的日常实践范围。

图 4. ED 案例的性能和帕累托前沿。点表示使用 GPT-5 的 、基准 LMs 以及参与医生(图例)在急诊科评估后入院患者身上的平均诊断准确率和平均累计医疗成本。图中描绘了单个医生的开卷性能(灰色 x)和平均性能(粗体 x)。

我们假设,部分优势源于训练接触的规模:前沿 LMs 在涵盖罕见病、非典型表现和跨专业推理的海量语料库上进行训练,从而获得了任何个体医生都无法掌握的广泛医学知识,同时允许 LMs 在不同案例中一致地应用这些知识。人类临床医生的诊断推理可能会受到近期病例、时间压力、认知疲劳或全科及专科特有的偏见和盲点的影响,而这些系统则保持统一的召回率和系统性的评估。 CPC 实现的编排推理过程(其中模拟的临床专家追求不同的推理目标)有助于强制执行一致的信息收集和成本评估,而这些行为是医生们努力追求但可能无法在认知负荷以及时间和资源限制下始终维持的。

此外,常规临床实践会适当地将避免漏诊和确保患者安全置于对累计测试成本的显式优化之上。尽管临床医生在日常工作中可能会考虑资源利用率,但他们很少拥有能够持续量化每项额外测试的边际诊断价值和成本效益的正式决策支持工具。通过维持一个显式的鉴别诊断列表,通过对抗性批判挑战主导假设,并量化每项测试的边际价值,该系统旨在减轻常见的推理失败,如锚定效应和过早闭结。相比之下,大多数医生没有奢侈的条件能够拥有一个持续可用的团队,来系统地审计他们的推理、挑战假设,并在整个检查过程中帮助维持诊断的严谨性。

这些优势在受控的模拟环境中被放大了。基准环境抽象掉了医疗实践中的许多细节,包括患者病史和报告中的不确定性、记录不完整、信任关系的建立以及纵向随访。临床医生还必须应对时间限制、行政要求以及影响医疗交付的情绪和伦理考量,而这些都超出了本研究的范围。因此,性能优势特指在理想化条件下的信息收集和诊断准确性,而非实践中所要求的临床推理、患者护理或医疗判断的全部范围。

结果表明,DxO 性能背后的结构化推理过程(显式假设跟踪、对抗性批判和成本意识的测试选择)可以增强人类的临床判断。医生已经在潜意识中执行了许多此类认知任务,但很少能达到同样的系统化程度、经济问责制或针对认知偏差的保障措施。通过将这些过程编纂成典,此类系统可以在补充医疗护理中至关重要的临床专业知识和情境判断的同时,提高诊断的一致性并使推理更加透明。未来工作的一个重要方向是设计能够整合自动化顺序诊断核心能力的临床医生-AI 工作流 (11)。除了支持医生对个体患者进行诊断和成本效益管理外,这里描述的方法还可以应用于教育领域,包括交互式诊断挑战和旨在提升医学培训及继续专业教育期间临床推理能力的洞察力构建案例模拟。

尽管 SDBench 使我们能够更真实地评估 AI 系统的诊断推理,但局限性依然存在。该基准目前仅包含来自 CPC 案例和急诊(ED)就诊的病理案例。CPC 案例可能过度代表了具有诊断挑战性的表现,且两者都排除了健康或良性的就诊情况,因此整体案例组合和疾病患病率并未反映常规临床实践的情况。此外,医生和 AI 代理都是与基于文本的“先知”门卫进行交互,而非与电子健康记录(EHR)或开放世界中丰富的患者就诊情况交互。测试环节并未体现出因记录不完整和沟通细微差别(例如患者遗漏或忘记信息)而产生的噪声、不确定性和歧义,也未体现时间动态(包括对初步干预的生理反应)。测试环节也没有捕捉到成像、波形或病理切片等对真实诊断工作流至关重要的多模态数据。因此,SDBench 衡量的是理想化信息条件下的诊断推理,而非床边表现或患者预后。

我们评估的一个局限性是将 DxO 的性能与个体医生进行比较。现实世界的诊断通常涉及多学科协作,并置于一个拥有适当转诊至不同专家团队流程的丰富医疗生态系统中。在指标方面,SDBench 中使用的成本估算依赖于标准化的美国定价数据,这些数据虽然接近但无法完全捕捉现实世界的变异性和实际维度,如结果出具时间、侵入性、患者不适感和物流可用性。同样,Judge 评分量表在疾病层面评估诊断的正确性,但并未评估治疗的适当性、安全性或纵向管理质量。在实践中,医生会随着时间的推移迭代地进行诊断、开药和调整,而 SDBench 和 DxO 仅关注推理的诊断阶段。

更广泛地说,将诊断建模为一个顺序的、具有成本意识的过程——而非一个单次预测问题——为开发 AI 系统提供了一个框架,使其能更紧密地契合临床推理的迭代特性,同时支持更透明、更经济且更具协作性的医疗决策。随着模型能力的不断增强,将结构化顺序推理与临床医生专业知识相结合的方法可能会重塑 AI 支持诊断推理的方式,并有望提高全球医疗服务的质量和可及性。

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参考文献与注释

1. H. Nori et al., arXiv:2311.16452 [cs.CL] (2023).

2. H. Nori, N. King, S. M. McKinney, D. Carignan, E. Horvitz, arXiv:2303.13375 [cs.CL] (2023).

3. H. Nori et al., arXiv:2411.03590 [cs.CL] (2024).

4. D. McDuff et al., Nature 642, 451–457 (2025).

5. S. Cabral et al., JAMA Intern. Med. 184, 581–583 (2024).

6. E. Goh et al., JAMA Netw. Open 7, e2440969 (2024).

7. P. G. Brodeur et al., Science 392, 524–527 (2026).

8. New England Journal of Medicine, Case Records of the Massachusetts General Hospital (2026); https: / www.nejm.org / medical-articles / case-records-of-the-massachusetts-general-hospital.

9. A. Johnson et al., MIMIC-IV-ED (version 2.2). PhysioNet (2023); https: / doi.org / 10.13026 / 5ntk-km72.

10. Kaiser Permanente Washington, “Central Hospital standard charges” (2023); https: / healthy.kaiserpermanente.org / content / dam / kporg / final / documents / health-plan-documents / coverage-information / 910511770-central-hospital-standard-charges-wa-en.xlsx.

11. S. S. Everett et al., NPJ Digit. Med. 9, 409 (2026).

12. H. Nori et al., SDBench code and data. Zenodo (2026); https: / doi.org / 10.5281 / zenodo.21286121.

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致谢

我们感谢 NEJM 集团允许我们在本文呈现的研究中使用来自《新英格兰医学杂志》(New England Journal of Medicine)临床病理会议病例的叙述和数据。这项工作受益于微软公司许多团队的贡献。我们向微软内部及外部同事提供的宝贵见解表示诚挚感谢,包括 B. Bunning(斯坦福大学)、N. Ding ()、N. de Freitas ()、K. Mandl ()、A. Milicevic ()、V. Patel(哥伦比亚大学)、J. Petro ()、H. Poon ()、D. Rhew ()、A. Rodman(贝斯以色列女执事医疗中心)、N. Shah(斯坦福大学)、C. Sherstan ()、C. Cooper Simpson ()、E. Shortliffe(哥伦比亚大学)、K. Simonyan ()、P. Szolovits(麻省理工学院)、E. Topol(斯克里普斯研究所)、R. Wachter(加州大学旧金山分校)以及 J. Weinstein ()。我们同时感谢 G. Fontana (Prova Health) 和 K. Hawkins (Prova Health) 在健康经济学和结果方面提供的支持。资金:这些研究未获得外部资金。作者贡献:概念化:C.K., E.H., H.N., M.D., M.T.R., M.W., S.L.。方法论:C.K., E.H., H.N., M.D., M.T.R., M.W., S.L., X.L.。调查:C.K., E.H., H.N., M.D., M.T.R., M.W., S.L., V.S., X.L.。可视化:C.K., E.H., H.N., M.D., M.T.R., M.W., S.L.。项目管理:E.H., D.K., H.N., M.S.。监督:E.H., H.N., D.K.。初稿撰写:C.K., E.H., H.N., M.D., M.T.R., M.W., S.L., X.L.。审阅与编辑:B.G., C.K., E.H., H.N., J.M.C., M.D., M.P.L., M.T.R., M.W., P.H., S.L., V.S., X.L.。竞争利益:所有作者均为该公司员工并持有该公司股权,该公司提供 AI 和医疗保健方面的商业服务。C.K., E.H., H.N., M.D., M.T.R., M.W., S.L. 和 X.L. 是由该公司提交的美国专利申请 19 / 722,651 的发明人,该专利涉及一种用于序贯诊断的自动化评估框架。数据、代码和材料可用性:本研究未产生新材料。代码和数据可在 Zenodo (12) 获取。实现 SDBench 的源代码——包括 Gatekeeper、Judge、Cost Estimator 和基准编排——也可在 MIT 许可证下通过 https: / github.com / sdbench 获取。报告的研究中使用了三个数据集:(i) NEJM 病例记录:SDBench 是利用发表在《新英格兰医学杂志》上的麻省总医院病例记录开发的 (8)。源自这些病例的 SDBench 数据集可由 NEJM 集团提供给非商业研究使用(需获得许可);请求应发送至 elicensing@nejm.org。(ii) MIMIC-IV-ED:急诊科就诊记录提取自 MIMIC-IV 的一个模块 MIMIC-IV-ED (9)。本研究中使用的精选病例子集将在论文发表时在 PhysioNet 上发布,前提是完成 PhysioNet 身份验证并签署 MIMIC-IV 数据使用协议。(iii) 测试成本:本研究中使用的成本数据获取自 Kaiser Permanente 华盛顿中央医院标准收费文件 (chargemaster) (10),该文件公开可见于 https: / healthy.kaiserpermanente.org / content / dam / kporg / final / documents / health-plan-documents / coverage-information / 910511770-central-hospital-standard-charges-wa-en.xlsx(访问于 2026 年 4 月)。该文件由 Kaiser Permanente 根据美国医疗保险和医疗补助服务中心 (CMS) 的医院价格透明度规则 (45 CFR Part 180) 发布,该规则要求医院公开标准收费信息

以机器可读的格式免费公开,且不对重复使用设限。SDBench 原生支持导入此文件,但该框架也可以调整为接受任何其他收费表或成本表。许可信息:版权所有 © 2026 作者,保留部分权利;独家被许可方为美国科学促进会(AAAS)。不对美国政府的原创作品主张权利。https: / www.science.org / about / science-licenses-journal-article-reuse

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补充材料

材料与方法;补充文本;图 S1 至 S9;表 S1 至 S13;参考文献 (13–29);MDAR 可重复性检查清单

提交日期 2026年4月4日;接收日期 2026年8月10日

二维金属中的电子连续谱束缚态

Morgan Thinel $^{1,2}$ , Xiong Huang $^{1}$ , Daniel G. Chica $^{2}$ , Simon Turkel $^{1,3}$ , Sebastian E. Rossi $^{1}$ , Christie S. Koay $^{2}$ , Hong Li $^{3}$ , Willa Mihalyi-Koch $^{2}$ , Bipasa Samanta $^{4}$ , Madisen Holbrook $^{1}$ , Aravind Devarakonda $^{5}$ , Luca M. Nashabeh $^{1}$ , Alexandru B. Georgescu $^{4*}$ , Xavier Roy $^{2*}$ , Xiaoyang Zhu $^{2*}$ , Abhay N. Pasupathy $^{1,3*}$ , Raquel Queiroz $^{1*}$

连续谱束缚态(BICs)是指尽管处于扩展的离域态连续谱之中,但仍保持局域化的量子态。虽然光学 BIC 已在光子系统中实现,但在金属背景中实现嵌入的电子束缚态仍然是一个持续的挑战。在本研究中,我们利用扫描隧道显微镜,在二维范德华金属 $Pd_{5}AlI_{2}$ 的金属连续谱中识别出两种由缺陷诱导且保持局域化的电子态。我们的计算表明,$Pd_{5}AlI_{2}$ 装饰棋盘格晶格上的电子跳跃干涉产生了一个由空间局域本征态构成的(准)平带,这些本征态与色散连续谱正交。在这种受挫晶格中的原子缺陷将相关的平带局域态移入金属连续谱中,从而形成了鲁棒的、对称保护的 BIC。

波动方程的解通常在扩展的连续谱态与空间局域的离散频率之间具有光谱分离。然而,在量子力学早期,von Neumann 和 Wigner 表明,薛定谔方程中的特定势能可以导致波函数在空间上局域化,且其能量处于扩展态的连续谱之内 (1)。这些连续谱束缚态(BICs)已被证明源于衍射干涉,使其成为波动方程(包括声学和光子学中的麦克斯韦方程组)的一个通用特性 (2)。BIC 已在光子系统中得到实验实现,其中纳米加工工具能够对光子模式的能量和对称性进行定制 (3–5)。基于此研究,已出现了诸如手性激光 (6–9)、增强的非线性频率转换 (10–12) 以及减轻波导器件辐射损耗 (13–15) 等应用。通常,BIC 是通过精细的参数调节设计的,从而强制扩展波产生局域相消干涉 (16, 17)。尽管拓扑 BIC 已在声学和光子晶格的角点和边缘实现 (18–21),但光子晶格中由晶格对称性保护并产生光学 BIC 的点缺陷,比拓扑边缘提供了更可控的平台 (22, 23)。这些进展激励了在凝聚态系统中寻找金属连续谱内类似电子束缚态的探索。

缺陷周围的束缚态在绝缘体和半导体(如 $MoS_{2}$ (24, 25))中普遍存在,它们存在于能带之间的光谱隙中。这些状态的局域化与带隙的存在直接相关,使得缺陷态能够避免与连续态发生杂化。然而,在金属中,稀疏的点缺陷表现为扩展态的散射中心,仅对其产生微弱扰动 (26, 27)。局域缺陷态也可以出现在拓扑绝缘体中,在这种情况下,拓扑保护的表面态会发生散射,且缺陷态位于体相的光谱隙内 (28, 29)。诸如近藤效应 (30) 等多体相互作用可以产生局域共振 (31–34),但它们通常出现在费米能级附近,而非金属能带深处。少数研究报道了在二维 (2D) 电子气系统(如 GaAs (35–37))中,由人工设计的周期性势场或势阱所限制的电子 BIC。然而,由于这些工作中缺乏空间分辨测量,关于空间局域束缚态的主张仍具有模糊性 (38)。因此,在实验上实现明确的指数级局域电子 BIC 仍然是一个开放的追求。

类比于光学 ,调制晶格跳跃参数可能是实现电子 的一条有前景的途径 (39)。在这项工作中,我们报道了一种通用机制,可在由于相邻晶格位点之间电子跳跃受阻而表现出平带的晶格中产生鲁棒的 。这种受阻现象发生在子晶格位点数量不等的二分晶格(如 Lieb 晶格 (40))以及线图晶格(如 kagome (41) 和 dice (42) 晶格)中。受阻跳跃也可以由晶格对称性与轨道组成的相互作用引起,例如在装饰棋盘晶格中 (43, 44)。在所有这些晶格中,色散带与高度简并的平带共存,其中扩展的布洛赫态可以组合成空间局域的本征态,称为紧凑局域态 (CLSs) (45–47)。电子 的形成可以在以下框架内理解(图 1A):晶格缺陷将 CLS 的化学势移入色散带的连续谱中。由于本征态的局域特性,较远的 CLS 基本不受影响,而连续态仅受到轻微扰动。值得注意的是,在这一位移过程中,CLS 与色散态之间的正交性可以得以保持,这使得 CLS 在不与连续谱杂化的情况下保持完美的空间局域化,从而形成 。这种机制对于承载非平凡平带的材料是内在的 (48, 49),使得通过局部空位或杂质即可形成电子 ,而无需对模型参数进行精细调优。

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实验系统

我们使用扫描隧道显微镜和光谱学(STM 和 STS)来直接表征 $Pd_{5}AlI_{2}$ 中电子 BIC 的局部状态密度(LDOS)。$Pd_{5}AlI_{2}$ 是一种具有装饰棋盘格晶格的范德华(vdW)金属,该晶格会导致受挫电子跳跃(50)。$Pd_{5}AlI_{2}$ 的四方晶体结构(空间群 I4 / mmm)由一层层堆叠的 vdW 薄片组成,每片厚度为 5 个原子。这些薄片可以通过机械剥离从晶体中剥离,并作为空气稳定的薄片而存在。每个金属间化合物薄片由一个 PdAl 棋盘格晶格组成,该晶格夹在两个 $Pd_{2}$ 正方形平面之间,并由碘原子封顶(图 1B)。对 PdAl 层的紧束缚模型显示,它形成了一个二分晶格,在正交的 Pd $d_{xz}$ 和 $d_{yz}$ 轨道之间存在受挫跳跃,并由 Al $p_{z}$ 轨道介导(图 1℃)(50)。

这种类 Lieb 晶格(称为装饰棋盘格)的电子结构已在光电子发射实验中测得,其特点是在高对称点(M 和 $\Gamma$)具有线性色散能带,且这些能带被一个平带所相交(50)。图 1℃ 显示了该平带在 $Pd_{5}AlI_{2}$ PdAl 内层的 CLS 映射图。图 1D 显示了在负样本偏压下测得的劈开的 $Pd_{5}AlI_{2}$ 晶体表面碘原子的原子分辨率 STM 形貌图。图像呈现出一个面内晶格常数 a = 4.05 Å 的正方形晶格(图 S1),这与单晶 X 射线衍射结果一致(51, 52)。在表面上观察到 3 种类型的点缺陷(在图 1D 中标记为 i, ii, 和 iii),其密度相对较高($\sim2.3\times10^{12}~cm^{-2}$)(图 S2)。$Pd_{5}AlI_{2}$ 的隧道光谱显示在所有电压下状态密度(DOS)均非零(紫色光谱,图 1E),这与该材料的金属性一致。该光谱在 +150 mV 和 +400 mV 处具有峰值。我们将准粒子干涉(QPI)图样与密度泛函理论(DFT)计算的联合状态密度(JDOS)进行对比,以确定这些峰值的能带结构起源(图 S3 和补充文本)。能带结构(图 S4)显示这些特征源于 2 种不同的现象:峰 1 源于 $\Gamma$ 空穴口袋关闭附近的能带曲率变化($\sim150~meV$),峰 2 源于 400 meV 附近能带的 Lifshitz 转变。值得注意的是,对 ii 型缺陷的 STS 表征显示,在连续的金属性能带内存在两个额外的 LDOS 峰,分别位于 +475 和 +620 mV(绿色光谱,图 1E),而 $Pd_{5}AlI_{2}$ 光谱的所有其他特征保持不变。这些额外的峰在其他类型的缺陷隧道光谱中并不存在(图 S5)。

B

C

图 1. $Pd_{5}AlI_{2}$ 中缺陷上的束缚态。(A) 金属连续体中的扩展态与平带的紧凑局域态示意图。一个由缺陷局部势能将其推入连续体的平带本征态,由于其与连续体态正交,因此仍保持局域化。(B) $Pd_{5}AlI_{2}$ 范德华(vdW)薄片的晶体结构,沿 ab 平面观察。(C) 中心 PdAl 棋盘格平面的顶视图,叠加层显示了紧凑局域态(CLS,灰色方块)的原子轨道表示。在正交的 $Pd\ d_{xz}$ 和 $d_{yz}$ 轨道之间发生了受挫跳跃,由 Al $p_{z}$ 轨道介导。蓝色和红色箭头分别表示同相和反相跳跃。(D) $Pd_{5}AlI_{2}$ 一个 $16\text{-nm}^{2} \times 16\text{-nm}^{2}$ 区域的恒流 STM 形貌图(设定点:-300 mV, 50 pA),显示了表面碘原子和三种类型的点缺陷。(E) 在无缺陷区域(紫色虚线)以及 (D) 中圈出的 ii 型缺陷(绿色)上测得的平均隧道谱(设定点:150 mV, 30 pA;调制:25 mV, 927 Hz)。在缺陷 ii 上出现了两个连续体中的束缚态。数据采集时的样品温度为 T = 6.7K。dI / dV 为微分电导。

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束缚态的光谱分析

通过对比不同样品偏压下的实验 STM 形貌和 DFT 模拟(图 2, A 和 B, 以及图 S6),我们将感兴趣的缺陷确定为中心装饰棋盘格 PdAl 平面中的 Pd 空位。对图 2℃ 所示区域的光谱成像显示,在 +470 mV 时,Pd 空位周围呈现出四叶图案,类似于原子的 d 轨道(图 2D)。+620 mV 时的状态则呈现为类似于原子 s 轨道的圆形图案(图 2E)。通过测量图 2℃ 中蓝色线沿线的点光谱,我们证明这些状态被限制在亚纳米的空间范围内(图 2F 和图 S3 中的 DFT 计算),表明两种状态都具有显著的局域化特性。此外,与半导体中束缚态的隧道光谱,甚至分子和量子点中束缚电子的光谱 (53) 相比,这些峰的线宽(35 至 47 )异常尖锐。高斯线形(不同于受寿命限制的洛伦兹线形)表明,外在展宽(例如电子-声子耦合)主导了测得的线宽,这意味着内在的 BIC 寿命显著更长(图 S7)(54)。值得注意的是,在 +470 的大面积光谱成像中,我们没有观察到缺陷诱导的散射图案,而是在其他偏压下观察到了明显的干涉(图 S8)。这种无法检测到准粒子干涉的现象与与连续态耦合极弱的 BIC 是一致的。金属能带内的离散能级、空间局域化以及缺乏散射的结合,表明这些状态在电子上与金属连续态隔离,类似于与光子连续态解耦的光学 BIC。

图 2. Pd 空位上束缚态的光谱结构。(A 和 B) 在 (A) 负偏压 (-300 , 50 pA) 和 (B) 正偏压 (+550 , 50 pA) 下,包含 Pd 空位的 $Pd_{5}AlI_{2}$ 区域的实验(紫色)和 DFT 模拟(灰度)STM 形貌。(C) 包含所有三种类型缺陷区域的 5-nm $^{2}$ $\times$ 5-nm $^{2}$ STM 形貌,在此区域获取了 STS 图谱。(D 和 E) 在对应于 LDOS 中缺陷诱导峰的偏压下的实空间 LDOS 图 [(D) = +470 ; (E) = +620 ]。颜色刻度表示 LDOS。DOS 中的强特征仅在 ii 型缺陷周围明显,并且在两个量化能级上具有不同的类轨道对称性。(F) 跨越 (C) 中蓝色线限定区域的线光谱。缺陷状态在距离缺陷中心 1 nm 范围内衰减。面板 (C) 至 (F) 中的数据是在反馈设定点 -300 , 50 pA 下获取的。光谱是在样品温度 6.7 K 下,使用 10 , 927 Hz 的锁相调制获取的。a.u.,任意单位。

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束缚态建模

我们转向包含该缺陷的 PdAl 层的受挫跳跃能带结构,以解释局域化效应。图 3A 显示了没有次近邻跳跃的理想化装饰棋盘格模型的能带结构。在图 3B 中,我们使用描述 Pd $d_{xz}$ 和 $d_{yz}$ 轨道以及 Al $p_{z}$ 轨道的简化三带模型,计算了一个 41-by-41 的 PdAl 超原胞(移除单个 Pd 原子)的 DOS 光谱。该模型推导自我们此前为该材料开发的基于 DFT 的 Wannier 模型 (50)。空位周围的光谱与实验结果高度一致,其中在费米能级 ($E_{F}$) 之上几百毫电子伏特处出现了两个峰。在这些模拟中,这些峰的宽度由一个任意展宽参数决定。这些本征态是由

在 Pd 缺陷周围 3-by-3 网格中的对称 CLS 形成的(图 S9)。形成局域态的相邻轨道的相对相位受系统关于空位的 $C_{4}$ 对称性约束,从而产生四个可能的本征态,我们根据它们在 $C_{4}$ 对称算符下的本征值 $\pm1$ 或 $\pm i$ 对其进行标记。在检查局域态的对称性时(图 3B),我们发现 +400 meV 处的较低能量状态对应于 -1 本征态,而 +700 meV 处的状态则对应于 +i 本征态。为了使 +i 态出现,需要额外的原位势,我们将其归因于位于 PdAl 棋盘格上方和下方的碘原子的 p 轨道(图 S10)。这些 p 轨道受到平面内 Pd 轨道缺失的影响。通过绘制由波函数 $\pi$ 相移定义的节点线(图 3, C 和 D),我们发现 -1 态具有角节点面,形成一个四叶结构,而 +i 态具有径向节点,从而形成一个圆形结构。虽然单个 CLS 通常在 LDOS 中不可见,但将 CLS 移入连续谱会导致局限在缺陷位置的 LDOS 增强,且保留 CLS 波函数的节点结构。这些理论结果与实验光谱成像一致(图 3, E 和 F)。

图 3. 受挫跳跃模型中的节点结构。(A) 理想化装饰棋盘模型的能带结构,其中跳跃干涉导致一个平带被两个线性色散能带所相交。(B) 模拟的 41-by-41 装饰棋盘超晶格的态密度 (DOS) 光谱。Pd 空位周围 3-by-3 超晶格的光谱(绿色)显示出两个在没有空位的 3-by-3 超晶格(紫色)中不存在的峰。 (A) 和 (B) 中所示计算的详细信息可见于补充文本部分“Pd 空位紧束缚计算详情”。(C 和 D) 包含单个 Pd 空位的 41-by-41 超晶格的两个本征态示意图。色轮表示 Pd d 轨道的相对相位。在波函数发生 $\pi$ 相移的地方出现节点线(橙色虚线)。(D) 中所示的状态由于来自碘 $p_{x} + ip_{y}$ 轨道(彩虹圆圈,图 S10)的原位势能产生的额外 $\sigma_{y}$ 变换而出现。这些本征态是平带紧束缚局域态 (CLSs) 的组合,因此也是平带的本征态。它们与高能色散态正交并保持局域化。(E 和 F) 紧束缚模型产生的节点线叠加在图 2, D 和 E 所示的实验光谱图上,显示出定性一致。

为了理解理想装饰棋盘格的完全平带是否是 $Pd_{5}AlI_{2}$ 中承载点缺陷连续域束缚态 (BICs) 的必要条件,我们在模型中人为引入了次近邻跳跃,这给平带增加了色散。这种变换使得 CLSs 不再是系统的精确本征态,因此,缺陷态可以与扩展态的连续谱发生杂化。然而,BICs 的指数级局域化在很大范围的次近邻跳跃和能带色散参数下都是鲁棒的,包括与 $Pd_{5}AlI_{2}$ 实验能带结构相匹配的实际参数(图 S11)(50)。此外,其他缺陷类型中不存在 BICs(图 S5)表明,扰动 PdAl 受挫晶格是一个必要条件。为了支持这一点,我们合成了掺杂有微量 Fe 的 $Pd_{5}AlI_{2}$ 单晶,其中 STM 形貌显示在 PdAl 棋盘平面内的 Pd 位点发生了替代(表 S1 和 S2 以及图 S12 至 S14)。在这些 Fe 替代位点的光谱成像识别出了 BICs,但其能量与固有空位相关的能量不同。光谱成像显示,这些状态具有与空位诱导的 BIC 相同的范围和四叶空间对称性,证实了不同的杂质势可以在该晶格位点产生类似的 BICs(图 S14)。这证明了局域化是由平带的拓扑非平凡特性驱动的,而非由传统的杂质态驱动。这些状态源于相邻轨道的干涉,在孤立轨道中没有类似物 (55–57)。事实上,在图 2, D 和 E 中观察到的类原子轨道 LDOS 模式明显

大于原子轨道。

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束缚态的二聚体

由此产生的电子 BICs 类似于不同能量下具有不同对称性的原子轨道。与传统的原子轨道一样,它们在靠近时可以结合,形成分子束缚态。然而,与原子轨道不同的是,它们分裂为成键轨道和反键轨道的能量分裂不需要遵循传统规则。我们对一个包含两个由单个原子晶格常数分隔的缺陷区域进行了光谱成像(图 4A)。该二聚体的空间平均光谱显示出四个束缚态,

图 4. 电子 BICs 的二聚体。(A) 获取光谱图的包含双空位区域的 STM 形貌图。(B) 缺陷二聚体 [(A) 中所示的虚线椭圆] 的空间平均隧穿光谱,并叠加了图 1E 中的单个缺陷光谱。(C 至 F) 对应于 (B) 中二聚体束缚态峰值的偏置电压下的实空间 LDOS 图。(G 至 J) 由两个空位本征态组合而成的二聚体本征态示意图。(G) 和 (I) 是两个空位状态之间存在 $\pi$ 相位关系的组合。(H) 和 (J) 是两个同相缺陷状态的组合 (图 S17)。(G) 至 (J) 中定义的节点线与实验数据的形状在定性上是一致的。数据是在反馈设定点为 -400 mV, 50 pA,锁相调制为 5 mV, 1127 Hz,样品温度为 6.7K 的条件下获取的。

对应于与单个空位相关的两个 BICs 中每一个的分裂(图 4B)。这种分裂让人想起同核双原子分子中形成的成键和反键能级。与双原子分子成键的预期一致,对四叶 BICs 的双空位状态进行光谱成像显示,在 +440 处有一个成键轨道,在更高能量的 +510 处有一个反键轨道(图 4, C 和 D)。与之不同,圆形状态的杂化在缺陷之间创建了一个节点,类似于 +590 处的反键分子轨道(图 4E)。在 +650 处的更高能量状态在缺陷之间表现出高状态密度,类似于成键分子轨道(图 4F)。对包含一个二聚体和一个孤立空位区域的光谱成像证实了这种能量分布 (图 S15)。当 Pd 空位被两个或更多原子晶格常数分隔时,未观察到缺陷间杂化,这进一步支持了 BICs 的强局域特性 (图 S16)。我们可以将这些二聚化状态在 PdAl 紧束缚模型中描述为两个单缺陷本征态的线性组合(图 4, G 至 J)。在双原子分子中,成键轨道源于原子轨道线性组合中的有利相位相互作用,这使得组成分子轨道的节点数少于反键轨道。在这种情况下,BIC 相对于其邻居的相对相位——即线性组合的符号——是决定成键和反键 CLSs 能量的唯一因素 (图 S17)。特别是,当两个缺陷状态彼此反相时,相互作用是有利的,且双空位状态的能量较低。由两个同相缺陷状态组合而成的二聚体状态能量较高,无论最终结构中的节点数量如何。

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讨论与展望

利用 STM 和 STS,我们证明了在 $Pd_{5}AlI_{2}$ 的金属连续谱中,空位周围会形成电子束缚态。这一现象源于 $Pd_{5}AlI_{2}$ 装饰棋盘格上的电子跳跃干涉,从而导致产生与连续谱正交且具有强抗杂化能力的空间局域本征态。我们的结果表明,$Pd_{5}AlI_{2}$ 中的点缺陷可以承载光学 BIC(连续域束缚态)在凝聚态物理中的类比。更广泛地说,我们的结果指向了一种在其他实验实现的二维受挫跳跃晶格(如 Lieb 和 kagome 晶格 (58, 59))中创建 BIC 的通用机制,在这些晶格中,CLS(紧凑局域态)被认为在包括超导、密度波和磁性在内的奇异关联电子相中起着关键作用。我们对缺陷局域 CLS 的成像为受挫晶格中由轨道干涉引起的拓扑非平凡局域态提供了实验验证。此外,我们证明了缺陷二聚化可以控制这些电子态的能量,并证明了这些 CLS 与原子轨道截然不同。受近期缺陷工程进展的启发(例如在半金属 $PtSe_{2}$ (60) 等 vdW 材料中组装原子级精确的空位晶格),我们预见 $Pd_{5}AlI_{2}$ 可以为可控合成可能承载拓扑特性的电子 晶格提供平台。事实上,当缺陷上的 LDOS 排列成线或晶格时,可以实现无损的缺陷介导传输通道。它们与体态的共存为调节电子特性和探索多体相互作用(包括模拟 Kondo 物理 (61))提供了一个丰富的平台。类比于光子 所携带的对扰动具有鲁棒性的拓扑电荷,我们的缺陷 源自平带的非平凡拓扑。CLS 的多位点、相位相干结构允许对 LDOS 晶格或阵列进行精确工程,其能量由 CLS 波函数之间的相位关系决定。这种原子级精确的拓扑非平凡晶格可以在催化和能量存储方面实现功能 (62)。最后,$Pd_{5}AlI_{2}$ 的 vdW 结构通过机械剥离、堆叠和扭转,为与其他材料的接口提供了路径。总而言之,缺陷密度和迁移的热力学与动力学控制,结合传统的 vdW 材料操纵,使 $Pd_{5}AlI_{2}$ 成为高度可调局域态的有潜力的候选材料,这可能对拓扑量子化学以及拓扑系统中多体效应的研究有用。

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致谢

本研究中展示的 DFT 计算是在印第安纳大学的 Big Red 200 和 Quartz 超级计算机集群上完成的。资金支持:这项关于新型受挫跳跃模型中局域态的研究由加州理工学院布朗基础科学研究所的布朗研究员奖(Brown Investigator Award)资助。合成与结构表征部分得到了美国国家科学基金会(NSF)通过哥伦比亚大学精密组装量子材料材料研究科学与工程中心(MRSEC)DMR-2011738 的支持。STM 测量由美国空军科学研究办公室在奖项编号 FA9550-22-1-0389 和 FA9550-21-1-0378 下资助。合成工作还作为可编程量子材料(一个能源前沿研究中心)的一部分得到了部分支持,该中心由美国能源部(DOE)科学办公室基础能源科学部在奖项 DESC0019443 下资助。哥伦比亚大学的理论研究得到了 NSF 在奖项编号 DMR-2340394 下的支持。印第安纳大学的 DFT 计算部分得到了礼来基金会(Lilly Endowment)通过其对印第安纳大学普适技术研究所的支持,以及印第安纳大学启动资金的支持。作者贡献:DFT 计算:B.S., A.B.G.;资源(代码):A.D.;STM 实验:M.T., X.H., S.T., H.L., M.H.;监督:R.Q., X.R., X.-Y.Z., A.N.P.;合成:D.G.C., C.S.K., W.M.-K., X.R.;紧束缚计算:S.E.R., M.T., L.M.N., R.Q.;撰写——初稿:M.T.;撰写——审阅与编辑:所有作者。竞争利益:作者声明没有竞争利益。数据、代码和材料可用性:本研究的原始数据和处理后的数据可在 Zenodo (63) 下载。本研究中所用材料的合成在方法部分有描述,在 Devarakonda 等人 (50) 的研究中描述得更为详细。评估本文结论所需的其他数据已在正文或补充材料中提供。许可信息:版权所有 © 2026 作者,保留部分权利;独家许可方为美国科学促进会(AAAS)。不对美国政府的原始作品主张权利。https: / www.science.org / about / science-licenses-journal-article-reuse

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补充材料

材料与方法;补充文本;图 S1 至 S17;表 S1 和 S2;

参考文献 (64–76)

提交日期 2024年10月18日;重新提交日期 2025年8月28日;接收日期 2026年8月14日

10.1126 / science.adt9825

MEMBRANES

纳米通道中动态功能驱动的快速且选择性传输

Hao Zhang $^{1}$ †‡, Yuan Kang $^{2,3*}$ †, Fan Feng $^{4}$ , Ting Hu $^{2}$ , Rongming Xu $^{5}$ , Hang Yu $^{5}$ , Kaiqiang He $^{2}$ , Zhe Yang $^{1}$ §, Zhuyuan Wang $^{1}$ , Cher Hon Lau $^{3}$ , Ze-Xian Low $^{6}$ , Qinfen Gu $^{7}$ , Jefferson Zhe Liu $^{4*}$ , Huanting Wang $^{2}$ , Xiwang Zhang $^{1,8*}$

能够实现快速且选择性质量传输的纳米通道在能源、资源、生物医学和环境应用中至关重要。然而,极端的纳米级限域,通常伴随着刚性的通道环境,会产生巨大的摩擦和粘附障碍,导致传输缓慢且选择性受限。我们发现,通过利用限域功能基团的内在迁移率(例如自旋转)来增强分子传输,纳米通道动力学是解决这些挑战的关键。通过实验和模拟相结合,我们证明了这种动力学通过促进动能传递并实现更高效的分子接力来重塑传输,从而将分离性能提升至超越当前基准的水平。我们的研究结果强调了纳米通道动力学在调节限域质量传输中的作用,并为设计先进的纳米通道系统提供了一个框架。

特征尺寸低至 1-nm 和亚 1-nm 范围的人造通道对于理解和利用该尺度下的质量传输至关重要 (1, 2)。此类尺寸与大多数离子、气体、溶剂和溶质的尺寸相当,为在多种应用中实现可控传输提供了基础 (3–5)。这一能力的核心在于适当设计的通道几何结构(例如尺寸)和内置功能(例如嵌入颗粒),它们通过尺寸和化学亲和力的差异来区分目标物种,同时通过连续的吸附-脱附事件(跳跃)提供定向接力,以维持快速传输 (6–9)。

因此,研究重点一直集中在优化通道尺寸和功能设计上 (10–12)。尽管这些方法对于快速且选择性传输至关重要,但它们通常在渗透性和选择性之间存在内在的权衡 (2, 12–14),这在很大程度上源于大多数纳米通道的刚性和空间受限特性。狭窄的通道壁和固定的功能基团会对快速传输产生空间位阻(摩擦障碍) (2, 15, 16),而纳米限域下增强的通道-目标亲和力虽然有利于选择性,但会通过加深局部势阱(粘附障碍)来阻碍目标的迁移 (17)。

相比之下,生物通道(如膜蛋白)通常表现出卓越的渗透选择性。除了精确编程的通道几何结构和功能基元外,它们的动态灵活性也被认为是实现卓越传输特性的关键 (18–25)。在代表性的离子通道(例如用于 $K^{+}$ 的 A 链地霉菌 K 通道)、溶剂通道(例如用于 $H_{2}O$ 的水通道蛋白-1)和气体通道(例如用于 $NH_{3}$ 的铵转运蛋白 B)中,蛋白质骨架和功能侧基会经历构象波动、翻转或旋转 (18–23)。尽管处于极窄的限域中,这些动力学能够调节局部能量景观并降低传输障碍,从而在保持卓越选择性的同时实现目标的超快渗透。

受此原理启发,我们将纳米通道动力学确定为在人工通道中实现快速且选择性传输的关键。我们在二维(2D)通道中引入了自旋转的铵离子 ($\mathrm{NH}_{4}^{+}$),以引入调节分子传输的局部动力学。这些可旋转的功能基团除了排斥竞争分子外,还能加速目标分子的吸附-脱附,并通过增强的动能传递促进连续跳跃。通过这种方式,可以很大程度上克服纳米限域下的摩擦和粘附势垒,将快速传输与高选择性相结合,从而在实际条件下实现卓越的溶剂分离性能。

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具有动态功能的二维通道的设计与制备

与生物通道相比,由常用材料构建的人造纳米通道通常缺乏周期性的骨架灵活性。因此,我们选择通过引入具有快速自运动功能的组分,将动态特性引入纳米通道中,例如在二维 $Ti_{3}C_{2}T_{x}$ MXene 通道中接枝旋转的 $NH_{4}^{+}$(图 1A 和图 S1)。$Ti_{3}C_{2}T_{x}$ 是带负电且经过功能化(-OH、-O 和 -F)的纳米片,具有较高的 Hamaker 常数(图 S2 和 S3)。这些特性使其能够轻松堆叠成层状组件,形成极性的、亚 1 nm 的层间通道,通过纳米限域效应产生的增强氢键和静电吸引力,实现 $NH_{4}^{+}$ 的稳定锚定 (11, 26)。正如我们的密度泛函理论计算和从头算分子动力学 (AIMD) 模拟所支持的,$NH_{4}^{+}$ 可以通过与多达四个表面功能基团的相互作用稳定地驻留在 MXene 通道内,且位置波动有限(图 S4 和 S5)。

为了引入 $NH_{4}^{+}$,将制备好的处于湿态的原始 MXene 膜(untreated-M)暴露在氯化铵($NH_{4}Cl$)溶液中,以获得 $NH_{4}^{+}$ 功能化的 MXene 膜($NH_{4}^{+}-M$)(示意图见图 S6),该膜显示出无缺陷的表面和层状截面(图 1B 和图 S7, A 至 D)。高分辨率透射电子显微镜 (HRTEM) 和 X 射线衍射均显示,在引入 $NH_{4}^{+}$ 后,层间通道定义明确且未受干扰(图 S8)。X 射线光电子能谱 (XPS) 通过特征 N 信号确认了 $NH_{4}^{+}$ 的引入,并通过深度剖析显示其在层压材料中的均匀分布,这与元素映射结果一致(图 1B 和图 S7, E 和 F,以及 S9)。同时,引入的 $NH_{4}^{+}$ 在傅里叶变换红外光谱中于 $1450\ cm^{-1}$ 处产生了一个新峰,归属于 N-H 弯曲振动,同时 O-H 伸缩振动从 3470 红移至 $3440\ cm^{-1}$。这些变化意味着 MXene 与 $NH_{4}^{+}$ 之间通过氢键和静电吸引力存在非共价相互作用(图 S10),这也通过多功能交联赋予了 $NH_{4}^{+}-M$ 更好的机械性能(图 S11)。

图 1. 通道表征与传输特性。(A) 分子通过 $NH_{4}^{+}-M$ 通道(上)的示意图,以及由自旋转 $NH_{4}^{+}$ 促进的传输过程(下)。(B) $NH_{4}^{+}-M$ 的扫描电子显微镜 (SEM)(左上;比例尺 250 nm)和高分辨率透射电子显微镜 (HRTEM)(左下;比例尺 5 nm)图像,右侧为深度剖面 N 1s XPS 光谱,显示了 $NH_{4}^{+}$ 从表面到 200 nm 深度处的分布。SEM 图像中的黄色虚线表示膜厚度。HRTEM 图像中的白色虚线框表示插图中的放大区域,其中黄色线条突出了层间通道。(C) 溶剂蒸气透过 untreated-M 和 $NH_{4}^{+}-M$ 的透过率。(D) $NH_{4}^{+}-M$ 内纳米受限 $NH_{4}^{+}$ 与溶液中自由 $NH_{4}^{+}$ 的 ${}^{1}H$ VT-NMR 光谱。a.u.,任意单位;ppm,百万分比。(E) 通过 untreated-M、$ND_{4}^{+}-M$、$NH_{4}^{+}-M$ 和 mix-M($NH_{4}^{+} / ND_{4}^{+}$ 摩尔比 = 1:1)的水通量。(F) untreated-M、$ND_{4}^{+}-M$ 和 $NH_{4}^{+}-M$ 的 ${}^{1}H$ 时域 NMR 光谱。(G) 体相水、untreated-M、$ND_{4}^{+}-M$ 和 $NH_{4}^{+}-M$ 的 PFG-NMR 光谱。(H) 根据 PFG-NMR 光谱推导出的体相状态和受限状态下的水自扩散系数。

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功能基团旋转的作用

通过测量代表性溶剂(包括水、乙醇、异丙醇和乙酸乙酯)在 untreated-M 和 $NH_{4}^{+}-M$ 通道中的渗透率,评估了 $NH_{4}^{+}$ 功能基团对质量传输的影响(图 1℃ 和图 S12)。在相同的溶剂环境下,两种通道具有相似的溶剂可及尺寸(图 S13)。然而,较大的溶剂(如乙醇)在 $NH_{4}^{+}-M$ 中的渗透速度明显慢于在 untreated-M 中的速度,这与传统观点一致,即引入的功能基团通常会在纳米通道中产生额外的空间位阻 (13, 26)。出乎意料的是,$NH_{4}^{+}$ 带来的这种显著拥挤(约 3 Å)反而加速了水分子的扩散,将渗透率从 1.5 提高到 2.2 mol m $^{-2}$ h $^{-1}$ kPa $^{-1}$ ,几乎等同于开放空气中的水分蒸发速率 (2.4 mol m $^{-2}$ h $^{-1}$ kPa $^{-1}$ )。

这种增强的水渗透性能还通过液态水的单组分渗透汽化测试得到了验证,在该测试中,通道与液体直接接触(图 S14)。同样,$NH_{4}^{+}-M$ 的水通量增加了 70%,同时排除了通道宽度及其分布作为影响因素的可能性(图 S15 和 S16)。这种增强效果在不同厚度的 $NH_{4}^{+}-M$ 膜中也得到了持续观察(图 S17)。

我们将这种异常的传输加速归因于 $NH_{4}^{+}$ 的旋转动力学。与静态功能基团不同,$NH_{4}^{+}$ 在少数极性溶剂(如水)中表现出超快旋转,由于其四面体 N-H 构型,在 1.1 ps 内旋转角度可达 $33^{\circ}$(旋转相关时间 $\tau_{c}$)(27, 28)。它形成了一个由 4 个氢键结合的水分子以及 1 个与其不断交换的第 5 个水分子组成的流动内水合壳层(图 1A)(29, 30)。这种动力学产生了角跳跃,使水合的 $NH_{4}^{+}$ 发生旋转,并驱动推测相邻的水分子向前移动。通过 ${}^{1}H$ 变温核磁共振 (VT-NMR) 对 MXene 通道内 $NH_{4}^{+}$ 的动力学进行了探测(图 1D)(31)。在测试的温度范围内没有出现峰合并失效(decoalescence),表明 $NH_{4}^{+}$ 在纳米限域状态下仍保持快速的局部平均化,而线宽对温度的弱依赖性与旋转动力学而非质子交换更为一致 (32)。结合 AIMD 模拟证明的 $NH_{4}^{+}$ 受限的平移运动(图 S5),这些结果支持 $NH_{4}^{+}$ 在 MXene 通道内持续旋转。

基于这些结果,我们通过将旋转速度与水渗透率相关联,验证了 $NH_{4}^{+}$ 旋转的传输增强作用。我们将 $NH_{4}^{+}$ 中的氢 (H) 替换为氘 (D),以获得功能化为 $ND_{4}^{+}$ 的 MXene 通道(称为 $ND_{4}^{+}-M$)以及 $ND_{4}^{+}-NH_{4}^{+}$ 混合物(摩尔比 1:1,称为 mix-M)(图 1E)。与其他离子功能化试剂(例如 $K^{+}$;图 S18 和表 S1)不同,$ND_{4}^{+}$ 是 $NH_{4}^{+}$ 的同位素类似物,具有相似的物理化学性质,因此导致几乎相同的通道特性(图 S19)。然而,较重的氘使 $ND_{4}^{+}$ 具有更高的转动惯量,因此在相同温度下,其理论旋转角速度比 $NH_{4}^{+}$ 低 $\sqrt{2}$ 倍(补充文本)。我们的结果确实揭示了水传输对 $NH_{4}^{+}$ 旋转速度的强依赖性,这由 $ND_{4}^{+}-M$ 的水通量(808 g m $^{-2}$ h $^{-1}$)低于 mix-M(1070 g m $^{-2}$ h $^{-1}$)和 $NH_{4}^{+}-M$(1145 g m $^{-2}$ h $^{-1}$)所证明,这意味着 $NH_{4}^{+}$ 旋转对水传输具有直接的正向影响。

这些结果通过 ${}^{1}H$ 时域核磁共振(NMR)中的自旋-自旋弛豫时间 $(T_{2})$ 分析得到了进一步证实(图 1F),该分析能够区分 $NH_{4}^{+}$ 结合水($10^{2}$ ms 范围)和自由水($10^{3}$ ms 范围)。$NH_{4}^{+}$ -M 在两种状态下均表现出最长的 $T_{2}$,其次是 $ND_{4}^{+}$ -M 和未处理-M,这表明功能基团旋转速度越快,受限水的流动性越强 (33)。一致地,脉冲场梯度刺激回波核磁共振(PFG-NMR)分析显示 $NH_{4}^{+}$ -M 中的水流动性增强,其自扩散系数为 $2.47 \times 10^{-9}$ $m^{2}$ $s^{-1}$ ,高于 $ND_{4}^{+}$ -M ( $2.09 \times 10^{-9}$ $m^{2}$ $s^{-1}$ ) 和未处理-M ( $2.01 \times 10^{-9}$ $m^{2}$ $s^{-1}$ ),接近于体相水(图 1, G 和 H)(4)。这种依赖于同位素的增强效应进一步支持了 $NH_{4}^{+}$ 旋转在受限水传输中的动力学作用。

由于 $NH_{4}^{+}$ 功能化还可能通过改变通道内的溶剂吸附来调节溶剂传输 (2, 34),我们测量了未处理-M 和 $NH_{4}^{+}-M$ 在气态和液态下的溶剂吸收量(图 S20 和 S21)。这些测量结果表明,$NH_{4}^{+}$ 的引入对水和乙醇的吸收影响极小,甚至具有负面影响,从而在很大程度上排除了增强吸附是水渗透增加的原因。在 $NH_{4}^{+}$ 功能化后,通道表面的自由能的分散分量和极性分量也显示出极小的变化(补充文本和图 S22)。这些结果表明,水通量的增强源于传输动力学的加速,而非溶剂吸附或分配的变化。

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功能互连的作用

E

为了进一步探究旋转的 $NH_{4}^{+}$ 如何调节传输,我们通过调整其在通道内的负载量来改变其分布。$NH_{4}^{+}-M$ 中的平衡 $NH_{4}^{+}$ 含量由 $NH_{4}^{+}$ 中的 N-H 与 MXene 通道壁上 -F 的摩尔比(N-H / -F)反映,随着 $NH_{4}^{+}$ 负载量的增加,该比值从 0 增加到 0.46, 0.78, 和 1.01(图 S23)。这导致通道逐渐收缩,从 5.3 到 4.9 Å(图 S24)。因此,乙醇的渗透速度逐渐减慢,而水通量则持续增加,并且在比值超过 0.78 时出现显著跳跃(图 2A)。这些趋势表明,$NH_{4}^{+}$ 的传输调节作用在稀疏和密集状态下均有效。特别是,当旋转的 $NH_{4}^{+}$ 达到饱和时,这种水传输增强效果变得显著,这表明

相邻功能基团之间存在协同传输效应,这一现象与其互连有关 (17, 35)。

为了确定相邻 $NH_{4}^{+}$ 位点能够相互互连的临界距离,我们利用分子动力学 (MD) 模拟中的径向分布函数 (RDF) 研究了水合 $NH_{4}^{+}$ 的结构(图 2B),结果显示 $NH_{4}^{+}$ 周围有一个半径为 3.7 Å 的定义明确的内水合壳层,对应于 7.4 Å 的临界距离。同时,我们计算了在不同 N-H / -F 比值下相邻 $NH_{4}^{+}$ 位点之间的平均间距(图 2℃ 及补充文本),并将其与该距离进行了比较。随着 $NH_{4}^{+}$ 负载量的增加,相邻 $NH_{4}^{+}$ 之间的平均距离从 9.1 Å(比值 = 0.46)迅速下降到 7.5 Å(比值 = 0.78),并进一步下降到 6.7 Å(比值 = 1.01)从而允许互连。这一过程通过绘制通道内水合 $NH_{4}^{+}$ 的分布图也得到了可视化呈现(图 2, D 至 F)。随着通道内 $NH_{4}^{+}$ 变得更加拥挤,它们的水合壳层逐渐重叠,最终形成了从通道入口到出口的互连路径。一致地,结合原子力显微镜和红外光谱的测量为潮湿条件下 $NH_{4}^{+}$ 周围水簇的形成和互连提供了额外证据(图 S25)。

C

F

图 2. 纳米通道中动态功能的互连。(A) 不同 $NH_{4}^{+}$ 覆盖度(由 N–H / F 摩尔比表示)下,通过 $NH_{4}^{+}-M$ 的水和乙醇渗透通量。(B) 在不同 $NH_{4}^{+}$ 覆盖度下,水平衡 $NH_{4}^{+}-M$ 通道内围绕 $NH_{4}^{+}$ 的水分子的 N–O RDFs。插图突出了 $NH_{4}^{+}$ 互连的临界 $NH_{4}^{+}$ 间距。(C) 平均 $NH_{4}^{+}$ 间距随 N–H / F 摩尔比的变化函数。插图阐明了 $NH_{4}^{+}$ 间距的定义。(D 至 F) 在 N–H / F 摩尔比为 0.46 (D)、0.93 (E) 和 1.39 (F) 时,水平衡 $NH_{4}^{+}-M$ 通道内水簇分布的可视化。对于每种情况,顶部和底部面板分别展示了通道的侧视图和顶视图。

总的来说,这些观察结果强调了 $NH_{4}^{+}$ 互连在调节溶剂传输(尤其是水传输)中的作用。虽然单个旋转的 $NH_{4}^{+}$ 能促进局部水的通过,但互连的 $NH_{4}^{+}$ 通过将离散的水域连接成延伸的流体路径,进一步加速了传输,使得水分子的传播比在未功能化区域中更具连续性和方向性。

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动态功能化使能的传输机制

我们利用分子动力学(MD)模拟来阐明功能基团的旋转与互连对质量传输的协同影响。我们构建了三种类型的 MXene 通道:(i) 无 $NH_{4}^{+}$,(ii) 固定 $NH_{4}^{+}$(完全固定),以及 (iii) 具有方向流动性的钉扎位点 $NH_{4}^{+}$(抑制平移,但允许旋转)。我们在不同的 $NH_{4}^{+}$ 负载量下评估了水传输和乙醇传输。与无 $NH_{4}^{+}$ 的情况相比,功能化通道呈现出三种与实验一致的趋势。首先,$NH_{4}^{+}$ 的流动状态强烈影响水传输,固定 $NH_{4}^{+}$ 作为“障碍”阻碍渗透,而旋转 $NH_{4}^{+}$ 作为“促进者”使渗透率几乎翻倍(图 3A)。其次,增加 $NH_{4}^{+}$ 负载量可能会放大这些相反的效果,在饱和状态(N-H / -F ≈ 1.39)下最为显著(图 3B)。第三,无论其流动性如何,$NH_{4}^{+}$ 功能化总是会降低乙醇的渗透(图 3℃)。

A

B

为了解释这种异常的水传输,我们首先重新审视了经典的“功能基团(载体)介导”传输理论,该理论将载体之间的分子迁移分为三个阶段(图 3D 和图 S26)(8, 9)。这一过程包括:(i) 捕获与释放,分子与第一个载体结合、重新定向并解离;(ii) 跳跃,解离的分子向相邻载体扩散;以及 (iii) 重新捕获与接力,分子被第二个载体重新结合,从而完成此次传输循环。我们的分析表明,旋转 $NH_{4}^{+}$ 重塑了所有三个阶段的水传输,将这一经典理论扩展到了动态载体。在阶段 1 中,它们通过缩短每个位点的水留存时间加速了捕获-释放过程,这可以通过 $NH_{4}^{+}$ 水合壳层寿命(局部水交换速率的指标)来量化。如图 3E 所示,旋转 $NH_{4}^{+}$ 的水合壳层寿命分布向更短的时间偏移(0 到 10 ps),而固定 $NH_{4}^{+}$ 则倾向于更长寿命的壳层(10 到 40 ps)。相应的平均寿命从 8.3 降低到 6.1 ps,表明 $NH_{4}^{+}$ 减少了局部陷阱并增加了每个位点的水交换周转率。

D

C

E

F

G

图 3. 动态功能介导的传输机制。(A) 无 $NH_{4}^{+}$、固定 $NH_{4}^{+}$ 或旋转 $NH_{4}^{+}$ 通道随时间的水渗透情况。(B) 不同 $NH_{4}^{+}$ 覆盖率通道的水渗透情况。(C) 无 $NH_{4}^{+}$ 以及具有固定或旋转 $NH_{4}^{+}$ 通道随时间的乙醇渗透情况。(D) 受限通道中 $NH_{4}^{+}$ 赋能的分子传输行为示意图。(E) 通道内围绕固定或旋转 $NH_{4}^{+}$ 的水分子的寿命分布。(F) 包含固定或旋转 $NH_{4}^{+}$ 通道内水分子的代表性轨迹。每条曲线代表一个单独的水分子,沿轨迹每隔 1 ps 的颜色演变表示其通过通道运动的时间进展。(G) 在具有固定或旋转 $NH_{4}^{+}$ 的通道内(包括互连和部分功能化两种情况),水传输过程中连续 $NH_{4}^{+}$-水碰撞的概率。插图显示了相应的整体 $NH_{4}^{+}$-水碰撞概率。

短暂的 $NH_{4}^{+}$-水接触事件(以下称为碰撞)通过瞬时能量和动量重新分布,重塑了阶段 2 的水运动。对标记水分子的碰撞后平移动能净变化的分析揭示了两种极限情况之间的对比(图 S27)。与固定 $NH_{4}^{+}$ 的碰撞对水动能产生的净影响可以忽略不计,而与旋转 $NH_{4}^{+}$ 的碰撞则导致显著的正动能增益 (19.1%)。因此,$NH_{4}^{+}$ 的旋转在近距离接触期间促进了向渗透水的瞬时动能转移。轨迹映射显示(图 3F 和图 S28A),这种额外的能量转化为更高的初始跳跃速度 (0.68 对比 0.26 nm ps $^{-1}$) 和更长的单步位移。因此,水分子的随机往复运动减少,总行程长度从 24.3 nm 减少到 16.3 nm,表明传输更具方向性(图 S28B)。此外,变温分子动力学(MD)揭示了水渗透率对 $NH_{4}^{+}$ 旋转速度的依赖性,进一步支持了这种动能转移机制(图 S29)。

此外,$NH_{4}^{+}$ 的旋转和互连相辅相成,增强了阶段 3 的水回收。由于水的释放和跳跃是随机的,下游 $NH_{4}^{+}$ 的回收能力本质上有限。我们在模拟过程中对 $NH_{4}^{+}$-水碰撞事件的追踪发现,当 $NH_{4}^{+}$ 位点既旋转又完全互连时,整体碰撞概率达到峰值 26.8%(图 3G,插图)。相比之下,固定 $NH_{4}^{+}$ 将该概率降低至 22.3%,这可能是因为受抑制的构型波动减少了其与水的有效接触截面。同样,从通道中部分移除 $NH_{4}^{+}$ 导致概率进一步下降至 9.3%,因为增加的位点间距延长了跳跃距离并降低了接触频率。

A

B

更重要的是,旋转和互连增加了通道内 $NH_{4}^{+}$ 与水分子连续碰撞的概率。如图 3G 所示,在旋转且互连的系统中,水分子发生多次碰撞(1 < n < 10)的概率最高(43%),而固定系统和部分功能化系统的概率分别为 36% 和 40%。总的来说,这些结果表明,$NH_{4}^{+}$ 的旋转和协同动力学将这些功能从原本的被动屏障转变为主动载体,从而在纳米通道沿线实现了快速的分子接力。相比之下,乙醇的传输一直受到抑制,因为 $NH_{4}^{+}$ 引起的空间位阻在通道入口处排除了大部分乙醇,并阻碍了其通过通道。

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动态功能化实现的溶剂分离

随后,我们研究了 $NH_{4}^{+}-M$ 依赖于旋转的传输特性如何缓解实际溶剂分离中的渗透率-选择性权衡 (36)。使用 90 wt % 的乙醇-水混合物作为模型系统(图 S30),我们发现 $NH_{4}^{+}-M$ 将水通量从 985 提高到 1422 g m $^{-2}$ h $^{-1}$ ,同时将乙醇通量从 39 降低到 4 g m $^{-2}$ h $^{-1}$ ,从而产生约 4000, 的分离因子,比未经处理的 untreated-M (240; 图 S31A) 高出一个数量级以上。这种选择性在不同的操作温度和进料组成下得以保持,证明了其性能的一致性(图 S31, B 和 C)。

共沸混合物在工业上难以通过常规蒸馏分离,因此为评估膜性能提供了一个严苛的基准。在使用 95 wt % 的乙醇-水共沸物进行测试时,$NH_{4}^{+}-M$ 实现了 3860, 的分离因子,远超 untreated-M 所获得的 167(图 4A)。在异丙醇-水和乙酸乙酯-水混合物中也观察到了类似的趋势(图 4, B 和 C),其中水渗透得到促进,而有机溶剂的传输被有效抑制。与此同时,

E

图 4. 分离性能。(A 至 C) untreated-M 和 $NH_{4}^{+}-M$ 在处理近共沸混合物时的溶剂-水分离性能,包括 (A) $40^{\circ}C$ 下的 95 wt % 乙醇-水,(B) $40^{\circ}C$ 下的 90 wt % 异丙醇-水,以及 (C) $50^{\circ}C$ 下的 94 wt % 乙酸乙酯-水。(D) $NH_{4}^{+}-M$ 在处理 95 wt % 乙醇-水混合物时的长期运行稳定性。(E) $NH_{4}^{+}-M$ 的乙醇-水分离性能与已报道膜的比较。

$NH_{4}^{+}-M$ 表现出强健的结构和化学稳定性(图 S15, S32 和 S33),在水-乙醇二元条件下(图 4D)以及在工业相关的含杂质条件下(图 S34)的长期连续运行中,均提供了稳定的分离性能。总的来说,这些结果表明,具有动态功能性的膜可应用于实际的脱水工艺,并提高能源效率(图 S35)。

动态功能化策略被扩展到了氧化石墨烯 (GO) 膜(图 S36)。尽管通道宽度略有减少(10.5 到 9.2 Å),但 $NH_{4}^{+}$ 功能化的 GO 表现出增强的水传输并阻碍了乙醇渗透(图 S37),这与在 MXene 系统中确定的传输机制一致。最后,与最先进的聚合物膜、二维膜、混合基质膜和商业膜的比较证实,$NH_{4}^{+}-M$ 在低至中等温度下运行,其性能超越了传统的渗透率-选择性上限(图 4E 和表 S2)。

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结论

我们确定纳米通道动力学是除通道几何结构和表面化学之外,实现传输控制的一种极具前景的途径。利用功能基团的固有迁移率(以自旋转的 $NH_{4}^{+}$ 为例),可将静态通道转化为动态传输环境,从而实现快速且选择性的亚纳米传输。这些动力学增强了能量传递和连续的分子跳跃,扩展了主要针对静态功能基团开发的载体介导传输理论,并实现了超越传统渗透性-选择性权衡的溶剂分离。除了旋转之外,这一原理还可以扩展到具有平移或振动自由度的功能基团,为调节纳米受限传输提供了一种模块化路径 (1, 37)。结合其他动态构建模块 (37, 38),它可以实现纳米流体器件、分离膜和离子导体中的定制传输。

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致谢

我们感谢上海交通大学(SJTU)仪器分析中心的 J. Wu 和中国科学技术大学(USTC)物理科学仪器中心的 R. Gao 在核磁共振(NMR)测量方面提供的帮助以及富有价值的讨论。我们还感谢 Monash X-ray Platform 的设施使用以及 J. Ma 提供的帮助。H.Z. 感谢中国国家留学基金管理委员会和昆士兰大学提供的奖学金。本工作还得到了澳大利亚核科学技术组织(ANSTO)、莫纳什大学电子显微镜中心以及昆士兰大学显微分析中心的资源支持。资金支持:Y.K. 和 C.H.L. 感谢欧盟 Horizon 2024 研究与创新计划在 Marie Skłodowska-Curie 资助协议(编号 101203526)下提供的支持。C.H.L. 感谢工程与自然科学研究委员会(EPSRC)为其 EPSRC 研究员计划(EP / X042286 / 1)提供的资金。X.Z. 感谢澳大利亚研究理事会(ARC)为其 ARC Future Fellowship(FT210100593)以及 ARC 二氧化碳绿色电化学转化卓越中心(CE230100017)提供的支持。J.Z.L. 和 F.F. 感谢澳大利亚研究理事会提供的 ARC Future Fellowship(FT220100149)。作者贡献:概念化:H.Z., Y.K., X.Z.;正式分析:H.Z., Y.K., F.F., T.H., J.Z.L., H.W., X.Z.;资金获取:Y.K., C.H.L., J.Z.L., X.Z.;调查:H.Z., Y.K., F.F., T.H.;方法论:H.Z., Y.K., T.H., R.X., H.Y., K.H., Z.Y., Z.W.;项目管理:Y.K., J.Z.L., X.Z.;资源:R.X., H.Y., C.H.L., Z.-X.L., Q.G., X.Z.;软件:F.F., T.H., Q.G., J.Z.L.;监督:Y.K., J.Z.L., X.Z.;验证:H.Z., Y.K., Q.G., J.Z.L.;可视化:H.Z., Y.K., R.X.;初稿撰写:H.Z., Y.K.;审阅与编辑:Y.K., Z.-X.L., J.Z.L., H.W., 和 X.Z.。竞争利益:作者声明不存在竞争利益。数据、代码和材料可用性:所有数据均可在正文或补充材料中获得。所有材料的合成和表征详情见补充材料。许可信息:版权所有 © 2026 作者,保留部分权利;独家许可方为美国科学促进会(AAAS)。对美国政府原始作品不主张权利。https: / www.science.org / about / science-licenses-journal-article-reuse

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补充材料

材料与方法;补充文本;图 S1 至 S37;表 S1 和 S2;参考文献 (39–104)

2025年11月11日提交;2026年8月25日接收

二维材料

对对称性破缺陈绝缘体及其量子熔融的可视化

Minhao He $^{1\dagger}$ , Yen-Chen Tsui $^{1\dagger}$ , Ran Peng $^{2}$ , Kenji Watanabe $^{3}$ , Takashi Taniguchi $^{4}$ , Oskar Vafek $^{2,5}$ , Ali Yazdani $^{1*}$

在磁场存在的情况下,莫尔量子材料的电子态会产生霍夫施塔特能谱(Hofstadter spectrum),这为研究能带拓扑与强电子-电子相互作用之间的相互作用提供了一个独特的环境。利用扫描隧道显微镜,我们研究了与六方氮化硼对齐的双层石墨烯中的霍夫施塔特态,并直接可视化了相互作用驱动的对称性破缺陈绝缘体(Chern insulators)的形成。我们的测量结果揭示了在霍夫施塔特能带的分数填充下,形成了将莫尔原胞扩大为两倍、三倍或四倍的相,以及具有复杂原胞内波函数的态。我们在不同的陈态中可视化了两种截然不同的量子现象,包括由拓扑缺陷的出现和增殖驱动的量子熔融,以及与相竞争和相分离共现的量子相变。

磁场与晶格周期性之间的相互作用会产生分形能带,这最早由 Hofstadter 预言 (1)。霍夫施塔特模型最初在电子系统中被提出,此后已在广泛的实验平台中实现,例如波导阵列 (2)、光学晶格 (3, 4)、超导量子比特链 (5),或通过制造横向人工超晶格的 GaAs / AlGaAs 异质结构 (6)。由扭转或晶格失配形成的堆叠范德华材料中的莫尔超晶格,为研究霍夫施塔特能谱及其拓扑结构提供了一个理想平台。早期实验 (7–9) 已经证明,当霍夫施塔特子带填充至单粒子能隙时,会出现被称为陈绝缘体 (CIs) 的拓扑态。每个陈绝缘体可以用两个量子指数来描述:陈数 C (10) 和能带填充指数 s (11)。最近,利用扫描隧道谱 (STS) 检测到了产生这些不可压缩态的分形霍夫施塔特能谱 (12)。

当霍夫施塔特子带的带宽变得狭窄且与库仑相互作用相当时,在子带的部分填充下会出现异常的相关拓扑相 (13, 14)。在这种情况下,仅凭拓扑不变量 (C 和 / 或 s) 无法提供完整的描述,因为它们对任何对称性破缺的出现并不敏感。结果是,根本不同的多体态可能共享相同的拓扑指数,但在其底层的微观对称结构上有所不同。强相互作用霍夫施塔特态的理论预测包括两种可能的基态:与分数电荷相关的准粒子不可压缩态 (15–18),以及破缺莫尔平移对称性的相 (19)。尽管这些相存在于各种基于石墨烯的莫尔材料中 (13, 14, 20–23),但尚未对这些强相互作用霍夫施塔特态的波函数和对称性进行微观研究 (24)。一个同样重要的开放性问题是,驱动此类相失去破缺对称性或拓扑序的量子相变的性质。

最近的扫描隧道显微镜(STM)测量已经证明,在针尖与样品功函数失配极小的情况下,能够对精细的电子相进行成像(25–27)。在这项工作中,我们报告了利用 STM 对与六方氮化硼(h-BN)完全对齐的伯纳尔堆叠双层石墨烯(BLG)中对称性破缺的霍夫施塔特状态(Hofstadter's states)进行直接成像,并将其相关的量子熔融过程可视化。我们利用光谱测量来识别各种 CI 绝缘相(通过测量其 C 和 s),并发现了对称性破缺的陈绝缘体(SBCIs),它们将莫尔原胞扩大了两倍、三倍或四倍,其中一些具有复杂的原胞内结构。我们的方法还可以用于直接可视化 SBCIs 和 CIs 的量子熔融过程,而这一过程对于宏观平均技术来说一直无法实现。

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莫尔超晶格与霍夫施塔特状态的出现

本文研究的 BLG 器件与 h-BN 基底完全对齐。图 1A 显示了超净区域内典型的恒流形貌图,提取的莫尔周期 $\lambda$ 为 $14.28\mathrm{nm}$,这与完全对齐的 BLG / h-BN 的超晶格周期一致 (28, 29)。在垂直磁场 $B = 14\mathrm{T}$ 下,达到了高达 $\phi / \phi_0 \approx 0.6$ 的磁通比,从而实现了分形霍夫施塔特(Hofstadter)能谱中电子波函数的实空间成像。此处,$\phi = B\left(\sqrt{3} \times \lambda^2 / 2\right)$ 是穿过一个莫尔原胞的磁通量,$\phi_0 = h / e$ 是磁通量子,其中 $h$ 是普朗克常数,$e$ 是基本电荷。

在图 1B 中,我们展示了在该区域 $B = 13.8\mathrm{T}$ 时测得的 STS 随栅极电压 $V_{G}$ 的变化关系。与之前关于不对齐 BLG / hBN 样品的研究 (26) [图 S1,S1 节 (30)] 类似,我们器件中(hBN 仅位于 BLG 的一侧)强烈的固有位移场 ($D_{0}$) 消除了最低 8 个朗道能级 (LLLs) 的层简并,并倾向于首先填充底层极化(靠近 hBN 侧)的 LLs。由于距离隧道探针较远,这使得 $V_{G} < 0$ 时的谱权重弱于 $V_{G} > 0$ 时。尽管如此,我们观察到了与 hBN 不对齐样品之间的显著差异,包括一系列额外的不可压缩状态(图 1B)。当电子极化到底层 ($V_{G} < 0$) 时,我们观察到剧烈的峰值能量偏移(在远程能带中也可见),这标志着在与 LL 填充因子 $v_{LL} = -3, -2, -1$ 处的量子霍尔铁磁体不同的载流子密度下,化学势在不可压缩状态之间发生了跳跃 [图 1B 和图 S2,S2 节 (30)]。这些状态突显了当电子极化在莫尔界面附近时产生的强莫尔效应,并且可以被归类为霍夫施塔特能谱中的 CIs。CIs 仅在 $B = 6\mathrm{T}$ 以上被观察到 [图 S3,S3 节 (30)],这进一步支持了上述结论。当电子极化到顶层 ($V_{G} > 0$) 时,我们仍然观察到了额外的霍夫施塔特状态,但其谱特征要弱得多 [图 S4,S4 节 (30)],表明莫尔效应较不明显。

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识别 CI

我们首先通过确定量子指数 $C$ 和 $s$ 来识别每个 CI。我们仔细检查了 $V_{G} < 0$ 时的 Hofstadter 态,重点关注费米能级(偏置电压 $V_{B} = 0$)附近的谱特征。不可压缩能隙被识别为隧道阈值能隙 $\Delta_{t}$ 中的峰值,该能隙由起始隧道电流定义 [图 S5,第 S5 节 (30)]。我们进行了随磁场变化的 STS 测量以构建 Wannier 图(图 1℃),该图绘制了载流子密度 $n$ 与每个 moiré 晶格单元的磁通量 $\phi / \phi_{0}$ 之间的关系,其中每个不可压缩态遵循一条直线(图 S6 和 S7)。根据这些直线的斜率和截距,我们利用丢番图关系 $n / n_{s} = C\phi / \phi_{0} + s$ 确定了陈数 $C$ 和能带填充指数 $s$。这里,$n_{s} = 1 / (\sqrt{3} \times \lambda^{2} / 2)$ 是对应于周期为 $\lambda$ 的每个 moiré 晶格单元中 1 个电子的载流子密度。我们的测量涵盖了很大范围的磁场,特别是在磁通比 $\ / \phi_{0} = 1 / 2$ 附近,正如预测的那样,我们在那里观察到了色散 Hofstadter 子能带的谱特征 [图 S8,第 S6 节 (30)]。我们对观察到的状态进行了分类 [图 S9,第 S7 节 (30)],并在图 1℃ 中总结了完整的相图,包括在 $V_{\mathrm{G}} > 0$ 时进行的类似测量(图 S10 和 S11)。

A

C

B

D

图 1. Bernal 堆叠双层石墨烯 / hBN 异质结构中 Hofstadter 能谱的光谱研究。(A) 一个具有双层石墨烯 / hBN moiré 周期结构的器件的清晰形貌图。黑色标尺为 50 nm。插图显示了形貌图的傅里叶变换。moiré 的布拉格峰由红圈标出,相应的周期为 14.28 nm。插图的白色标尺为 0.5 nm $^{-1}$。(B) 在 B = 13.8 T, $\ / \phi_{0} = 0.588$ 时测量的密度(由栅极电压 $V_{G}$ 调节)依赖性 STS。纵轴是针尖偏置电压 $V_{B}$,其中 $V_{B} > 0$ ($V_{B} < 0$) 探测电子(空穴)激发。在 $V_{G} > 0$ ($V_{G} < 0$) 时,电子远离(靠近)moiré。绝缘能隙可以被识别为费米能级处的能隙开启。相对于电荷中性点,$V_{G} > 0$ 处开启的能隙与 $V_{G} < 0$ 处是不对称的。顶部横轴显示了 LL 填充因子 $v_{LL}$。dl / dV 为微分电导(详见材料与方法)。(C) 在密度 $n / n_{s}$ 依赖性 STS 中观察到的绝缘相随 $\ / \phi_{0}$ 变化(对于 $\ / \phi_{0} > 1 / 2$)的 Wannier 图。拓扑指数 (C, s) 列在上方,并由公式 $n / n_{s} = C\ / \phi_{0} + s$ 表征。彩色线代表相应的 (C, s) 态,橙色点代表数据点。所有数据均在有效温度 $T_{eff} = 210$ mK 下采集。IQH,整数量子霍尔能隙;FQH,分数量子霍尔能隙。(D) $\ / \phi_{0} = 1 / 2$ 时色散能带结构的示意图。显示了由磁平移对称性强制产生的 2 个相同的磁子能带。(E) 当磁通进一步增加至 $\ / \phi_{0} > 1 / 2$ 时,每个磁子能带的最小值形成了 LLs。这里,对于 (C, s) = (-2, 1) 态,最低的 2 个简并 LLs 被完全填充(黑点表示在磁场 B 下完全填充)。(F) 当我们半填充最低的 2 个简并 LLs 时,通过自发打破 moiré 平移对称性,形成了一个相互作用驱动的 SBCI 态 (C, s) = (-1, 1 / 2)。

莫尔势主要影响 $V_{G} < 0$ 时的相图,此时载流子密度在最靠近莫尔势的层中进行调节。在此机制下,我们观察到四组遵循序列 $(C, s) = [-2(N + s_{0}), N](N = 0, 1, \ldots)$ 的陈绝缘体(CIs),每组在不同的密度 $-s_{0} = 0, -1, -1.5$ 和 -2 处穿过 $\phi / \phi_{0} = 1 / 2$。这些 CIs 可以理解为在 $\phi / \phi_{0} = 1 / 2$ 时,色散磁子带的最大值或最小值发生朗道量子化而产生(图 1, D 和 E)。换句话说,当磁通 $\$ 从半磁通量子偏移时,这些色散磁子带极值附近的电子轨道根据失谐磁通比 $\delta\ = \ / \phi_{0} - 1 / 2$ 被量子化为朗道能级(LLs)。$\ / \phi_{0} = 1 / 2$ 时的磁子带可以使用磁平移群(MTG)的本征函数来构建 (3I)。通常,对于磁通 $\ / \phi_{0} = p / q$ 且朗道规范 $\mathbf{A} = (0, Bx, 0)$,磁晶格动量写为 $k = k_{1}g_{1} = k_{2}g_{2}$,其中 $k_{1} \in [0, 1)$ 且 $k_{2} \in [0, 1 / q)$。莫尔超晶格的离散磁平移对称性要求子带能量在 $k_{1} \to k_{1} + 1 / q$ 下是简并的 [section S8 (30)]。因此,在磁通 $\ / \phi_{0} = 1 / 2$ 时,只要平移对称性得以保持,磁子带以及磁通偏离半磁通时出现的 LLs 就是二重简并的 (3I)(图 1D)。这反过来解释了为什么每组中保持平移对称性的状态的陈数彼此之间相差偶数。为了证明这一点,考虑在半磁通时,从电中性点价带子带的最大值处耗尽两个 LLs,如图 1E 的示意图所示。此类状态的填充率为 $n / n_{\mathrm{s}} = -2\delta \ = -2(\ / \phi_0 - 1 / 2)$,对应于 $(C,s) = (-2,1)$(图 1E)。更一般地,耗尽 $2N$ 个此类 LLs 会产生序列 $(-2N,N)$。具有非零 $s_0$ 的序列可以类似地理解为:首先将费米能级置于半磁通时色散子带之间的陈数 $-2s_0$ 能隙中,然后耗尽 $2N$ 个半磁通偏移的 LLs。此时此类状态的填充率为 $n / n_{\mathrm{s}} = -2s_0\ / \phi_0 - 2N(\ / \phi_0 - 1 / 2)$,从而导致观察到的序列 $(C,s) = [-2(N + s_0),N]$。请注意,由于每个子带携带一个整数陈数,$2s_0$ 是一个整数(可以是偶数或奇数)。

更值得注意的是,我们还观察到了具有整数 C 但分数 s 的相互作用 Hofstadter 态 (13, 14)。这些状态可能的基态候选者包括具有破缺莫尔平移对称性的电荷密度波(CDWs)(14, 21–23)。随着一个方向上的平移对称性破缺,$k_{1}$ 和 $k_{1} + 1 / 2$ 状态之间的简并度被解除,这使得单个半磁通偏移的 LL 可以在陈数 -4 能隙之上被填充,导致 $(-3, -1 / 2)$,或者从电中性点陈数 0 能隙开始被排空,导致 $(-1, 1 / 2)$(图 1F)。然而,此类对称性破缺状态从未在实验上被证实,因为之前的研究缺乏微观信息。

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可视化陈绝缘体及其对称性破缺

为了确定分数填充下的陈绝缘体(CIs)是否破坏了任何平移对称性,我们使用扫描隧道显微镜(STM)直接可视化其电子态密度的空间结构。我们在小偏压下测量了隧道电流的空间调制 $\delta / I_{dc} / $ [附录 S9 (30)]。正如预期的那样,$(C, s) = (2, 1)$ 的陈绝缘体积分态密度图保持了莫尔平移对称性,如图 2A 所示。这一点在图 2F 所示的结构因子 $S(\bar{q})$ 中得到了进一步确认 [附录 S9 (30)],其中在 $C_{3}$ 对称性下出现了六个尖锐的莫尔布拉格峰(红色六边形)。值得注意的是,$(C, s) = (4, 1)$ 的陈绝缘体虽然保持了莫尔平移对称性,但产生了一种具有莫尔原胞内结构的涌现 Kagome 电荷序(图 2B)。这一特征导致了图 2G 中出现更高阶的布拉格峰(蓝色圆圈)。这种丰富的莫尔原胞内结构凸显了原胞内库仑相互作用的重要性 (32),即使是在 $(C, s)$ 为整数的陈绝缘体情况下也是如此。

莫尔平移对称性破缺的特征出现在分数 $s$ 的陈绝缘体 STM 图像中,例如图 2℃ 所示的 $(C, s) = (1, 1 / 2)$ 状态。我们测得的是一种具有重构原胞(绿色矩形)的条纹状电荷序,而非原始的三角形莫尔平移对称性。由这些图像构建的结构因子 $S(\overline{q})$ 图(图 2H)显示, $C_{3}$ 对称的莫尔布拉格峰(红色六边形)消失,而出现了新的 $C_{2}$ 对称布拉格峰(绿色正方形)。主布拉格峰出现在莫尔超晶格倒格向量 $b$(在图 2F 中标出)的一半位置,表明条纹电荷序的实空间周期是莫尔晶格常数的两倍。我们的观察结果与在 Hofstadter 子带半填充时电荷密度波(CDW)使莫尔原胞倍增的情况一致。我们观察到具有有限陈数 $C$ 的 CDW,这与之前报道的被称为广义维格纳晶体 (33) 的莫尔共度 CDW 不同,后者在拓扑上是平凡的。

我们的成像实验确定了整数 $C$ 和分数 $s$ 情况下的基态为预期的对称性破缺陈绝缘体(SBCIs)。我们的实验证明,所有具有整数 $C$ 和分数 $s$ 的不可压缩状态都表现出这种行为,包括那些在 $V_{G} > 0$ 时的状态 [图 2, D, E, I 和 J,以及图 S13 至 S15,附录 S10(30)]。图 2D 显示了 $(C, s) = (2, 1 / 3)$ 状态的 STM 成像,其显示出莫尔原胞三倍大小的结构(橙色平行四边形)。相应的 $S(\overline{q})$ 图(图 2I)也显示了相应的 $C_{3}$ 对称布拉格峰(橙色六边形),出现在 $ / b / \sqrt{3}$ 的倒格向量处。这与 Hofstadter 子带三分之一填充的最简单图景一致,即一个电子电荷分布在三个莫尔原胞中。此外,我们表明破缺的平移对称性可以采取比现有预测更复杂的形式,例如在 $(C, s) = (1, 1 / 2)$ 的情况下(图 2E)。能带填充指数 $s$ 表示半填充的 Hofstadter 子带,在最简单的情况下,这对应于两个莫尔原胞中的一个电荷。相反,我们观察到了使原胞四倍化的电子结构(粉色平行四边形)。相应地,在 $S(\overline{q})$ 图(图 2J)中出现了六个量级为 $ / b / 2$ 的尖锐峰。我们的实空间成像表明,$(C, s) = (1, 1 / 2)$ 的 SBCI 对应于一个四倍重构的原胞,其中包含两个电子电荷。

除了丰富的单元格间重构外,我们还观察到这些 SBCI 具有复杂的单元格内结构,这可能是由于莫尔势的高次谐波引起,或者是由于强电子-电子相互作用而形成的。此外,我们还发现,在同一视野中,$(-1, 1 / 2)$ 条纹 SBCI 的方向在轻微电荷掺杂时会发生旋转 [图 S16, 第 S11 节 (30)],这表明该电子序与底层晶格或样品应变之间没有强耦合。然而,SBCI 的形成究竟是因为电子-声子耦合还是纯电子库仑相互作用,仍然是一个开放性问题。

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量子熔融与拓扑缺陷

我们的成像技术还能够直接研究由电子密度调控的 SBCI 量子熔融过程,并确定在这些相接近熔融时可能出现的拓扑缺陷的作用。在较大视野范围内对条纹 SBCI $(C, s) = (-1, 1 / 2)$ 进行成像(图 3A),我们观察到了许多显著特征,例如具有不同方向条纹的畴,以及分隔它们的边界。这三组条纹在快速傅里叶变换 (FFT) 图(图 3B)中产生了倒格波矢量 $q_{i=1,2,3}$,其数值为原始莫尔波矢量 $b_{i} / 2$ 的一半。我们采用一种分别研究单个条纹分量的分析方法来表征这种交织 的性质,该方法此前曾用于分析条纹相中的类似现象 (34, 35) [章节 S12 (30)]。

图 3, D to F, 分别显示了与 $\{q}_1$ 相关的条纹 的相对相位 $\varphi_{\boldsymbol{q}_1}(\boldsymbol{r})$、 幅度分布 $\rho_{\{q}_1}^o (\ {r})$ 以及余弦电荷调制 $\cos [\ {q}_1\cdot \ {r} + \varphi_{\{q}_1}(\ {r})]$。同样的操作可以针对 $\{q}_2$ 和 $\{q}_3$ 重复执行(图 S17)。图 3℃ 显示了归一化的

A B C E D

图 2. Cls 的直接成像。(A to E) 在 $B = 13.2\mathrm{T}$ [(A) to (C)] 或 $13.8\{T\}$ [(D) and (E)] 以及每个 $(C,s)$ 状态的低偏置电压 $V_{\{B}}$ 下测得的实空间隧道电流 $\delta / I_{\mathrm{dc}} / $ 图。白色比例尺为 $40~\{nm\}$。(F to J) 分别为面板 (A) to (E) 中隧道电流调制 $\delta / I_{\{dc\}} / $ 的结构因子 $S(\overline{q})$。比例尺为 $0.5\{nm}^{-1}$。双层石墨烯 / hBN 莫尔布拉格峰由红色六边形标出。[(A) and (F)] $(-2,1)$ 状态遵循莫尔平移对称性。(A) 中的红色平行四边形代表莫尔原胞。[(B) and (G)] $(-4,1)$ 状态的涌现 Kagome 晶格遵循莫尔平移对称性。Kagome 结构在 $S(\overline{q})$ 图 (G) 中表现为高次谐波(蓝色圆圈)。[(C) and (H)] $(-1,1 / 2)$ 状态通过使原胞翻倍打破莫尔平移对称性,并形成拓扑条纹相(绿色矩形为原胞)。涌现条纹相的布拉格峰被标为绿色正方形,条纹序可通过两个主布拉格峰来识别,其长度为倒格矢量 $(b) / 2$ 的一半。[(D) and (I)] $(2,1 / 3)$ 状态通过使原胞三倍打破莫尔平移对称性,并形成三角晶格 [橙色平行四边形 (D) 为原胞]。布拉格峰被识别为六个 $\sqrt{3}$ 橙色六边形 (I)。[(E) and (J)] $(1,1 / 2)$ 状态通过使原胞四倍打破莫尔平移对称性,并形成三角晶格 [粉色平行四边形 (E) 为原胞]。涌现三角晶格的布拉格峰被识别为六个粉色六边形 (J)。所有数据均在 $T_{\{eff\}} = 210\{mK\}$ 下采集。

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[⚠ 低质量翻译,建议复核] 图 3. SBCI($C = -1, s = 1 / 2$)的拓扑熔融。(A) 在 $B = 13.8$ T 和 $V_{\mathrm{B}} = 6$ mV 下测得的大尺度实空间隧道电流 $\delta / I_{dc} / $ 图。可以观察到具有三种不同方向的条纹。(B) 图 (A) 中 $\delta / I_{dc} / $ 图的快速傅里叶变换 (FFT)。不同方向的条纹由 $\boldsymbol{q}_{i=1,2,3}$ 矢量标识。比例尺为 $0.25$ nm $^{-1}$。(C) 三个 $\boldsymbol{q}_{i=1,2,3}$ 矢量的归一化振幅的实空间分布。(D) 提取的相对相位 $\varphi_{\{q}_1}(\{r})$ 图。其中拓扑缺陷由黑色(红色)虚线圆圈标识,相位的顺时针绕数(winding)为 $2\pi (-2\pi)$。黑色(红色)虚线圆圈代表位错(反位错)。(E) $\{q}_1$ 的振幅 $\rho_{\{q}_1}^o (\{r})$ 图,显示了沿 $\{q}_1$ 方向条纹的强度。(F) $\cos [\{q}_1 \cdot \{r\} + \varphi_{\{q}_1}(\{r\})]$ 图,具有偏移半个晶胞的锐利边界。(G) 跨越 SBCI($C = -1, s = 1 / 2$)绝缘能隙的密度依赖 STS。(H) 跨越能隙的 $\cos [\{q}_1 \cdot r + \varphi_{\{q}_1}(\{r\})]$ 图随 $V_{\mathrm{G}}$ 变化的选样图。顶行、中行和底行分别对应 $\{q}_1$、$\{q}_2$ 和 $\{q}_3$。图中的位错(反位错)被标记为黑色(红色)点。随着掺杂远离能隙中心($V_{\{G}} = -0.168$ V),拓扑缺陷的数量增加。(I) 拓扑缺陷数量(位错 + 反位错)随 $V_{\{G}}$ 变化的函数图。随着系统掺杂远离能隙中心,拓扑缺陷大量增加,表明 SBCI 条纹相通过一种拓扑驱动机制发生熔融。所有面板中的白色比例尺均为 $50~\{nm}$。所有数据均在 $T_{\{eff}} = 210$ mK 下采集。h-dope,空穴掺杂;e-dope,电子掺杂。

拓扑缺陷并未被钉扎在特定的形貌特征(如晶格点缺陷)上。相反,我们观察到在对 SBCI 进行掺杂时,拓扑缺陷的位置会发生变化(图 3H)。我们在图 3G 中展示了在 $(C, s) = (-1, 1 / 2)$ SBCI 附近门电压 $V_{\{G}}$ 下的放大 STS。我们在 8 个不同的 $V_{\{G}}$ 下对具有破缺平移对称性的电荷序进行了成像(图 S18 和 S19),并像图 3H 中那样分析了拓扑缺陷的位置和类型。将所有三个波矢量 $q_{i}$ 的拓扑缺陷总数绘制成图。

聚焦于图 3D 所示的相对相位 $\varphi_{\{q}_{1}}(\{r\})$, 我们讨论单一条纹方向内拓扑缺陷的存在。两种拓扑缺陷是位错和反位错,分别对应于条纹终止和条纹合并的地方。在相位图中,它们表现为奇异点:围绕位错的顺时针回路产生 $+2\pi$ 的相位绕数(黑色),而围绕反位错的顺时针回路产生 $-2\pi$ 的相位绕数(红色)。我们观察到一对位错和反位错;它们导致了图 3F 中分隔两个条纹区域的锐利边界,且偏移量为一个莫尔超晶格常数。一个值得关注的问题是,(反)位错是否携带分数电荷。

三个波向量 $q_{i}$ 的 SBCI 振幅分布,分别由红色、绿色和蓝色表示。我们发现,振幅分布分析表明所有三个方向可以相互共存。

在图 3I 中作为 $V_{G}$ 的函数。我们观察到,随着系统掺杂远离 $V_{G} = -0.168$ V 附近不可压缩能隙的中心,(反)位错的总数呈现增加趋势。我们的测量表明,该 SBCI 向可压缩相的量子相变是由拓扑缺陷的增殖介导的,这与 Kosterlitz-Thouless 相变一致 (36, 37)。

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量子熔融与相分离

最后,我们展示了一个通过相分离发生的陈绝缘体(CI)量子相变示例,以及相边界处拓扑边缘模的可能特征。图 4 显示了一系列在 $(C,s) = (-4,1)$ 附近(如图 4A 所示)的图像,该状态具有 Kagome 晶格结构(图 4B)。随着 $V_{\mathrm{G}}$ 的增加,发生了从不可压缩的 Kagome 陈相到另一种具有花瓣状电子结构的不可压缩相的量子相变 [图 S20, S13 节 (30)]。实空间图谱显示在此转变过程中存在相分离。随着 $V_{G}$ 的增加,Kagome 晶格区域缩小,而花瓣状区域扩大(图 4, C 至 E),最终填满了整个视野(图 4F)。图 4A 中的光谱显示,当 $V_{\mathrm{G}}$ 变化导致相边界经过 STM 针尖位置(红星,图 4, B 至 G)时,能隙关闭并重新打开,这表明边界包含一种无能隙模式,正如在 CI 边界所预期的一样 (38)。尽管我们未能在此转变的门电压依赖光谱中实验性地检测到迟滞现象,但相分离的观察结果表明,这种相互作用陈相的熔融是一个一级相变。最后,随着进一步的电子掺杂,花瓣状结构演变为一种表现出复杂原胞内结构的可压缩状态 [图 4G 和图 S20, S14 节 (30)]。

A B C D

图 4. Kagome CI 的相分离与量子熔融。(A) 在磁场 $B = 13.2\{T\}$ 下,$(C,s) = (-4,1)$ 状态附近的 STS。标注了 Kagome CI 的不可压缩光谱特征以及能隙关闭(橙色和黄色箭头之间)。能隙关闭发生在 (C) 和 (D) 中的锐利相边界经过针尖下方时,表明相边界是可压缩的。(B) 至 (G) 中图像的门电压由光谱右侧的有色箭头标出。(B) 在 $V_{\{G\}} = -1.982\{V\}$(红色)和 $V_{\{B\}} = 4.8\{mV\}$ 下测得的隧道电流 $\delta / I_{\{dc}} / $ 图谱显示了涌现的 Kagome 晶格。莫尔原胞用红色平行四边形标出。(C) 在 $V_{\{G\}} = -1.972\{V\}$(橙色)和 $V_{\{B\}} = 3.6\{mV\}$ 下测得的 $\delta / I_{\{dc}} / $ 图谱显示了 Kagome 晶格原子级锐利的相边界。(D) 在 $V_{\{G\}} = -1.962\{V\}$(黄色)和 $V_{\{B\}} = 5.6\{mV\}$ 下测得的 $\ / I_{\{}} / $ 图谱显示了不可压缩 Kagome 晶格与不可压缩花瓣状结构之间的相边界,且 Kagome 晶格岛在缩小。(E) 在 $V_{\{G\}} = -1.952\{V\}$(绿色)和 $V_{\{B\}} = 5.0\{mV\}$ 下测得的 $\ / I_{\{}} / $ 图谱。(F) 在 $V_{\{G\}} = -1.922\{V\}$(蓝色)和 $V_{\{B\}} = 4.0\{mV\}$ 下测得的 $\ / I_{\{}} / $ 图谱。整个视野被花瓣状电子结构填满。(G) 在 $V_{\{G\}} = -1.860\{V\}$(紫色)和 $V_{\{B\}} = 1.6\{mV\}$ 下测得的 $\ / I_{\{}} / $ 图谱。系统进入具有复杂原胞内结构的可压缩状态。所有 $\ / I_{\{}} / $ 图谱中的比例尺均为 $\$40~\{nm\}$。(B) 至 (G) 中的红星表示测量 (A) 中光谱时的针尖位置。所有数据均在 $T_{\{eff\}} = 210\{mK\}$ 下采集。

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结论与展望

我们的研究可视化了大量的 SBCI 状态,并直接确定了描述此类相的量子指数(C 和 s)与其波函数空间结构之间的关系,展示了扩大原胞的状态以及具有复杂原胞内结构的状态示例。关于是什么稳定了这些对称性破缺相的详细理解,仍需进一步的理论研究。我们还为关联相和拓扑相的量子相变提供了一个独特的视角,证明了 Kosterlitz-Thouless 型缺陷介导相变和相分离型相变均可发生。展望未来,当我们的技术应用于在场和零场分数量子陈绝缘体(CIs)的类似实验时,可以提供重要的新见解。一个值得关注的场景是在场分数量子陈绝缘体状态,因为理论研究预测拓扑缺陷将承载分数量子电荷并具有非阿贝尔统计特性 (39)。

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参考文献与注释

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致谢

我们感谢 T. Wang, J. Y. Lee, 和 M. Zaletel 提供的有益讨论。资金支持:本研究主要由 DOE-BES 拨款 DE-FG02-07ER46419、Gordon and Betty Moore 基金会的 EPIQS 计划拨款 GBMF9469,以及美国陆军研究办公室(US Army Research Office)授予 A.Y. 的 MURI 项目(拨款号 W911NF-21-2-0147 和 W911NF261A052)资助。实验工作的其他支持由美国国家科学基金会材料研究科学与工程中心(NSF-MRSEC)通过普林斯顿复杂材料中心 NSF-DMR-2011750、NSF 拨款 DMR-2312311、NSF 拨款 OMA-2326767 以及 ONR N00012-21-1-2592 提供。O.V. 部分得到了 Gordon and Betty Moore 基金会 EPIQS 计划(拨款号 GBMF11070)和 Simons 基金会拨款 SFIMPS-NFS00006741-09 的支持。A.Y. 感谢英国剑桥的三一学院、物理系和卡文迪许实验室的款待。作者贡献:M.H.、Y.-C.T. 和 A.Y. 设计了实验。M.H. 和 Y.-C.T. 创建了器件结构并进行了 STM 测量和数据分析。R.P. 和 O.V. 进行了理论计算。K.W. 和 T.T. 提供了 h-BN 基底。M.H.、Y.-C.T.、A.Y.、R.P. 和 O.V. 共同协作撰写了手稿。竞争利益:作者声明不存在竞争利益。数据、代码和材料可用性:本研究的数据可在 Figshare (40) 获取。所有化合物和材料的合成与表征详情见方法部分。许可信息:版权所有 © 2026 作者,保留部分权利;独家许可方为美国科学促进会(AAAS)。不对美国政府原始作品主张权利。

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补充材料

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science.org / doi / 10.1126 / science.aef0940

材料与方法;补充文本;图 S1 至 S20;参考文献 (41–44);视频 S1 提交于 2025 年 12 月 29 日;接收于 2026 年 7 月 24 日

比较认知

鸟类大脑中的超快速决策

Philipp Schmidbauer 和 Andreas Nieder\*

感知决策在哺乳动物中得到了充分研究,但在其他脊椎动物中的运作机制仍不清楚。我们证明,寒鸦(Corvus corone)在经典的视觉运动辨别任务中能以前所未有的速度做出审慎决策,平均报告选择的时间约为 235 毫秒,这大约比在猴子或人类中观察到的速度快两倍,且并未牺牲准确性。来自外套脑(pallial endbrain)的记录显示,方向选择性神经元在刺激出现后约 70 毫秒,以及在做出反应前约 170 毫秒就对即将做出的选择进行了编码,其活动呈递增趋势,并随感觉证据的增加而缩放,在反应开始时趋于一致。这些发现突显了鸟类决策电路的卓越效率,这可能是由快速视觉运动控制的进化压力所塑造的。

感知决策涉及整合感觉信息以引导对生存至关重要的行为 (1–3)。在执行随机点运动辨别任务的灵长类动物中,感知决策在数百毫秒内展开,后顶叶皮层的神经元在顺序采样动力学下积累感觉证据,直到其活动达到一个信号,表明已决定做出选择的阈值 (4–6)。目前尚不清楚这些经典的决策机制是哺乳动物新皮层特有的,还是可以通过不同的神经架构在其他脊椎动物中产生。

鸦科鸣禽(如渡鸦、乌鸦和蓝鸦)为解决这一问题提供了一个强大的比较模型,因为它们表现出高度复杂的感知和认知能力 (7–10)。在 3.6 亿 年前与哺乳动物分化之后 (11),鸟类进化出了一种独特的核外套层(nuclear pallium),它缺乏分层的新皮层 (12, 13),但保留了哺乳动物大脑特有的关键组织和计算原则 (14)。这些能力的核心是尾侧 nidopallium (NCL),这是一个位于鸟类外套层处理层级顶端的关联外套区域。NCL 被广泛认为是灵长类前额叶皮层的功能类似物 (15),支持乌鸦等智能鸟类灵活决策背后的执行功能 (16, 17)。

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乌鸦的运动辨别性能

为了研究鸟类感知决策的行为和神经相关因素,我们对两只寒鸦(*Corvus corone*)进行了测试。这些乌鸦经过训练,可以在一个经典的随机点运动任务中辨别视觉运动方向,该任务采用具有不同相干性的动态点图案(图 1A)(见材料与方法)。每轮试验在乌鸦将头部置于刺激屏幕前时开始,由红外光屏监测。点图案以 3%、9%、27% 或 81% 的相干性向四个方向之一(左对右或上对下)运动,此外还设有 0% 的随机运动条件。两个响应目标(左-右或上-下)位于中央刺激的两侧,乌鸦在离开光屏后通过啄击其中一个目标来报告其决定。

乌鸦 1 和 2 分别完成了 55 和 102 个 session,每 session 的平均正确试验数分别为 207 和 209,每 session 的平均总试验数分别为 276 和 285。总体选择准确率为 $75.0 \pm 0.4\%$ ( 1) 和 $73.4 \pm 0.3\%$ ( 2),且强烈依赖于运动强度(图 1B 和表 S1)。在 81% 相干性时,准确率达到上限( 1: $99.9 \ 0.1\%$ ; 2: $99.4 \ 0.2\%$ ),并随着运动强度的减弱而下降,在 9% 相干性时接近阈值( $\sim75\%$ )( 1: $78.5 \ 0.8\%$ ; 2: $71.8 \ 0.6\%$ )。两只乌鸦在 3% 相干性时的表现均高于随机水平( 1: $56.5 \ 0.8\%$ , $t_{(54)} = 7.8$ ; 2: $57.5 \ 0.7\%$ , $t_{(101)} = 10.9$ ,两者 P < 0.001;单样本 t 检验)。正如预期的那样,在 0% 相干性(此时“正确”方向被随机分配)时,选择在两个方向之间分布大致均匀( 1: $49.8 \ 1.0\%$ , $t_{(54)} = -0.25$ , P = 0.803; 2: $49.6 \ 0.7\%$ , $t_{(101)} = -0.6$ , P = 0.575;单样本 t 检验),表明不存在系统性的方向偏差。

反应时间(从刺激出现到头部运动开始的时间间隔)非常短,包含所有正确试验和 0% 试验且独立于选择的 session 中位数平均值为 $235 \ 2$ ms ( 1) 和 $235 \ 1$ ms ( 2)。反应时间随运动强度的变化幅度很小(图 1℃ 和表 S1),在 1 中范围从 220 (81% 相干性)到 254 (0% 相干性),在 2 中范围从 216 到 243 ,表明任务难度对决策时间的影响极小。两只乌鸦在水平(图 S1)和垂直(图 S2)目标布局中均显示出较小的准确率和反应时间偏差。在错误试验中,两只乌鸦的响应速度均显著慢于正确试验(图 S3),这与基于证据的审慎决策一致 (4)。

为了测试乌鸦的表现是否依赖于点密度、运动算法或运动开始后的短暂等待期,我们测试了四种在所有三个因素上均不同的经典随机点运动变体 (18)。在不同随机点运动刺激类型、点密度以及不存在短暂等待期的情况下,准确率和反应时间相当(图 S4)。在不存在短暂等待期时,1 的响应速度甚至略快。综合来看,这些结果表明,乌鸦准确且快速的决策不能用任务或刺激设计来解释,而更像是反映了一种内在的生物能力。

我们测试了记录期间乌鸦的表现是否符合决策的漂移扩散模型 (19, 20)。标准模型假设漂移率与感觉证据之间存在线性映射,但该模型未能很好地捕捉乌鸦的反应时间分布(图 S5 和 S6)。受心理物理学中已知的感知刺激强度与物理刺激强度之间非线性关系的启发,我们评估了相干性与漂移率之间的非线性映射。

指数函数 $(x^{1 / 2}, x^{1 / 3})$ 和对数函数 $(\log_{2}x)$ 与线性映射相比,均改善了模型拟合度 [乌鸦 1: $F_{(54)} = 1975.0, P < 0.001$ ; 乌鸦 2: $F_{(101)} = 3701.6, P < 0.001$ ; 重复测量方差分析 (ANOVA)]。对数映射为两只乌鸦都提供了最佳拟合 ( $P_{corrected} < 0.05$ , 事后配对 t 检验; 图 1, B 和 C, 绿线, 以及图 S5B 和 S6B), 这表明运动相干性与证据积累之间存在非线性关系。

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方向选择性 NCL 神经元预测行为选择

在任务执行期间,我们记录了 NCL 中 248 个神经元的活动(乌鸦 1:127 个;乌鸦 2:121 个;图 1D),已知 NCL 包含对随机点运动方向敏感的神经元 (21)。对于每个神经元,首选运动方向被定义为在决策形成期间(刺激出现后 80 ms 直至做出反应)诱发最高放电率的方向;相反方向被指定为非首选方向。

四分之一的神经元(58 / 248,23.4%)具有方向选择性,在正确试次中,首选方向的放电显著更强 [受试者工作特征 (ROC) 分析,$P < 0.05$]。首选方向的活动在刺激出现后稳步上升,在行为反应附近达到峰值,而非首选方向的反应则保持平稳(图 1, E 和 F)。

A

E

D

F

图 1. NCL 中的决策行为和运动方向选择性神经元。(A) 任务设计。试次开始于乌鸦将头部置于触摸屏前的一个光栅中。在刺激前周期之后,屏幕两侧出现两个选择目标,随后中心出现动态点刺激。乌鸦通过啄击相应的目标来报告感知的全局运动方向(箭头仅用于示意),并立即终止运动刺激。(B) 乌鸦 1 和 2 在五个运动相干水平(0 到 81%)下的辨别准确率(分别经过 55 和 102 个 session)。(C) 平均中值反应时间,测量时间从运动刺激出现到头部移出光栅。黑色圆圈表示 session 平均的行为数据(平均值 ± SEM);绿色曲线显示 session 平均的漂移扩散模型 (DDM) 拟合结果,阴影区域表示 SEM。(D) 乌鸦大脑的侧视图示意图,显示 NCL 中的记录位置(灰色)。Tel.,端脑;Cb,小脑;TeO,视顶盖。(E 和 F) 辨别首选和非首选(上 / 下)运动方向的示例神经元。试次分别与刺激出现(左)或反应出现(右)对齐。顶端面板显示脉冲光栅图(每条线代表一个试次;每个点代表一个动作电位),底端面板显示使用 100-ms 高斯核平滑后的脉冲密度函数。灰色阴影分别表示刺激出现时间和反应时间的分布。

群体分析显示,NCL 活动在早期就反映了即将做出的选择。在正确试次中(3 到 81% 相干度),首选方向的活动从刺激出现到反应持续上升(图 2A),在刺激出现后 67 ms 以及运动前 171 ms 与非首选活动产生分叉(滑动窗口 Wilcoxon 符号秩检验,$P < 0.05$,$n = 58$)。我们使用具有更大平滑窗口的滑动 Mann-Whitney U 检验验证了神经元选择性的时间进程,该方法降低了时间精度(图 S7),并获得了与原始分析密切匹配的时间估计值。

我们计算了 ROC 曲线下面积 (AUC),用于量化神经元的放电率在区分两种运动方向上的表现,其中 0.5 表示无区分能力,1.0 表示完美的区分能力。在所有神经元中,AUC 值均超过了 0.5 的随机水平(平均值 = 0.631,$t_{(57)} = 18.06$ , P < 0.001,单样本 t 检验),表明对运动方向具有显著的区分能力,并将 NCL 活动与乌鸦的感知决策联系起来(图 2B)。基于单个神经元在偏好方向与非偏好方向放电率的时间分辨滑动 ROC 分析,支持了在决策形成期间观察到的活动分离(图 S8)。

为了将感觉相关活动与选择相关活动分开,我们分析了按选择侧分组的随机运动试次(0% 相干性)。即使在没有方向性运动线索的情况下,NCL 活动也能预测选择:偏好信号与非偏好信号在刺激出现后 96 ms 以及响应前 99 ms 出现分叉(在正确试次中分别为 69 和 161 ;P < 0.05, n = 56)(图 2℃),且 AUC = 0.569($t_{(55)} = 5.21$ , P < 0.001;单样本 t 检验;图 2D)。

错误试次显示出类似的模式。当乌鸦尽管运动方向向非偏好侧但仍选择偏好目标时,NCL 活动类似于正确的偏好方向响应,反之亦然(图 2E)。在正确试次中,分叉发生在刺激出现后 63 ,而在错误试次中则发生在 113 (分别在响应前 171 与 55 ;P < 0.05, n = 49)。错误试次中的 AUC 值(平均值 = 0.571,$t_{(48)} = 4.87$ , P < 0.001;单样本 t 检验;图 2F)证实了选择相关的编码。

基于正确试次放电率训练的支持向量机 (SVM) 分类器成功解码了正确试次 (87.3%)、随机运动试次 (72.5%) 和错误试次 (67.7%) 中选择的方向,表现优于随机打乱的对照组(第 95 百分位数 = 65%;图 2G)。这些结果表明,NCL 活动独立于感觉输入地编码决策结果。

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NCL 神经元编码感觉证据

我们接下来研究了运动相干性如何调制方向选择性活动(图 3)。在刺激开始后以及反应发生前瞬间,群体活动随运动相干性而缩放(图 3A)。展示运动相干性依赖性活动的单神经元示例见图 S9。对于每个神经元,决策形成期间的平均归一化活动随首选方向的相干性增加而增加 $t_{(42)} = 3.00, P = 0.002$(单样本 t 检验;图 3, B 和 C),但在反首选方向则没有增加 $t_{(42)} = 0.70, P = 0.246$。群体活动随时间追踪运动相干性,直到决策时期的后期才变得与相干性无关(图 S10)。因此,NCL 神经元同时编码了决策结果和感觉证据的数量,这对应于由运动相干性提供并逐渐累积的信息,以达到决策阈值。

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图 2. 方向选择性 NCL 神经元的群体活动编码了选择。(A) 在正确试次(3 到 $81\%$ 相干性)中,所有方向选择性神经元( $n = 58$ )在首选(蓝色)和反首选(红色)方向上的归一化活动,分别与刺激开始(左)或反应开始(右)对齐,并使用 100-ms 高斯核进行平滑。阴影表示神经元间的 SEM。黑色条表示首选和反首选活动之间的显著差异(滑动窗口 Wilcoxon 符号秩检验,50-ms 窗口,1-ms 步长,$P < 0.05$)。灰色阴影分别表示反应和刺激开始时间的分布。(B) 正确试次中方向选择性神经元的 AUC 分布。AUC 根据刺激开始和反应之间的脉冲率计算。箭头表示平均值;星号表示显著 $>0.5$ 的值(单侧单样本 $t$ 检验)。(C) 正确试次中方向选择性神经元( $n = 56$ )的活动,同 (A)(首选,蓝色;反首选,红色),以及随机运动试次( $0\%$ 相干性;所选目标,浅蓝色 / 橙色),按乌鸦选择的目标进行分组。(D) 随机运动试次中的 AUC 分布。(E) 正确试次(首选,蓝色;反首选,红色)和错误试次(浅蓝色 / 橙色)中方向选择性神经元( $n = 49$ )的归一化活动。错误试次按乌鸦选择的目标进行分组,该目标与刺激方向相反。(F) 错误试次中的 AUC 分布。(G) 基于正确试次脉冲率训练的 SVM 分类器的准确率( $n = 48$ 个神经元;10,000 次重复),并在正确、随机运动和错误试次上进行测试。对照组显示了标签置换后的性能;虚线表示对照分布的第 95 百分位数。

为了将神经元动力学与感觉证据(即运动相干性)联系起来,我们量化了首选方向上的爬升率(ramping rates),即每秒活动的增加量。爬升率是在以群体信号拐点(刺激后 110 ms)为中心的 150-ms 窗口内提取的。平均爬升率随运动相干性而增加,尽管增幅较小 $(t_{(42)} = 1.64, P = 0.055;$ 单样本 t 检验;图 3, D 和 F)。

由于行为建模揭示了运动相干性与证据积累之间存在对数关系,我们测试了上升率(ramping rates)是否遵循类似的模式。上升率与运动相干性的线性回归显示,对数尺度上的拟合效果 $(R^{2}=0.83, P=0.032)$ 优于线性尺度 $(R^{2}=0.65, P=0.103;$ 图 3E)。在所有神经元中,对数尺度上的斜率分布显著高于零 $(t_{(42)}=2.17, P=0.018;$ 图 3F),证实了上升率与对数转换后的运动相干性之间存在稳健的正相关关系。这反映了行为学所提示的,作为感觉证据的运动相干性与积累率之间的非线性关系。

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NCL 神经元的决策相关动力学

为了将决策信号动力学与行为联系起来,试验根据反应时间被分为短、中、长三类(图 4 和图 S11)。脉冲密度函数显示,在刺激出现后,长反应时间试验中的活动上升速度比短或中反应时间试验慢(图 4A,左),证明了决策时间与上升率之间存在紧密耦合。然而,当以反应开始时间为基准对齐时,所有反应时间组都表现出相似的时间概貌(图 4A,右),其活动在反应前 50 ms 内的纯前运动期趋向于一个相似的水平(图 4B;短:$0.99 \pm 0.19$ SD;中:$0.67 \pm 0.21$ SD;长:$0.77 \pm 0.27$ SD;$\chi^{2}_{(2)} = 4.42$ , P = 0.110;Kruskal-Wallis 检验)。这种近似的收敛与证据积累的阈值式终止是一致的,尽管缺乏

完全的收敛表明 NCL 活动并非由一个简单的固定阈值控制。事实上,最近在猴子外侧顶内区(lateral intraparietal area)使用类似任务的研究揭示了反应概貌存在显著的异质性,仅有一部分神经元显示出经典的上升至阈值(ramp-to-threshold)活动,而其他神经元则表现出被认为反映决策置信度的相干性依赖反应 (22)。因此,与外侧顶内区一样,额外的认知变量可能会调节 NCL 中与选择相关的活动,从而导致反应开始时放电率的异质性。

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乌鸦的快速决策:跨物种比较

我们证明了乌鸦 NCL 中的神经元编码了运动方向决策的稳健神经相关物,其时间动态与顺序采样下的证据积累一致,并且与新皮层中的经典决策过程高度平行 (4–6, 22–26)。即使在没有明确要求快速响应的情况下,乌鸦在各种运动相干度下报告运动方向的头部运动平均时间为 235 ms,同时保持了高准确率。相比之下,即使猴子和人类使用眼跳(灵长类动物中最快的刻意运动响应之一,潜伏期短至 $\sim 70$ ms,通常为 $\sim 140$ ms (27, 28))尽可能快地报告运动方向,尽管乌鸦使用的是高惯性的头部运动(图 S12),其反应时间仍大约是乌鸦的两倍。

在高度匹配的自定步调随机点运动任务中,猴子在三个研究中、在相当的运动相干度水平下表现出的反应时间分别为 $\ 410$、$\ 490$ 和 $\ 600$ ms (29-31)(图 S12)。灵长类动物在某些条件下可以表现出极快的响应 (32–34),但这些研究与此处使用的经典随机点运动范式有显著不同,特别是在任务结构、刺激属性和时间限制方面。猴子在自定步调随机点运动任务中的反应时间与人类执行相同任务时的反应时间相当,后者在三个研究中显示的平均反应时间分别为 $\ \$ 450$、$\ \$ 510$ 和 $\ \$ 820$ ms (35–37)(图 S12)。执行自定步调随机点运动任务的大鼠显示的平均反应时间在 $\ \$ 500$ 到 1000 ms 之间,具体取决于刺激难度,因此比猴子慢 (38)。蚂蚁和蜜蜂也能做出快速的视觉辨别决策,但这些结果与乌鸦和猴子的随机点运动研究不具有直接可比性,因为任务和决策范式存在根本差异 (39, 40)。

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图 3. 群体活动也反映了感觉证据的数量。(A) 方向选择性神经元($n = 43$)在不同运动相干度下的归一化活动,分别对齐至刺激开始(左)或反应开始(右)。实线表示乌鸦选择该神经元偏好目标的试次;虚线表示非偏好选择。活动使用 100-ms 高斯核进行平滑,并在神经元之间取平均值。灰色阴影分别表示反应和刺激开始时间的分布。(B) 在偏好和非偏好方向上,从刺激开始 80 ms 后到每次试次反应期间,不同运动相干度下的平均活动。灰色线显示单个神经元中相干度依赖性活动的平均线性拟合。(C) 对每个神经元活动进行线性拟合所得斜率的分布,分为偏好选择(上)和非偏好选择(下)。(D) 每秒归一化活动的平均增量($\Delta \text{rate}_{\text{norm}} / \text{s}$)随运动相干度的函数关系。误差棒表示神经元间的标准误差(SEM);黑线显示线性拟合($R^2 = 0.65$)。(E) 平均爬升率随运动相干度在对数尺度上的函数关系。黑线显示对数尺度上的线性拟合($R^2 = 0.83$)。(F) 对每个神经元的爬升率在线性(上)和对数(下)运动相干度尺度上进行线性拟合所得斜率的分布。

图 4. 方向选择性神经元的反应时间依赖性活动。试次按反应时间分组(短:175 至 225 ;中:230 至 280 ;长:285 至 335 )。(A) 按反应时间分组的方向选择性神经元的归一化群体活动(短:n = 58;中:n = 58;长:n = 43),对齐至刺激(左)或反应开始(右)。实线显示使用 100- 高斯核平滑后的偏好方向活动;灰色阴影表示反应前分析窗口。(B) 每个反应时间组在偏好和非偏好方向上,在反应前 50 内的平均归一化活动 [见 (A) 右图中的灰色阴影]。误差棒表示神经元间的标准误差(SEM)。

乌鸦做出决定的速度大约是灵长类动物的两倍,且没有牺牲准确性。这种表现表明,其证据积累和决策承诺速度更快,而非在速度-准确度权衡中发生了偏移。在刺激开始后约 70 以及行为反应前约 170 迅速出现的选择选择性 NCL 活动进一步支持了这一结论。

乌鸦的超快决策速度可能部分反映了鸟类视觉系统的高时间精度,这可能是由快速感觉-运动处理的选择压力所塑造的。鸟类表现出极高的时间视觉分辨率,某些鸣禽能够分辨频率高达 145 Hz 的闪烁光(临界闪烁融合频率)(41, 42)。在神经元层面,快速视觉处理得到了快速视网膜脉冲传导 (43) 和高效的鸟类视顶盖逃逸通路(tectofugal pathway)的支持,其中视顶盖反应在刺激开始后约 5 内出现 (44, 45),下游的圆核(rotundus)活动在约 20 内出现 (46)。虽然这些潜伏期与灵长类动物的早期视觉反应重叠,但它们表明视觉信号通过鸟类视顶盖逃逸通路快速传播至更高阶的处理阶段。这种快速的早期视觉处理,结合紧凑的鸟类外套层(pallium)中较短的传导距离和密集的循环连接 (15–17, 47, 48),可能促进了感觉证据向感知决策的高效转换,且在各个处理阶段累积的微小潜伏期优势加速了“感知-行动”循环。

综上所述,这些研究结果表明,鸦科动物的 NCL 代表了一种感知决策的趋同演化方案。它在截然不同的神经架构中支持着类似于灵长类动物的计算动力学,且具有显著更高的时间效率。这种速度可能反映了鸟类在视觉运动控制方面所承受的演化压力,以实现快速的喙部运动、捕食者检测以及飞行导航 (49, 50)。

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致谢

我们感谢 Z. Hafed 在生成运动刺激方面的帮助。作者贡献:P.S. 和 A.N. 设计了实验。P.S. 执行了实验。P.S. 和 A.N. 分析了数据。P.S. 和 A.N. 撰写了手稿。P.S. 和 A.N. 编辑了手稿。A.N. 监督了本研究。竞争利益:作者声明不存在竞争利益。数据、代码和材料可用性:用于重现分析和图表的数据可在 Figshare 数字存储库 (51) 中获取。许可信息:版权 © 2026 作者,保留部分权利;独家许可方为美国科学促进会(AAAS)。不对美国政府原始作品主张权利。https: / www.science.org / about / science-licenses-journal-article-reuse

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补充材料

材料与方法;表 S1;图 S1 至 S12;参考文献 (52–56);

MDAR 可重复性检查清单

提交日期:2025年11月4日;接收日期:2026年8月25日

10.1126 / science.aed6459

二维材料

广义维格纳晶体量子熔融中的电子-空穴不对称成像

Emma Berger $^{1,2,*}$ $\dagger$ , Michael Arumainayagam $^{1}$ $\dagger$ , Zhihuan Dong $^{1}$ , Lucas Schneider $^{1}$ , Tianle Wang $^{1,3}$ , Greyson Nichols $^{4}$ , Salman Kahn $^{1,5}$ , Rwik Dutta $^{6}$ , Gaoqiang Wang $^{7}$ , Takashi Taniguchi $^{8}$ , Kenji Watanabe $^{9}$ , Mit H. Naik $^{6,10}$ , Michael P. Zaletel $^{1}$ , Feng Wang $^{1,5,11,*}$ , Michael F. Crommie $^{1,5,11,*}$

二维莫尔材料为探索强关联系统中的相变提供了一个多功能平台。利用扫描隧道显微镜,我们对具有三角形莫尔超晶格的电子掺杂、近60°扭转二硒化钼双层材料中广义维格纳晶体(GWC)和莫特绝缘体(MI)的密度驱动熔融进行了成像。我们观察到 GWC 熔融中显著的电子-空穴不对称性:空穴掺杂的 PLOS 产生了相互作用驱动的无序状态,而电子掺杂的 PLOS 则熔融为离域的类液体状态。这种不对称性源于莫尔超晶格破缺的粒子-空穴对称性,这导致 凝聚时产生了具有不同动量几何结构的电子和空穴费米口袋。MI 状态的熔融则没有这种不对称性,这与缺乏对称性破缺的密度调制相一致。这项工作为 PLOS 在经历量子熔融转变时出现的涌现相提供了直接的可视化。

当强相互作用电荷被放置在二维(2D)周期性晶格上时,共度相与非共度相之间的竞争预计会导致新的多体状态。这些状态包括“弹珠液体”(1–4)、无序的“电子泥”(5–11)以及向列相液晶(12),其中势能与动能的平衡导致了局域化、离域化和无序的异常组合。理解这些相之间由密度调控的“量子熔融”转变是凝聚态物理中的一个核心挑战,与从受挫磁性(13, 14)到高温超导(15, 16)的许多领域相关。由扭转原子级薄材料制成的莫尔超晶格是探索这种行为的理想平台,因为它们承载了强关联的广义维格纳晶体()(17–20)和莫特绝缘体(MI)(21–25)状态,且可以通过静电门控进行连续掺杂。莫尔系统中量子熔融的一些证据已经通过体相表征技术(26, 27)被观察到,但由于这些技术缺乏直接可视化,其微观机制尚未被充分理解。例如,电子-电子相互作用与淬火无序的各自作用仍然不清楚。扫描隧道显微镜(STM)非常适合探索这一课题,因为它能够将电子结构和无序成像至原子尺度(28–33)。尽管 STM 已被用于成像过渡金属硫族化合物(TMD)莫尔双层材料中的共度 (18, 34),但 在被掺杂至非共度填充状态时的量子熔融尚未被可视化。

在这项研究中,我们报道了在扭转角接近 $60^{\circ}$ 的电子掺杂二硒化钼同质双层(tMoSe $_{2}$)中,广义瓦尔登晶体(GWC)和莫特绝缘体(MI)状态量子熔融的 STM 成像,该系统具有三角形莫尔超晶格。我们观察到,在莫尔超晶格的共度填充略有偏离时,密度调控的 GWC 熔融呈现出显著的电子-空穴不对称性:空穴掺杂倾向于产生相互作用驱动的无序状态,而电子掺杂则诱导产生均匀的、离域的类液体状态。这一趋势在 v = 1 / 2 的条纹有序 以及 v = 2 / 3 的蜂窝有序 中均有观察到,其中 v 是每个莫尔原胞中的电子数。相比之下,在 v = 1 时对 MI 状态进行掺杂,无论掺杂极性如何,均会导致均匀的类液体状态。我们的图像表明,空穴掺杂 中的无序主要由关联效应驱动,而淬火无序有助于稳定一组近简并状态。这些结果与之前的理论工作一致,即预测莫尔系统在非共度填充时会出现相互作用驱动的无序相(5–8, 11, 12, 35),但我们对 PLOS 量子熔融中强电子-空穴不对称性的实验观察是出乎意料的。利用 Hartree-Fock 框架,我们证明了这种行为的产生是因为掺杂的空穴和电子占据了涌现 布里渊区中的不同区域。

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tMoSe$_{2}$ 中 GWC 的 STM 成像

我们在图 1A 中概述的实验装置由一个接近 $60^{\circ}$ 的 tMoSe$_{2}$ 同质双层组成,该双层由一个约 60-nm 厚的六方氮化硼 (hBN) 绝缘体支撑,并放置在 Si / SiO$_{2}$ 晶圆之上。为了降低接触电阻并实现对裸 TMD 表面的 STM 成像,我们使用石墨纳米带阵列与 $_{2}$ 建立电接触 (29–33, 36, 37)。$_{2}$ 的载流子密度通过在 Si 基底和石墨接触之间施加背栅电压 ($V_{G}$) 来控制,而隧道电流是通过在该接触相对于接地的 针尖施加偏置电压 ($V_{B}$) 来获得的 (38)。图 1B 显示了扭转角约为 $\sim$ $ 57.4$° 的 $_{2}$ 莫尔图案的典型 形貌图,对应的莫尔晶格常数约为 $\sim$ $ 7.4$ nm(所有 数据均在 T = 4.8 K 下采集)。图 1℃ 的形貌放大图显示了 $_{2}$ 莫尔原胞中的三个不同堆叠位点(MX、XX 和 MM,其中 M = Mo 且 X = Se;图 1D)。掺入 $_{2}$ 导带 (CB) 的电子占据低能 MM 堆叠位点 [见 (38) 的第 2 节] (33, 39, 40)。

图 1E 显示了在改变 $V_{G}$ 和 $V_{B}$ 时,将针尖保持在 MM 位点上方所获得的 隧道电流。“直接”隧道效应发生在 $V_{B} > 0$ 时,此时电子从 针尖隧道传输到 $_{2}$ 导带中的空状态(图 1F)。“带隙内”隧道效应发生在 $V_{B} < 0$ 时,此时电子从 $_{2}$ 导带隧道传输到针尖,而针尖的费米能级 ($E_{F}$) 位于 $_{2}$ 的带隙内(因此称为“带隙内”,ingap)(图 1G)(29–31, 33)。图 1E 中围绕 $V_{B} = 0$ 的暗区代表宽度为 $\Delta V_{B}$ 的隧道能隙,在此范围内没有 电流流动。这归因于针尖与表面之间功函数不匹配导致的能带弯曲、石墨与 $_{2}$ 之间的接触电阻以及关联电荷能隙的共同作用 (29, 33, 41, 42)。在特定 $V_{G}$ 值处 $\Delta V_{B}$ 的增强(白色箭头)与莫尔超晶格的共度填充相一致,如图 1E 所示 [详见 (38) 的第 3 节]。我们将 $\Delta V_{B}$ 的这些增加归因于绝缘 GWC 和 MI 状态特有的关联电荷能隙,这些状态需要额外的能量来产生带电激发 (34)。由于样本的不均匀性和针尖门控效应的存在,电荷能隙在 $V_{G}$ 方向上有所展宽 (42)。

这些 和 MI 状态及其相应的结构因子 $S(\boldsymbol{k})$ 的图像可见于图 2,范围为 $1 / 3 \leq v \leq 2$ [原始图像见 (38) 的图 S1]。我们通过调节 $V_{\text{B}}$ 来最小化 针尖与 $_2$ 之间的电场,以减少针尖的扰动效应 [见 (38) 的第 4 节] (29–31, 33)。$\nu = 1 / 3$ 和 4 / 3 处的 显示为三角形晶格(图 2, A 和 I),$\nu = 1 / 2$ 和 3 / 2 处的 显示为条纹序(图 2, B 和 J),而 $\nu = 2 / 3$ 和 5 / 3 处的 显示为蜂窝晶格(图 2, C 和 K)。相应的结构因子显示了 布拉格峰(绿色圈出)和莫尔布拉格峰(紫色圈出),后者也是高阶 布拉格峰。应变诱导的各向异性导致 $\nu = 1 / 2$ 和 3 / 2 处的条纹序与电子-电子间距最大的方向一致 [见第 5 节

[38)]。对于 $\nu \leq 1$ 的 GWC 模式与此前使用二硫化钨 (WS$_2$) / 二硒化钨 (WSe$_2$) 异质双层结构中的石墨烯传感器层器件几何结构所成像的模式相似 (18, 34),但由于此处 STM 成像是直接在裸 TMD 表面上进行的,因此空间分辨率有所提高。对于分数 $\nu' > 1$ 成像的 GWC 与 $\ = \' - 1$ 的 GWC 相似,不同之处在于每个莫尔位点多了一个电子的背景。整数填充 $\ = 1$ 和 2(图 2, D 和 L)表现出与莫尔超晶格相同的三角形晶格,分别对应于 Mott 绝缘体状态和能带绝缘体状态 (21–24)。$\ = 2$ 时的莫尔位点看起来比 $\ = 1$ 时的位点更大,但 $\ = 2$ 时的单个电子无法被分辨 [与 tWS$_2$ 不同 (33)],这可能是由于位内电子-电子相互作用与莫尔势能级分离的相对贡献所致 (40, 43)。

图 1. 器件几何结构和 STM 测量方案。(A) tMoSe$_2$ 器件示意图。将一个扭转角约为 57.4° 的 MoSe$_2$ 同质双层放置在 SiO$_2$ / Si 基底上的 hBN 绝缘层之上。在接地的 STM 针尖与接触 tMoSe$_2$ 的石墨纳米带阵列之间施加偏置电压 ($V_B$)。在 tMoSe$_2$ 与 Si 基底之间施加背栅电压 ($V_G$)。(B) tMoSe$_2$ 莫尔超晶格的大面积形貌图,其中 Z 表示形貌高度(电流 $I = 1$ nA, $V_B = 1.5$ V, $V_G = 60$ V)。(C) (B) 中白色虚线区域内形貌的特写,采用相同的扫描参数。(D) 在 (C) 中识别的高对称莫尔原胞区域的原子堆叠配置(蓝色,Mo;红色,Se)。(E) 针尖位于 MM 位点上方时获取的恒定高度栅极扫描 $I-V_B$ 曲线。图中标出了相关绝缘能隙(白色箭头)。$\ = 5 / 3$ 处的能隙看起来被抑制了,因为针尖位于 $\ = 5 / 3$ 蜂窝图案中一个被双占据的 MM 位点之上(设定点:$I = 5$ nA, $V_B = 1.$ V, $V_G = 70$ V)。(F 和 G) (F) “直接”隧穿 ($V_B > 0$) 和 (G) “能隙内”隧穿 ($V_B < 0$) 技术的示意图。所有 STM 数据均在 $T = 4.8$ K 时采集。

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GWC 量子熔融中的电子-空穴不对称性

图 3 展示了 $\nu = 2 / 3$ GWC 的量子熔融随电子密度的变化情况。在空穴掺杂的 GWC 区域($\nu = 2 / 3 - \delta = 0.61$;图 3A),我们观察到一种无序相,其空间和动态上的局部电子密度是不均匀的,其特征是取决于位置和 $\$ 的电报噪声 [section 6 of (38)]。研究发现,无序图案中隧道电流的位点间变化与点缺陷的位置无关 [section 9 of (38)]。随着电子密度增加到 $\ = 0.63$,蜂窝图案开始出现(图 3B),到 $\ = 0.66$ 时,图案移动了一个晶格位点,并凝固成更稳定的蜂窝电荷有序态(图 3℃)。左下角的均匀电荷密度显示了一个熔融区域,用一条绿线标出以指示畴壁熔融前沿。随着进一步的电子掺杂($\ > 0.66$),该畴壁从图像的左下角向右上角推进,直到整个区域的电子密度变得均匀(图 3, D to F, 以及图 S2)。在均匀的电子掺杂相中未观察到电报噪声。熔融前沿的运动遵循莫尔晶格的应变梯度(图 3G),因为单位晶格较小的局部区域需要更高的电荷密度才能达到相同的 $\$ [details in section 7 of (38)]。空穴掺杂和电子掺杂情况下电荷分布的显著差异在图 3H 中得到了进一步量化,该图显示了 $S(\pmb{k})$ 中 GWC 傅里叶峰的积分强度 $\rho_{\mathrm{g}}$ 随 $\$ 的变化关系。在 $\ = 2 / 3$ 附近,由于稳健的蜂窝有序,$\rho_{\mathrm{g}}$ 达到最大值(图 3H 插图),随后随着 $\$ 的进一步增加而剧烈衰减。另一方面,当 $\$ 降低到 $\ = 2 / 3$ 以下时,$\rho_{\mathrm{g}}$ 的衰减较为缓慢。$\ \sim 0.64$ 处 $\rho_{\mathrm{g}}$ 的轻微下降对应于两个移动了一个晶格位点的蜂窝有序态之间不稳定的转变,这短暂地削弱了长程有序。

在 $\ = 1 / 2$ 的条纹有序 GWC 中也观察到了类似的量子熔融掺杂不对称性(图 4)。在这里,空穴掺杂区域($\ = 1 / 2 - \delta = 0.46$)表现出以位点间强度变化、短程条纹、柱状二聚体以及少量残余 $\ = 1 / 3$ 三角形畴为特征的无序状态(图 4A)。与 $\ = 2 / 3 - \delta$ 的情况一样,$\ = 1 / 2 - \delta$ 时的无序电子密度与点缺陷的位置无关 [section 9 of (38)]。随着电子密度达到 $\ = 1 / 2$,在空穴掺杂区域看到的短条纹开始伸长(图 4B),此时,两个巨大的、高度有序的条纹 GWC 畴结晶,并由一个无序边界分隔。这两个畴之间相对移动了一个莫尔晶格位点,这可能是由于不同的缺陷诱导钉扎势所致。与空穴掺杂相反,对条纹 GWC 进行电子掺杂($\ = 1 / 2 + \delta = 0.58$)会导致条纹有序通过一个遵循应变梯度的畴壁熔融前沿的推进而熔融成均匀状态(图 4℃;完整的 $\ = 1 / 2$ 熔融系列见图 S3)。

对 $\nu = 1 / 2 - \delta$ 的 $S(\mathbf{k})$ 进行检查显示,空穴掺杂导致条纹 GWC 的傅里叶峰发生分裂,这与短程向列序的出现一致(图 4D,蓝色虚线椭圆)。随着 $\nu \rightarrow 1 / 2$,分裂的峰合并,表明条纹伸长为更稳健的条纹序(图 4E)。电子掺杂的行为则截然不同,因为对于 $\nu = 1 / 2 + \delta$,条纹序峰的强度单调下降而非分裂(图 4F)。这一点在图 4G 中得到了突出显示,该图显示了在 $\nu$ 变化时,$S(\mathbf{k})$ 中沿 $q$ 方向(上方插图)穿过条纹序峰的线切图。空穴掺杂侧的分裂对应于 $\Delta q = 1 / l_{s}$,其中 $l_{s} \sim 20$ nm(2 到 3 个莫尔晶格常数;下方插图)是缩短条纹的平均长度。这种电子-空穴不对称性在条纹序 $S(\mathbf{k})$ 峰的积分强度中也有体现,由于短程条纹序的存在,仅在空穴掺杂侧出现肩峰(蓝色箭头)(图 4H)。

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$\nu = 1$ 莫特绝缘体的量子熔融

在 $\nu < 1$ 的 GWC 量子熔融中观察到的电子-空穴不对称性,在 $\ = 1$ MI 状态的量子熔融中并不存在(图 5)。相反,MI 状态在两种掺杂极性下均熔融为空间均匀状态,且没有电子无序。这可以从 $\ = 1$ 附近拍摄的能隙内隧道电流图(图 5A)中看出,该图显示了由应变诱导的不均匀性引起的三个具有不同电子占据率的区域:(i) $\ = 1 - \delta \approx 0.95$(底部),(ii) $\ \approx 1$(中间),以及 (iii) $\ = 1 + \delta \approx 1.10$(顶部)。这些状态的拟议能带排列草图见图 5B。区域 (ii) 呈暗色且无特征,因为其填充对应于有能隙的 MI 状态,且针尖和样品的费米能级均位于莫特能隙之内(这与图 2D 不同,图 2D 是在更负的 $V_{B}$ 下获取的,允许 MI 中的电子隧道传输到针尖)。另一方面,区域 (i) 相对于 $\ = 1$ 是空穴掺杂的,导致莫特能隙坍塌并形成一个可压缩状态,电子可以在其中自由地隧道传输到针尖。区域 (iii) 中的莫特能隙同样坍塌,只不过此时样品是电子掺杂且 $\ > 1$。对于两种掺杂极性,熔融状态在空间上都是均匀的,没有出现掺杂诱导的电子无序迹象(大规模图像见图 S4)。由于包含第二个电子的概率增加,区域 (iii) 中的电子掺杂位点看起来比区域 (i) 中的位点更大。

图 2. GWC 和 MI 状态的图像。(A 至 D) $\text{tMoSe}_{2}$ 中相关绝缘体状态的能隙内隧道电流图,分别为 (A) $\ = 1 / 3$, (B) $\ = 1 / 2$, (C) $\ = 2 / 3$, 以及 (D) $\ = 1$。相应的结构因子 $S(k)$ 如图 (E 至 H) 所示。(I 至 L) $\ > 1$ 时观察到的状态电流图,分别为 (I) $\ = 4 / 3$, (J) $\ = 3 / 2$, (K) $\ = 5 / 3$, 以及 (L) $\ = 2$。相应的结构因子 $S(k)$ 如图 (M 至 P) 所示。$S(k)$ 中与三角形莫尔晶格和 GWC 序相关的傅里叶峰分别用紫色和绿色圆圈标出。原始 STM 图像已减去一个平面;原始数据见图 S1。所有 $S(k)$ 图均使用未裁剪的能隙内隧道电流图通过全尺寸自相关函数计算得出。

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讨论与展望

我们的数据表明,GWC 量子熔化存在显著的电子-空穴不对称性:空穴掺杂的 GWC 产生了与淬火无序无关的电子无序,而电子掺杂的 GWC 则产生了均匀的类液体相。这与之前的光学测量 (27) 一致,该测量检测到了在 $\nu = 1 / 2$ 附近掺杂的 $WS_{2} / WSe_{2}$ 异质双层中 GWC 量子熔化的不对称性。使用经典 (12, 27, 35) 和量子 (6, 7) 模型的理论研究也预测了不同的不共度相,从费米液体 (6, 44) 到由竞争电荷序产生的无序状态,这些预测与我们的观察结果大致一致 (5–7)。然而,之前的理论或实验研究都没有清晰地捕捉到我们所观察到的显著的电子-空穴熔化不对称性。为了解释这一行为,我们进行了自洽 Hartree-Fock (SCHF) 计算,求解了一个由填充度在 $\nu = 1 / 2$ 和 2 / 3 附近的三角晶格电子组成的扩展 Hubbard 模型。我们的处理提供了一个框架,展示了莫尔三角晶格的粒子-空穴不对称性 (45) 如何导致我们在实验中观察到的 GWC 熔化不对称性。

图 3. $\ = 2 / 3$ GWC 的量子熔化。(A 至 F) $\ = 2 / 3$ 填充附近带隙隧道电流图,分别为 (A) $\ = 0.61$, (B) $\ = 0.63$, (C) $\ = 0.66$, (D) $\ = 0.68$, (E) $\ = 0.70$, 以及 (F) $\ = 0.72$。畴壁(绿线)将熔化区域与电荷有序区域分开。(G) 与 (A) 至 (F) 相同区域的莫尔原胞面积图,带有 10-nm 比例尺。(H) 蜂窝序 GWC 傅里叶峰(插图,蓝色圆圈)的积分强度 $\rho_{g}$ 随 $\$ 的变化函数($\rho_{g}$ 由莫尔傅里叶峰的积分强度归一化)。(I) $\ = 2 / 3$ 时沿 rBZ 中 K-Γ-K' 路径的 SCHF 能带。rBZ 见插图(实线),莫尔布里渊区作为参考(虚线)。在 $\ = 2 / 3$ 时,化学势 $\mu_{v} = 2 / 3$(红色虚线)位于 LHB 和 UHB 之间。掺杂在 $\ = 2 / 3$ 之上的电子占据 rBZ 边缘(实心圆),而空穴掺杂则从 rBZ 中心移除电子(空心圆)。

E

H

图 5. $\ = 1$ MI 状态的量子熔化。(A) $\ = 1$ 附近的带隙隧道电流图。应变变化导致三个截然不同的掺杂区域:(i) $\ = 1 - \delta \approx 0.95$ , (ii) $\ \approx 1$ , 以及 (iii) $\ = 1 + \delta \approx 1.10$ ,其中 $\$ 是根据括号区域内的平均原胞面积估算的。区域 (ii) 呈现暗色,因为针尖费米能级位于 Mott 能隙内,这与图 2D 不同,后者是在更负的 $V_{B}$ 下采集的。(B) 样品和针尖状态密度 (DOS) 的示意图,显示了它们在三个区域中的能级对齐情况:对于区域 (ii),样品和针尖的化学势均位于 MI 能隙中,不发生带隙隧道传输。对于区域 (i) 和 (iii),对 MI 进行电荷掺杂导致 Mott 能隙坍塌,从而产生带隙隧道

电流能够流动。我们的出发点是将 $\nu = 2 / 3$ 的广义瓦尔特-克里斯蒂安(GWC)状态视为三角晶格上的电荷密度波(CDW),它将单个部分占据的莫尔(moiré)导带折叠成还原布里渊区(rBZ)内的三个能带(图 3I;在此处理中忽略了自旋)。通过在自洽哈特里-福克(SCHF)框架下求解扩展哈伯德模型,我们发现 CDW 势在 rBZ 边缘的顶层两个能带 [即下哈伯德带(LHB)和上哈伯德带(UHB)] 之间开启了一个关联能隙,从而降低了系统的总能量。由此产生的电子-空穴不对称能带结构在 LHB 和 UHB 之间表现出间接能隙。电子掺杂 UHB 会在 rBZ 边界(靠近 $K$ 和 $K'$)填充状态,这会使 $\nu = 2 / 3$ 的 GWC 不稳定,因为系统随后可以通过关闭 能隙并熔融成液体状态来降低其

能量。相比之下,空穴掺杂 LHB 会排空区中心(靠近 $\Gamma$)的状态,因此使 能隙保持原位,且电荷有序部分保持完好。实验中观察到的 GWC 序参数

图 4. $\ = 1 / 2$ GWC 的量子熔融。(A 至 C) $\ = 1 / 2$ 填充附近 (A) $\ = 0.46$、(B) $\ = 0.50$ 和 (C) $\ = 0.58$ 的能隙内隧道电流图。相应的结构因子 $S(\boldsymbol{k})$ 如图 (D 至 F) 所示 [蓝色虚线椭圆突出了用于计算 (H) 中 $\rho_{g}$ 的条纹有序傅里叶峰]。(G) $S(\boldsymbol{k})$ 中条纹有序傅里叶峰随 $\$ 变化的线切图。(上插图)红色虚线表示沿 $q$ 轴线切的方向。(下插图)$\ = 0.45$ 处的线切图(黑色虚线)显示了傅里叶峰的分裂。(H) 蓝色椭圆内条纹有序傅里叶峰的积分强度 $\rho_{g}$ 随 $\$ 的变化。$\rho_{g}$ 由莫尔傅里叶峰的积分强度归一化。蓝色箭头指示了 $\ = 1 / 2$ 空穴侧的一个不对称肩峰。

$(\rho_{\mathrm{g}})$(见图 3H)在我们的 SCHF 计算中得到了定性地重现(图 S11)。正如 (38) 的第 8 节中所讨论的,$\ = 1 / 2$ 的情况与之类似。由于在 $\ = 1$ 时没有自发产生的 ,该机制也解释了 MI 状态缺乏电子-空穴不对称熔融的原因。

因此,电子掺杂的 GWC 会因为 GWC 能隙的崩溃而熔融成均匀相,产生由有利于电子离域的量子涨落所稳定的类液体状态 (6, 44, 46)。另一方面,空穴掺杂的 GWC 保留了一个有限的关联 能隙,从而产生反映不同电荷有序之间竞争的无序状态。我们的数据表明,我们观察到的无序状态是由电子-电子相互作用驱动的,因为我们发现隧道电流强度的点对点变化与点缺陷的空间配置之间没有相关性。电报噪声(竞争有序的标志)也仅在空穴掺杂的情况下被观察到。我们在空穴掺杂 $\ = 1 / 2$ 和 $2 / 3$ GWC 中观察到的无序性,还与理论预测的在不共度填充下即使在没有淬火无序的情况下也会出现的无序“电子泥浆(electron-slush)”状态 (5–8, 10) 一致。例如,经典蒙特卡罗模拟预测,由于相互作用驱动的短程向列无序,在 $\ = 1 / 2 - \delta$ 时 $S(\boldsymbol{k})$ 的条纹有序峰会发生分裂,这与我们的实验结果一致(图 4, D 和 G)(12, 27, 35)。

尽管电子-电子相关性驱动了无序状态,但材料本身的固有无序可能会稳定这种由相互作用驱动的无序。我们在扫描背栅电压时,未在电子无序图案中观察到迟滞现象,这意味着淬火无序(quenched disorder)钉扎了在大量简并无序状态中的一小部分子集。实验中观察到的电报噪声可能源于这些竞争基态之间的波动(图 3, A 和 B,以及图 S9)。我们的数据与之前的理论预测一致,即淬火无序应当能稳定相互作用驱动的“电子泥浆”(electron slush)相 (7, 47)。

我们观察到 GWC 量子熔融在 v = 1 / 2 和 2 / 3 时存在显著的电子-空穴不对称性,其中空穴掺杂有利于电子无序态,而电子掺杂则有利于类液体态。这种不对称性在 SCHF 理论层面可以解释为:电子口袋与空穴口袋在动量空间几何结构上的差异强烈影响了 GWC 的稳定性。我们的结果表明,即使在存在淬火无序的情况下,电子-电子相互作用也能产生新的电子无序相。未来的温度依赖性和动力学测量将有助于量化相关性驱动的电子无序态的能量学。

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致谢

我们感谢与 V. Dobrosavljević 的有益讨论,以及 Z. Ge、Z. Xiang 和 Q. Li 提供的实验建议。资金支持:美国能源部科学办公室基础能源科学材料科学与工程部,在 van der Waals 异质结构计划 KCWF16 下的合同 DE-AC02-05-CH11231(M.F.C.、F.W.、M.P.Z.:STM 成像,SCHF 理论)。国防部 Vannevar Bush 教职研究员奖学金 N00014-23-1-2869(M.F.C.:器件制备)。国家科学基金会奖励 DMR-2528960(M.F.C.:电报噪声分析)。国家科学基金会研究生研究奖学金计划,资助编号 DGE 2146752(E.B.)。德国研究基金会(DFG, German Research Foundation)项目编号 529232793(L.S.:博士后奖学金)。国家科学基金会 MRSEC DMR-2308817(M.H.N.)。德克萨斯大学奥斯汀分校的德克萨斯高级计算中心(TACC)(M.H.N.、R.D.:DFT 计算)。通过高级网络基础设施协调生态系统:服务与支持(ACCESS)计划的分配 PHY250206 使用的德克萨斯大学奥斯汀分校 Stampede3 计算设施,该计划由国家科学基金会资助项目 2138259, 2138286, 2138307, 2137603, 和 2138296 支持(M.H.N.、R.D.:DFT 计算)。德克萨斯量子研究所研究生奖学金(R.D.)。JSPS KAKENHI 资助 21H05233 和 23H02052(K.W.、T.T.:hBN 晶体制备)。CREST 资助 JPMJCR24A5(K.W.、T.T.:hBN 晶体表征)。日本文部科学省(MEXT)的 JST 和世界顶尖研究中心计划(WPI)(K.W.、T.T.:hBN 合成开发)。作者贡献:概念化:M.F.C.、F.W.;监督:M.F.C.、F.W.;器件制备:E.B.、M.A.、G.N.、S.K.;hBN 晶体生长与表征:K.W.、T.T.;测量:E.B.、M.A.、L.S.、G.W.;SCHF 计算:Z.D.、T.W.、M.P.Z.;DFT 电子结构计算:R.D.、M.H.N.;数据分析:E.B.、M.A.、L.S.;写作:E.B.、M.A.、L.S.、M.F.C.。竞争利益:作者声明没有竞争利益。数据、代码和材料可用性:正文和补充材料中显示的所有数据均可在 Zenodo (48) 上获取。所有化合物和材料的合成与表征详情见方法部分 (38)。许可信息:版权所有 © 2026 作者,保留部分权利;独家许可方为美国科学促进会。对美国政府原始作品不主张权利。https: / www.science.org / about / science-licenses-journal-article-reuse

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补充材料

材料与方法;补充文本;图 S1 至 S12;表 S1 和 S2;参考文献 (49–63)

2025年12月18日提交;2026年8月18日接收

GLACIAL INCEPTION

晚全新世劳伦泰德冰盖的再次扩张

Nicolás E. Young $^{1*}$ , Gifford H. Miller $^{2,3}$ , Martha Raynolds $^{4}$ , Helga Bueltmann $^{5}$ , Scott J. Lehman $^{2}$ , Jonathan H. Raberg $^{2\dagger}$ , Kylie Seward $^{6}$ , Simon L. Pendleton $^{7}$ , John T. Andrews $^{2,3}$ , Patrick J. Webber $^{8}$ , Joerg M. Schaefer $^{1,6}$

在间冰期,劳伦泰德冰盖(LIS)作为更新世最大的冰盖,会退缩至加拿大北极地区,并在那里达到最小规模。LIS 在此最小值之后的再次扩张标志着下一次冰期的开始。在此,我们表明最近一次 的最后一个残余部分——巴恩斯冰帽(加拿大巴芬岛)在约 3.6 thousand 年前达到了间冰期的最小尺寸,随后在约 2000 年前再次扩张,标志着下一次冰期的开始。新的 在公元 1960 年左右达到最大尺寸,此后人为引起的夏季变暖导致质量平衡为负,冰缘退缩,并导致下一次冰期的终结。尽管夏季日照量持续下降,但下一次冰期的消亡说明了异常的温室气体强迫对气候的影响。

地球海洋底栖 $\delta^{18}\mathrm{O}$ 记录中高达 2 per mil ($\%$ o) 的周期性冰期-间冰期变化,在很大程度上是由第四纪(258 万 年前至今)陆地冰体积的变化驱动的,其中劳伦泰德冰盖()的影响最大 [相当于高达 $\sim 80$ 米的海平面冰体积;(1-3)]。在达到最大值后, 向东北方向退缩至加拿大东部北极地区,达到间冰期最小值,随后在下一个冰期循环开始时再次扩张 (4-7)。然而,关于冰盖最小值及随后冰盖重新生长(即冰期开始)的陆地证据,在很大程度上已被重复的冰期破坏,或位于现代冰盖之下,这使得人们难以深入了解冰盖究竟何时开始其向下一个

第四纪冰期最大值的千年尺度进军。模型表明,冰期可能起源于加拿大东部北极地区的巴芬岛 (4, 5, 7, 8),而如今,巴芬岛拥有巴恩斯冰帽(BIC;图 1),它是 在当前间冰期 [全新世;11.7 thousand 年前 (ka) 至今] 幸存下来的最后一个残余部分。BIC 位于巴芬岛中部高原(图 1),根据 $^{18}\mathrm{O}$ 值包含三代冰:表层的全新世间冰期冰,全新世冰之下的末次冰期冰,以及底部 $^{18}\mathrm{O}$ 值与全新世值相似的更古老的冰 (9)。因此,BIC 保存了 的最后残余以及过去 重新生长的证据,支持了长期以来关于巴芬岛中部高原是大陆规模

冰期主要起始点的假设 (6, 10-12)。

BIC 对气候尤为敏感,因为与加拿大北极地区其他坐落在高海拔基岩(海拔 >1500 米)上的现有冰帽不同,BIC 坐落在低海拔基岩(海拔约 500 米)上。直到最近,只有 自身的厚度(约 700 米)使其冰面能够与区域雪线相交,从而得以保存 (13)。例如,约 35% 的 表面积位于 1960–1980 CE 的平均雪线之上,而到 2000 年代初,仅有约 3% 仍位于 2000年代–2012 CE 的平均雪线之上,随后自 2010 CE 起 的积累区消失 (13)。在约 1960 CE 至 2022 CE 之间, 边缘后退了约 200 到 800 米,露出了一片独特的地形区域,其中包含在 LIS 经历间冰期最低配置后的初始扩张阶段而被杀死的植被,并因随后的当代后退而再次暴露(图 1)。我们利用两组新数据集——来自 前缘基岩和漂砾的原位 $^{10}$ Be 测量值,以及从后退的 边缘下方显露的被掩埋植被的放射性碳年龄——来约束 LIS 后退的最后阶段以及向 生长的反转。在此,我们表明,随着雪线在约 2 ka 前下降并与巴芬高原相交, 的质量平衡转为正值并开始重新扩张,标志着下一次冰期的自然开始。 的重新生长一直持续到约 1960 CE,当时当代夏季变暖导致的融化增加使质量平衡转为负值,从而驱动了冰帽的后退。

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冰缘年代学

BIC 前缘存在一条明显的修整线(trimline),标志着约 1960 CE 的历史最大 BIC 边缘 [见补充材料 (SM)]。1960 CE 的修整线以色调的剧烈变化为标志:修整线之外是长有地衣和植被的基岩地形,而修整线与现代冰缘之间的地形则几乎没有活体植被(图 1℃ 和 2 以及图 S1 至 S3)。这条清晰的色调修整线成为了一个关键的时间分界线,将全新世期间消融的景观与修整线紧邻内部的景观区分开来;后者在全新世期间虽曾消融,但随着 向 1960 CE 边缘重新推进而再次被冰川覆盖。此外,沉积冰碛的缺失表明 基底存在冷基(cold-based)至多热(polythermal)冰(13, 14)。冷基冰帽在北极地区广泛分布,由于冷基冰与其基底冻结,基底滑动可忽略不计,冰帽的演化主要受气候驱动的表面质量平衡变化控制(15–18)。在我们的野外研究区域中,基底滑动的缺失使得 在冰缘重新推进时充当了保存媒介而非侵蚀媒介(18–20)。

首先,我们限定了全新世期间 LIS 跨越现代 前缘退缩的时间。来自一个广泛冰碛系统的漂砾(位于距离现代 边缘约 7 至 9 km 处,n = 10;图 1℃,图 S1 和 S4,以及表 S1 和 S2)、紧邻 1960 CE 历史修整线外部的基岩表面(n = 13)以及修整线内部的基岩表面(n = 12)的新 ${}^{10}$ Be 表面暴露年龄在统计上均有重叠(图 1℃ 和 3 以及表 S1)。这三个地貌地层单位上重叠的 ${}^{10}$ Be 年龄表明,LIS 在距今(BP)(相当于 1950 CE;详见 SM;图 1℃ 和 3,图 S5,以及表 S1)$3.56 \pm 0.24$ ka 时,相对快速地跨越该景观并退缩至其 2022 CE 边缘之后。这一年龄与当地最小限制放射性碳年龄 $3275 \pm 420$ 和 $4110 \ 670$ 校准年 BP(图 1℃ 和表 S3),以及来自 北端的单个 ${}^{10}$ Be 年龄 $3.59 \ 0.22$ ka 和 $3.24 \ 0.31$ ka 是一致的 (21)。

接下来,我们限定了前缘在 $3.56 \ 0.24$ ka 消融后 重新推进的时间。由于在我们的研究区域中 与其基底冻结 (13, 14),我们假设对保存的原位枯死苔藓和木本植物进行 ${}^{14}C$ 定年可以限定 的扩张时期。数十年来,收集冷基冰帽相邻的原位枯死苔藓和植被已被用于重建巴芬岛的冰缘变化 (18–20, 22–24)。我们首先采用了成熟的策略,即在距离冰缘几米范围内采集样本,其中每个放射性碳年龄即为一个“死亡日期”,定义了冰川覆盖该特定地点的时刻 (18, 20, 25)。此外,最近的研究表明,从原位枯死苔藓和植被中获取的、向远离冰缘方向延伸的 ${}^{14}C$ 定年剖面可以限定冰川向

最终的历史最大范围 (23)。在 2022 CE 冰缘或其附近(距离见表 S4)采集的、此前被冰封的原位植被的 88 个新校准放射性碳年龄,均匀分布在 BIC 的南部和北部穹顶,并限制了更新后的 LIS 的广泛重新生长(图 1 B 和 C,以及图 2;图 S6;以及表 S4)。我们约 70% (n = 64) 的放射性碳测量值的中位年龄为 $1800 \pm 200$ CE,表明这些植物在小冰期接近顶峰时被杀死,当时很可能是公元 1780 年至 1880 年之间最寒冷的夏季 [(18, 26);图 2 和 3 以及表 S4;校准讨论见 SM]。不同穹顶之间的放射性碳年龄没有差异,这表明尽管在坡向、冰速、冰厚和质量平衡方面存在轻微差异 (13),但北部和南部穹顶之间冰缘变化的任何差异可能可以忽略不计。

图 1. LIS 的最后残余。(A) 末次冰盛期约 22 ka calibrated BP 时北美冰盖复合体的面积范围 (42)。LIS 与西侧规模小得多的科迪勒拉冰复合体 (CIC) 和东侧的格陵兰冰盖 (GrIS) 相连。(B) 巴芬岛上的 BIC (2015 CE Landsat 合成图像)。黄色和粉色圆圈标记了新的 $^{10}$ Be 和被封植被放射性碳定年的位置(表 S1 和 S4)。此前发表的 $^{10}$ Be(黄色菱形)和放射性碳年龄(粉色菱形)表明,古 LIS 在约 4 ka BP 时接近现代 BIC 的规模。位置 1:3240 ± 310 years (21);位置 2:3590 ± 220 years (21);位置 3:4290 ± 520 和 4180 ± 460 years (43);位置 4:4040+380 / –400 years (61)。来自高原冰帽被封植被的放射性碳年龄(绿色菱形;图 3)将区域雪线与地貌的初始交汇点限制在公元之前或公元早期 (18)。(C) 沿 BIC 东南部边缘的主要野外区域,标有约 1960 CE 历史最大范围的位置(蓝色虚线)、BIC 退缩期间填充山谷的前冰川湖古海岸线(白色虚线),以及此前研究中描述的显著跨谷冰碛 [(61);2024 年 9 月 CE Landsat 图像]。$^{10}$ Be 年龄(黄色圆圈;1σ 不确定度;离群值用斜体表示;图 S4 和 S5)表明,在约 3.6 ka 时,冰缘迅速穿过该山谷并进入 2022 CE 冰缘内部,这与此前发表的放射性碳限制一致 [粉色菱形;校准 years ;(61)]。图中显示了 BIC 边缘近期暴露的植物材料的新放射性碳定年的日历年校准中位年龄(粉色点;图 2 和表 S4);其他新的放射性碳年龄显示在图 2 中。

我们的一部分 ${}^{14}$ C 日期提供了劳伦泰德冰盖(LIS)重新扩张的更长记录。我们在历史最大修剪线(trimline)与 2022 CE 的巴恩斯冰帽(BIC)边缘的一段之间,沿着一条约 800-m 样线采集了一系列样本(n = 16),该段边缘比相邻的冰缘后退了约 4亿美元 [(27); 图 2]。BIC 边缘该段增强的局部后退是由一个现已排干的小型冰前湖驱动的,这使我们能够捕捉到更长的冰川前进记录(图 2)。正如在巴芬岛其他地方的冰川中所见,沿该样线的放射性碳年龄随着与冰缘距离的增加而逐渐变年轻,这与冰前沿的前进方向一致 (23)。在这些放射性碳年龄中最古老的样本位于冰缘附近,距离修剪线约 $ 700 至 750 m,表明新的 LIS 在约 $ 1000 CE 开始向历史最大范围前进(图 2)。来自同一位置(距离历史修剪线约 1.5亿美元)的 2 个 ${}^{14}$ C 日期,其校准中值年龄相差 300 年(1530 和 1830 CE;图 2, A 和 C,以及表 S4)。一种可能性是,根据我们样线中的 7 个 ${}^{14}$ C 日期(图 2)的约束,在约 $ 1450 至 1500 CE 期间发生了一次 BIC 扩张,随后是轻微的冰川后退,接着在 1800 年代初期再次发生冰川重新扩张。我们在同一位置采集的两个具有不一致 ${}^{14}$ C 日期的样本凸显了 BIC 边缘可能经历了多次后退与前进。然而,根据我们的 ${}^{14}$ C 杀灭日期(kill dates)的要求,这些微小波动发生在约 $ 1000 CE 之后整体净冰川扩张的时期。

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LIS 全新世最小值、重新扩张及当代退缩

我们的 ${}^{10}$ Be 和 ${}^{14}$ C 数据集将 LIS 的最小范围限制在 $\sim$ 2.6 千年 (kyr) 的窗口期内,处于 3.56 $\pm$ 0.24 ka BP 与 $\sim$ 1000 CE 之间。我们利用额外的数据集进一步细化 最小值的发生时间。首先,除非 在 3.56 $\pm$ 0.24 ka BP 的初始退缩期间恰好停止在 2022 CE 的边缘,否则冰盖的重新扩张必须发生在 $\$ 1000 CE 之前。然而,早于 $\$ 1000 CE 的植物至今仍被冰层覆盖,只有 BIC 的持续退缩才能使它们出露。其次,来自巴芬高原附近独立冰帽和冰川中出露的被冰封植被的大量 ${}^{14}$ C 日期 [高原冰帽 (PICs)] 为 LIS 在 1000 CE 之前可能发生的扩张时间提供了额外的见解(图 1B 和 3)。在该数据集包含的 $186^{14}\mathrm{C}$ 个日期中 (18),没有一个早于公元纪元 (Common Era)。缺乏单个 pre-Common Era ${}^{14}\mathrm{C}$ 日期表明,直到公元纪元 (Common Era) 之前不久或公元纪元早期(即 $\ 2$ ka BP),区域雪线才与巴芬岛中部高原 [海拔 $\ 800\{m}$;(18)](包括古 )相交,从而触发了广泛的冰帽和冰川的起始或扩张。综合这些额外的证据线索表明, LIS 在 $\ 3$ 和 $2\{kaBP}$ 之间达到了稳定状态——其真实的最小值配置尺寸小于今日——随后在 $\ 2\{kaBP}$ 开始重新扩张(图 3 和 4)。

PIC 数据集还包括在 $\ 250$ 至 450 CE、850 至 1000 CE 以及 1250 至 1450 CE 之间的明显 ${}^{14}$ C 杀灭日期集群,这些集群定义了区域雪线下降的额外脉冲 (18)。相反,PIC 数据集并不包含 BIC 数据集中存在的、以 1800 $\pm$ 200 CE 为中心的 ${}^{14}$ C 杀灭日期主峰(图 3)。PIC 和 BIC 数据集之间 ${}^{14}$ C 峰值的差异是由于冰帽退缩的幅度结合植被采样策略所致。PICs 和 BIC 都已从各自的历史最大范围退缩。然而,由于 PICs 相对较薄,冰量较少,因此对气候强迫的响应时间更快 (15, 18, 28),它们从历史最大范围退缩的程度超过了 BIC。被封植被主要在现代冰缘直接相邻处采集,因此在 PICs 的边缘附近预计会出现较旧的 ${}^{14}$ C 日期。尽管 $\ 1800$ CE 的峰值在 PIC 数据集中缺失,但根据海拔低于现有冰帽且缺乏密集植物覆盖的大片区域可以预测到该峰值,这些区域代表了在 $\ 1780$ 至 1880 CE 左右小冰期最寒冷夏季期间,冰帽扩张至其最低海拔的状态 (18, 26, 29)。尽管如此,$\ 250$ 至 450 CE、850 至 1000 CE 以及 1250 至 1450 CE 的雪线下降脉冲可能驱动了 LIS 的持续重新扩张,并且我们注意到 PIC 和 BIC 记录都共有 $\ 1450$ CE 的杀灭日期峰值,这表明该地区存在共同的气候强迫(图 3)。这些雪线下降的时间间隔与过去 2 kyr 的陆地代用指标和模拟温度冷却趋势相对应,这与现代观察结果一致,即夏季温度是巴芬岛冰川变化的主要驱动因素 [图 3; (17, 18, 30–32)]。

A

B

图 2. BIC 放射性碳数据。(A) 从冰缘到约 1960年代 CE 历史最大范围(蓝色虚线)的一条约 800 m 采样断面位置,见于 QuickBird-2 影像(©2011 Vantor)。数值为日历年 CE 的中值校正放射性碳年龄;样本 ID 在括号中(表 S4)。标有星号的样本不属于 (C) 中显示的主断面,但为了完整性在此列出。此处,由于一个现已排干的冰前湖 (L) 对退缩动力学的影响,BIC 冰缘比相邻冰缘后退了约 400 m,从而暴露了在整个 冰缘沿线发现的最古老的植物。更广泛的 LIS 冰缘在约 1960 CE 之前一直保持在其历史最大范围,但在我们的断面位置,由于冰前湖的影响,退缩在 1957 CE 之前就已经开始(见 SM)。(B) 所有被全新世晚期 再次前进所杀灭的植被的放射性碳定年概率密度函数。(C) (A) 中的 $^{14}\mathrm{C}$ 中值日期随 2024 CE 冰缘距离绘制的图表。星号标记来自航空或卫星影像的冰缘位置。误差棒代表校正中的 1σ 范围。

重新形成的 LIS 在 $1800 \pm 200$ CE 左右接近其历史最大修剪线,且航空照片显示 1957 CE 出现了孤立的冰缘退缩,而更广泛的 LIS 在约 1961 CE 之前仍保持在其历史最大范围(见 SM 及图 S2 和 S3)。这些约束条件与早期的冰川学研究一致,表明当时的冰帽处于近质量平衡状态 (13, 33, 34)。考虑到这些历史约束,我们将 1960 CE 标记为当代 广泛退缩的开始。区域记录显示,从 18 世纪末到 19 世纪初,夏季温度显著升高(图 3)。这种变暖驱动了低海拔薄 PIC 的早期退缩,而 在约 1960 CE 之前一直保持在其历史最大范围,这可能反映了北极中较大的冷基冰川和冰帽在气候扰动与冰缘响应之间固有的更长滞后时间 (15, 28)。冰帽特有的冰川学特性或降水模式的变化也可能驱动冰帽退缩,但自 20 世纪 60 年代初以来, LIS 的质量损失几乎可以完全由夏季温度升高来解释 (17)。此外,加拿大北极群岛及更广泛的北大西洋地区冰帽的广泛退缩表明,退缩是由夏季温度驱动的 (16, 17, 35)。夏季温度的升高与约 1750 CE 以来测得的混合均匀温室气体 (GHGs) 增加所相关的净有效辐射强迫增加相镜像 [CO₂、CH₄ 和 N₂O;(36–39)]。在约 1750 和 1850 CE 之间,混合均匀温室气体的浓度仅增加了约 12 ppm 二氧化碳当量 (CO₂e),这与最低海拔 PIC 的消失相吻合 (18)。到 1960 CE,当 退缩已经开始时,GHGs 又增加了约 50 ppm CO₂e,到 2024 CE 则又增加了 138 ppm CO₂e(图 3)。

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劳伦泰德冰盖(LIS)在全新世的演化与冰川起始

区域冰芯和陆地代理记录表明,北高纬度地区全新世最温暖的温度与约 11 至 10 ka BP 的北半球夏季日照峰值相吻合,随后随着辐射强迫在全新世期间下降,出现了净的多世纪尺度冷却 [图 4; (24, 30, 40, 41)]。然而,尽管存在这种长期冷却趋势,LIS 在全新世期间一直在退缩,直到约 2 ka BP

才开始重新生长 (42–44)。 BIC 在全新世期间的退缩表明, BIC 的几何形状与气候处于失衡状态;尽管有证据表明区域雪线自约 9 起就开始降低,并在约 5 后加速降低 [图 4; (22, 24)],但退缩中 的表面海拔仍不足以维持正的质量平衡。约 9 的初始雪线降低与约 2 的 BIC 重新扩张之间的滞后,部分程度上被冰期晚期和全新世早期的极端动力冰排放所放大 (45),导致冰盖表面低于仅由气候强迫所预期的水平。残余的等静压抬升在过去 3 kyr 中使 BIC 的海拔升高了约 20 m,这会略微改善其质量平衡,但可能不足以解释从退缩到前进的转变 (46, 47)。直到约 2 ,雪线才足够降低以与巴芬高原相交,从而允许 的重新扩张。

近期使用数据同化技术的温度重建表明,与全新世期间的冷却相反,表面温度在全新世期间几乎持平甚至有所上升 [图 4; (48–50)]。然而,这些重建要么没有包含陆地代理数据,要么表明数据同化方法低估了时间变率,且未能完全捕捉气候系统中的反馈机制 (50)。虽然这些温度趋势可能解释 在全新世期间直到约 2 的退缩,但它们可能无法驱动全新世晚期 的重新扩张。除了全新世晚期 的重新扩张外,整个北极和北半球的冰川在全新世期间经历了净前进 (51, 52)。这种始于全新世中期并在整个北半球的小冰期达到顶峰的长期冰川扩张典型模式,很难与那些显示全新世期间温度变率极小或呈变暖趋势的温度重建结果相调和。

A

C

E

图 3. 公元纪元(Common Era)。(A) 来自 PICs(图 1B)和 BIC 的校准放射性碳年龄的概率密度函数。PICs 中没有放射性碳年龄早于公元纪元($n = 186$),这表明直到公元纪元开始,区域雪线才开始与地形相交(这是驱动冰帽扩张所必需的)(18)。BIC 概率密度函数将冰川前进的主要脉冲限制在公元 $1800 \pm 200$ 年。 (B) 沿图 2℃ 所示的放射性碳年龄(点)和历史约束(星号)截面,冰缘前进的时间-距离关系(距离 2024 年冰缘的距离)。(C) 来自 Agassiz 冰芯的估计年平均温度异常及其 $2\sigma$ 不确定性(阴影区域)(30)。(D) 社区地球系统模型 (CESM) past2ka 模拟的公元纪元夏季温度(50 年平滑处理)(32)。模拟温度与 Agassiz 温度相似,并表明全新世最寒冷的夏季发生在公元 1780 年至 1880 年左右。(E) 测得的大气 $\mathrm{CO}_{2}$ 浓度 [符号和黑线;(62–64)] 和混合均匀的温室气体($\mathrm{CO}_{2}\{e}$ 红线)。WAIS,西南极冰盖。蓝色条形突出了跨越巴芬岛中北部的冰帽扩张脉冲,这些脉冲由 PIC 和 BIC 数据集约束,且与 Agassiz 和 CESM 温度记录中显示的寒冷区间相吻合。

根据米兰科维奇理论 (50, 53),由高纬度北半球夏季日照量下降及其相关的正气候反馈驱动的全新世晚期冷却,是冰川启动的必要前提。我们认为,全新世晚期重新出现的 LIS 约 2 kyr 的扩张代表了下一次冰期的开始。在人为夏季变暖的驱动下,BIC 在公元 $\sim 1960$ 年左右开始退缩,逆转了 2 kyr 的前进区间,标志着下一次冰期的终结。在 $\sim 8$ 至 2 ka BP 之间,$\{CO}_{2}\{e}$ 适度增加了 $\sim 20\text{-ppm}$,这与 LIS 退缩的最后区间相吻合,但这种幅度的 $\{CO}_{2}\{e}$ 增加不足以抵消日照驱动的区域冷却以及巴芬高原冰帽(包括 $\sim 2\text{ ka BP}$ 重新出现的 LIS)的扩张(图 3 和 4)。BIC 和 PIC 的冰帽扩张记录强调,地形起伏相对较低的巴芬岛中部高原对雪线的适度下降尤为敏感,这会导致永久雪盖在地形上迅速扩张。相关的地表反照率变化导致了强烈的正反馈,可能加速了过去 2 kyr 中北极海冰的扩张以及夏季温度的进一步下降 (18, 54)。巴芬岛高原,结合前一次冰期 LIS 的最后残余,为冰川启动提供了理想的环境,并支持了长期以来关于“瞬时冰川化”是冰期开始关键因素的假设 (4, 11, 12)。

图 4. 过去 11 kyr。(A) 北纬 65° 的 7 月太阳辐射量 (40)。(B) 根据 Agassiz 冰芯估算的年平均温度异常值,相对于 1750 CE,带有 2σ 不确定性(阴影部分)(30)。最高温度与最高太阳辐射量一致,而最低温度紧接在当代变暖之前。(C) 格陵兰岛中部冰芯重建的夏季(6 月至 8 月)温度,相对于 1860 至 2000 CE (41)。(D) 末次冰盛期再分析 (LGMR) (48) 和全新世 (49) 数据同化 (DA) 产品(相对于 1850–1900 CE),显示出长期全新世变暖或极小变化,与 (B) 和 (C) 中的区域记录形成对比。阴影区域表示 1σ 不确定性。(E) 过去 11 kyr 的大气 $\text{CO}_2$ 浓度和混合均匀的温室气体 (GHGs) ($\text{CO}_2, \{CH}_4, \{N}_2\{O}$),以 $\{CO}_2\{e}$ 表示,相对于约 8.1 ka BP 出现的 GHGs 最低浓度 (36–39)。(F) 北美冰盖复合体 (NAISC) 的面积范围,包含最小值和最大值估算(误差棒);该记录在约 10 ka BP 开始后几乎完全由 LIS 主导 (42)。(G) 概率密度函数 (PDFs)。来自被掩埋植被的放射性碳年龄将巴芬岛上全新世雪线下降的第一波时间限制在约 9.3 [蓝色; (24)]。$^{10}\{Be}$ 年龄将古 LIS 边缘退缩至 2022 CE 冰缘范围之内的时间限制在 3.56 ± 0.24 (本研究;红线为单个 $^{10}\{Be}$ 年龄,黑线为总分布;图 S5),而 LIS 的重新扩张可能始于约 2 [绿色 PDF;本研究及先前工作 (18)],且冰川在约 1000 CE 时接近其现代边缘(粉色 PDF;本研究)。

随着大气 $\{CO}_2$ 浓度的持续增加,回归冰期条件的可能性极低 (55, 56),但我们的新古 LIS 数据集为关于在工业化前气候状态下,冰期起始何时以及如何发生且持续的讨论提供了信息。之前的建模工作表明,下一次冰期起始将在数千年到数万年后才会发生。但重要的是,起始通常由北半球冰盖达到数米海平面当量来定义 (56–59)。然而,真正的冰期起始永远不会被这种古冰期的传统阈值标记所识别,因为该定义无法捕捉到间冰期后冰盖扩张的首次实例。先前的一项工作 (60) 探讨了轨道参数与底栖海洋 $\delta^{18}\{O}$ 值之间的经验关系,认为间冰期峰值条件发生在 1.8 至 -0.1 。间冰期峰值条件被定义为 $\delta^{18}\{O}$ 值从下降转为上升的预测变化,即冰盖增长的首次实例。这一预测转变的时间与我们的新直接地质观测结果显著相似,后者揭示了 LIS 在约 2 开始重新生长,标志着下一次冰期的起始(图 4)。

从 BIC 之下刚刚显露的地貌为我们提供了关于 LIS 最近一次脱冰历史、其间冰期最小配置以及冰川重新扩张时机的见解。LIS 在约 3.6 ka BP 时退缩至 2022 CE 的边缘线之内,但在全新世晚期并未完全消失。相反, BIC 在约 2 ka BP 开始重新生长,这标志着 启动阶段的首个直接证据。启动阶段发生在全新世期间温室气体(GHG)强迫适度增加的背景下。然而,这种温室气体强迫的增加未能扭转高北纬地区夏季冷却和区域雪线下降的千年趋势。过去约 2 kyr 的区域冷却可能得到了正反馈的助力,这些正反馈加速了巴芬岛上永久雪原和冰帽的扩张。在人为变暖的驱动下,当代的冰缘退缩已经逆转了约 2 kyr 的 BIC 前进,标志着人为终止了下一次冰期。

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致谢

我们感谢基基克塔尼因纽特人(Qikiqtaani Inuit)和努纳武特政府,感谢他们通过努纳武特研究学院(NRI)颁发的第 02-28-22R-M 号研究许可允许我们进入其领地,并感谢 NRI 在伊卡卢特提供的后勤协助。Batelle ARO 提供了额外的后勤支持。我们还感谢 R. Schwartz 和 J. Hanley 在 $^{10}$ Be 样品制备方面提供的帮助,以及劳伦斯利弗莫尔加速器质谱中心提供的最终 $^{10}$ Be 测量。我们还感谢 INSTAAR 实验室的 AMS 放射性碳制备与分析部门提供的样品制备,以及加州大学欧文分校 Keck 碳循环 AMS 实验室提供的放射性碳测量。资金支持:本工作由美国国家科学基金会(NSF)北极自然科学奖项(编号 1927148 和 2416598 (N.E.Y., J.M.S.) 以及 1927153 (G.H.M.))资助。NSF 极地计划

奖项(编号 1043681, 1559691, 和 2129685)为本工作提供了地理空间支持。作者贡献:概念化:N.E.Y., G.H.M., J.M.S.;方法论:N.E.Y., G.H.M., J.M.S., M.R., H.B., S.J.L., J.H.R., K.S.;调查:N.E.Y., G.H.M., M.R., H.B., S.J.L., J.H.R., K.S., S.L.P., J.T.A., P.J.W., J.M.S.;可视化:N.E.Y., G.H.M., S.L.P.;资金获取:N.E.Y., G.H.M., J.M.S.;项目管理:N.E.Y., G.H.M., J.M.S.;监督:N.E.Y., G.H.M., J.M.S.;论文初稿撰写:N.E.Y., G.H.M.;论文审阅与编辑:N.E.Y., G.H.M., M.R., S.J.L., J.H.R., S.L.P., J.T.A., P.J.W., J.M.S.。竞争利益:作者声明不存在竞争利益。数据、代码和材料可用性:所有数据均可在正文或补充材料中获得,也可在 NSF 北极数据存储库(65, 66)中找到。本研究未产生新材料。许可信息:版权所有 © 2026 作者,保留部分权利;独家许可方为美国科学促进会。对美国政府原始作品不主张权利。https: / www.science.org / about / science-licenses-journal-article-reuse

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补充材料

材料与方法;图 S1 至 S6;表 S1 至 S4;参考文献 (67–96)

2025 年 10 月 23 日提交;2026 年 8 月 29 日接收

10.1126 / science.aed3379

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当今受过 STEM 教育的专业人士在艰难的就业市场中面临着不确定性和陌生的挑战。美国联邦政策的变动、组织优先事项的快速转移,以及 AI 向几乎每个领域的扩张,足以让即使是最精明的科学家在探索职业成长方向时感到不知所措。

我们在此提供帮助。20 年多以来,《Science》一直开展年度“最佳雇主”调查,以探索顶尖制药和生物技术公司的脱颖而出之处。2026 年,有 5,100 多名读者参与了投票,强调了三大优先事项:科学与创新、以患者为中心以及员工支持。

然而,今年受访者对 AI 的态度出现了显著转变。评论反映出一种预期,即 将成为核心基础设施,而不仅仅是一个辅助工具。随着 在生命科学领域承担新角色,申请者在阐述自己的 NSF 能力如何能成为组织竞争优势时更加谨慎,无论是在研发、产品开发、质量控制还是其他部门。

Mix Talent 的几个生命科学招聘团队负责人 Tori Schaefer 表示,顶尖雇主确实在寻找具备 流利度( fluency)的科学家。这些人能够将 NSF 整合到日常工作中以解决复杂的研究问题——这远远超出了简单的聊天提示词。她说:“任何人都可以从 NSF 那里得到一个‘我们的目标应该是 X’的输出。但在科学上,在现实中,那真的是最佳选择吗?公司正在寻找能够弥合 流利度与科学知识之间差距的人才。”

这种大局观思维与实操专业能力的结合不仅限于 。Schaefer 还发现,雇主对那些是“战略执行者”或“战略实施者”的求职者感兴趣。“这种结合极其困难,因为你是在寻找一个已经进行了 10, 15 年战略思考的人,同时你还希望他们能将大约 50% 的时间花在处理具体、琐碎的实操工作中,”她说,“而这在传统角色中并不总是重叠的。”

虽然 已成为求职者更重要的考量因素,但调查还揭示了往年一直存在的一个常数:科学家希望在科学——以及人才——受到重视的地方工作。他们寻求能够获得尊重、被认可和被信任的工作场所,以及具有包容性、协作性和透明度的文化——部分受访者认为这些品质是不可妥协的。

“卓越的文化确实始于顶层。在这种文化中,人们渴望来上班,”Schaefer 说。然而,她发现一些公司在构建和维持职场文化方面投入的精力在减少,而求职者却在更仔细地审查潜在雇主。Schaefer 表示,即使在艰难的就业市场中,如果对雇主的文化有顾虑,他们也可能会放弃机会。“(候选人)可能会直接退出,因为他们听说那里并不是最好的地方。”

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我隐藏的无家可归经历

Sage Raymond

在机场候机期间检查电子邮件时,我兴奋地看到了一篇与我的博士导师共同提交的论文的期待已久的评审意见。这是一篇社论,我在其中提出了一个框架,旨在识别并缓解城市郊狼与无家可归者(露宿者)之间的冲突。基于我的学位论文研究,这篇文章比我之前写的任何文章都倾注了更多的心血。但评审意见却是压倒性的负面。我认可那些合理的科学批评,但我难以接受那些质疑我们的资质和专业知识的评论。其中一条尤其让我僵住了:“作者对无家可归的情况过于天真。”没有什么比这更远离事实的了。

在经历了动荡的家庭生活后,我在青少年晚期和 20 岁出头的时候一直处于无家可归的状态,有时住在街头,非法露营,或住在车里。在全职工作期间,我获得了一个 2 年制大学文凭,而当时我住在没有水和电的无暖气露营车里度过了加拿大的冬天。我在担任野外向导期间完成了本科阶段的学习,夏天露营,冬天则躲在不同的发霉的地下室卧室里。某种执拗、惯性以及对自然世界真正的好奇心支撑着我走下去。我热爱户外时光,热爱观察动物。我想要一份能够让我提出并回答自己的生态学问题的工作。

当读研成为一个选项时,这是一个显而易见的选择——毕竟,我还能因此获得报酬!我接受了一个研究城市化对郊狼行为影响的职位。该项目的野外工作促成了那篇社论的撰写。

写这篇文章并不容易。我的句子难以捕捉到我所观察到的问题的严重性。在野外工作中,我看到郊狼在露营地搜寻食物,食用会让它们生病的低质量食物。在其他地方,我收集到了感染有潜在致命绦虫的郊狼粪便,我知道露营地里的人可能会接触到这些,但他们很难获得医疗服务。这些观察与我希望自己没有的记忆交织在一起。在沉睡的城市中翻找垃圾桶的独特气味。与一位后来在街头惨死的朋友一起大笑并为她编辫子的场景。我将这些记忆推开,以便尽可能清晰且客观地写作。

无家可归夺走了我的很多东西,但它也给了我一些东西。我观察力敏锐。我善于利用资源。我非常擅长露营。我在恶劣天气中也能游刃有余。这些技能帮助我走过了许多有价值的道路——作为一名专业的野外向导,一名能够舒适地在荒野中独自露营的娱乐活动者,以及至关重要的,作为一名城市生态学家。在他人可能感到不安的城市空间进行野外工作,我感到很自在。正是这种能力让我注意到了我在论文中描述的事情,而那篇论文最终在另一本期刊上发表了。

我无法确切知道那位指责我们天真的评审员在想什么,但他们似乎从未想象过这样一篇文章的作者可能具有无家可归的第一手经验。这个假设震撼了我:它暗示像我这样经历的人不属于学术界。这已经不是我第一次有这种感觉了。我想起过往的研究生同学表达对一名睡在大学建筑入口处男子的恐惧,以及一次城市生态学安全简报会,其重点在于无家可归者的危险,而非如何与需要帮助的人沟通或支持他们。

许多为科学带来多样性的生活经历是不可见的,或者因为过于私人且禁忌而无法被谈论——例如虐待、贫困、强奸、成瘾、患有精神分裂症的家庭成员,以及一段无家可归的历史。我们对于研究人员是谁以及他们的过去是什么样的假设,创造了一种孤立的抹除景观——在这种环境下,某些历史被假定为不存在,使得拥有这些历史的人感到自己不属于这里。

多年来,我一直努力隐藏自己曾无家可归的历史。现在,我的心态更加中立——那是一个充满挑战且有时令人不快的章节,就像青春期,或者最近在学习贝叶斯统计一样。我致力于不让我的历史定义我。但我也不希望我的同事们认为,没有哪个科学家可能拥有像我这样的过去。□

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AI IN MEDICINE

Guiding a clinical workup to reach a diagnosis p. 423

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22 OCTOBER 2026

The FBI agent who sparked NIH's China investigations p. 378

Stopping an ice age in its tracks pp. 381 & 455

Science advocacy finds an ally in the arts p. 386

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CASE WESTERN RESERVE UNIVERSITY

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CONTENTS

22 OCTOBER 2026 | VOLUME 394 | ISSUE 6822

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381 & 455

The edge of the Barnes Ice Cap, Baffin Island, Canada, and its position of maximum extent around 1960

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EDITORIAL

363 The AI debate is missing half the system

—P. Michelucchi

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NEWS

364 Vaccine trial is a ray of hope in Congo's Ebola epidemic

Study will first test “mismatched” vaccine but Bundibugyo-specific shots may be added soon

—K. Kupferschmidt

366 Across fields, AI finds solutions hiding in plain sight "BootLoops" software enabled researchers to quickly find and attack problems in 22 disciplines —C. Zhao

367 How the domestication of a killer bacterium led to Botox

Scientists inadvertently turned C. botulinum into a tool for medicine and the beauty industry, study finds —J. Cohen

368 Microwave observatory peers into the infant universe In Chile, Simons Observatory begins hunt for galaxy clusters and signs of cosmic inflation —D. Clery

370 Deep-sea life is still reeling from the BP oil spill

A 13-year study shows

Gulf of Mexico ecosystems still haven't recovered

—E. Stokstad

371 Iron at Earth's heart may take a surprising form

X-ray experiments reveal cubic crystals that could complicate the picture of the inner core

—P. Voosen

372 Fired biologist wins \$6 million in defamation lawsuit

A jury ruled in favor of David Sabatini, dismissing accuser's claims of sexual harassment, retaliation —P. Jacobs

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FEATURES

374 Eyes on the ball

A “robo ump” that calls balls and strikes in Major League Baseball makes its World Series debut this week.

It has to be near-perfect

—J. Cohen

378 The instigator

A single FBI agent spurred NIH's campaign against foreign intervention on U.S. campuses. Now, he's studying the extent of the problem —J. Mervis

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COMMENTARY

PERSPECTIVES

381 Has the next ice age already come and gone?

The last remnant of a continental glacier shows that global warming may have forestalled the next glaciation —S. A. Marcott

RESEARCH ARTICLE p. 455

382 Putting glucose metabolism under electronic control

An electronic device controls the redox mechanisms that regulate glucose concentrations in mice —W. E. Bentley and G. F. Payne

RESEARCH SUMMARY p. 400

Two proteins that permeabilize mitochondria promote cell death through distinct mechanisms —C. Muñoz-Pinedo and S. J. Martin RESEARCH SUMMARY p. 401

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2026's Top Employers: From AI to I do

Science Careers' annual survey spotlights the biotech and pharma leaders earning the highest praise from Science readers.

Read the article on p. 461 and explore these highly-rated employers online at ScienceCareers.org/TopEmployers

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TOP EMPLOYERS

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385 The cognitive power of the avian brain

Carrion crows make decisions faster than monkeys and humans —M. Colombo and O. Poutrain-Sorel RESEARCH ARTICLE p. 445

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BOOKS ET AL.

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386 The microscope and the metaphor

Science shows us what to do to save the planet—poetry helps us understand why we should —P. Levin and D. Hassler PODCAST

387 The Monarch Bear

—L. Volski

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LETTERS

388 Indigenous higher education needs support

—B. E. Soares et al.

389 India needs a tree conservation plan —A. Dhyani

389 AI biosecurity must include agriculture

—J. Feldman et al.

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ANALYSIS

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POLICY ARTICLE

390 Fiscal discipline without physical resilience

Reforms could shift fiscal discipline and resilience investment into reinforcing forces rather than competing ones

—A. Mishra et al.

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RESEARCH

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HIGHLIGHTS

394 From Science and other journals

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RESEARCH SUMMARIES

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397 Cancer

Intron retention regulates STAT2 function and associates with immunotherapy response in lung cancer —R. P. Englander et al.

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398 Solar cells

Decoupled self-assembled monolayer and perovskite deposition for efficient flexible solar modules —Y. Wu et al.

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399 Artificial intelligence

The Virtual Biotech: A multi-agent AI framework for therapeutic discovery and development —H. G. Zhang et al.

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400 Metabolism

Wireless electrocatalytic closed-loop system for drug-free management of diabesity —D. Maity et al.

PERSPECTIVE p. 382

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401 Cell biology

BAK and BAX form a multiprotein complex to drive mtDNA efflux and caspase-independent cell death —S. Yang et al.

PERSPECTIVE p. 383

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RESEARCH ARTICLES

402 Molecular biology

Noncoding transcription controls the developmental dynamics of long-range gene regulation

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408 Conservation biology

Safeguarding global terrestrial vertebrate species from future sea level rise —Z.-W. Jiang et al.

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413 Natural products

Natural product biosynthesis by guanidine prenyltransferases in plants and bacteria

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419 Solid-state physics

Thermodynamic origin of the phonon Hall effect in a honeycomb antiferromagnet —Q. Meng et al.

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423 Machine learning

Sequential diagnosis with language models —H. Nori et al.

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429 Physics

Electronic bound states in the continuum in a two-dimensional metal —M. Thinel et al.

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434 Membranes

Dynamic functionality-enabled fast and selective transport in nanochannels —H. Zhang et al.

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440 2D materials

Visualizing symmetry-broken Chern insulators and their quantum melting —M. He et al.

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445 Comparative cognition

Ultrarapid decision-making in an avian brain

—P. Schmidbauer and A. Nieder PERSPECTIVE p. 385; PODCAST

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385 & 445

Crows perform random dot movement discrimination tasks with ultrarapid decision times.

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CONTENTS

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ON THE COVER

This image depicts a patient and a physician working together with artificial intelligence (AI) to reach a diagnosis. Researchers developed an AI-based approach to help physicians with real-life clinical workups, starting with the patient's chief complaint, systematically asking questions and deciding what laboratory and imaging tests to order, and then continuing the evaluation on the basis of the answers received. See page 423. Illustration: Jason Solo

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450 2D materials

Imaging electron-hole asymmetry in the quantum melting of generalized Wigner crystals —E. Berger et al.

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455 Glacial inception

Late Holocene reexpansion of the Laurentide Ice Sheet —N. E. Young et al.

PERSPECTIVE p. 381

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462 My hidden homeless past

—S. Raymond

362 Science Staff

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Sylvie Roke, École Polytechnique

Fédérale de Lausanne

Sarah Ross, U. of Pittsburgh

John Rubinstein, SickKids

Yvette Running Horse Collin,

Toulouse U.

Mike Ryan, UT Austin

Alberto Salleo, Stanford U.

Lawrence Berkeley Nat. Lab

Nitin Samarth, Penn State U.

Bhaven Sampat, Johns Hopkins U.

Erica Ollmann Saphire,

La Jolla Inst.

Vladimir Shalaev, Purdue U. Jie Shan, Cornell U.

Jay Shendure, U. of Wash.

Steve Sherwood,

U. of New South Wales

Robert Siliciano, JHU School of Med.

Emma Slack,

ETH Zürich & U. of Oxford

Richard Smith, UNC (S)

Carnegie Institution for Sci.

V. S. Subrahmanian,

Northwestern U.

Sandip Sukhtankar, U. of Virginia

Christopher Summerfield,

U. of Oxford

Tavneet Suri, MIT

Naomi Tague, UC Santa Barbara

A. Alec Talin, Sandia Natl. Labs

Patrick Tan, Duke-NUS Med. School

Fuchou Tang, BIOPIC Beijing

Dörthe Tetzlaff, Leibniz Institute of Freshwater Ecology and Inland Fisheries Amanda Thomas, UC Davis

Bozhi Tian, U. of Chicago

Rocio Titiunik, Princeton U.

Shubha Tole,

Tata Inst. of Fundamental Res.

Kimani Toussaint, Brown U.

Li-Huei Tsai, MIT

Jason Tylianakis, U. of Canterbury

Jo Van Ginderachter,

VIB, U. of Ghent

Matthew Vander Heiden, MIT

Ivo Vankelecom, KU Leuven

Henrique Veiga-Fernandes,

Champalimaud Fdn.

Elizabeth Villa, UC San Diego

Bert Vogelstein, Johns Hopkins U.

David Wallach, Weizmann Inst.

Jane-Ling Wang, UC Davis (\$) Jessica Ware,

Amer. Mus. of Natural Hist.

David Waxman, Fudan U.

Alex Webb, U. of Cambridge

Marjorie Weber, U. of Michigan

Chris Wikle, U. of Missouri (\$)

Ian A. Wilson, Scripps Res. (\$)

Sylvia Wirth, ISC Marc Jeannerod

Catherine Wolfram, MIT

Amir Yacoby, Harvard U.

Benjamin Youngblood, St. Jude

Kenneth Zaret, UPenn School of Med.

Magdalena Zernicka-Goetz, Caltech

Bing Zhai, Shenzhen Insts. of Advanced Technology

Lidong Zhao, Beihang U.

Bing Zhu, Inst. of Biophysics, CAS

Xiaowei Zhuang, Harvard U.

Maria Zuber, MIT

The AI debate is missing half the system

Pietro Michelucci

Last month, leading executives of artificial intelligence (AI) companies warned the United Nations Security Council about the risks of losing human control over this rapidly advancing technology. Their recommendations focused heavily on safeguards, evaluation, and governance of AI models and systems, largely overlooking the risks that arise from the interactions of AI with people and institutions. AI safety needs to be addressed at the level of the human-AI system, not the AI model alone.

The stakes are high. People are already embedded in systems that derive capabilities and behaviors from human interactions with AI. AI is influencing which medical treatments people pursue, where companies invest, how cities optimize civil infrastructure, and even how

optimize civil infrastructure, and even how countries approach national security. Humans are no longer thinking alone but in a continuous feedback loop with AI—they are not external to the system. As society becomes increasingly dependent upon AI systems, a kill switch cannot by itself serve as a viable or sustainable safety feature.

The real issue is the safety of the entire human-AI system. No single component, human or machine, can be made perfectly trustworthy. So the system itself must re-

main safe even when its components become unreliable. But how can self-correction and resilience be built into this complex system?

Although this might seem insurmountable, methods for building reliable systems from unreliable components have been under development in the field of human computation, which studies computing systems that rely on humans in a feedback loop. For example, one approach has been to implement a “trust score” modeled on the basic social principle that trust builds slowly but can be broken quickly. To accomplish this, a system randomly mixes test questions, for which the system already knows the correct answer, into work where the answers are unknown. As an individual gets a test question wrong or tries to cheat, their trust score drops. If the score dips below a certain threshold, the person can continue working, but their answers no longer affect the system output. The individual can slowly gain back trust by delivering correct answers again. Through dynamic monitoring, a participant’s contribution can remain valuable while their influence changes according to live fluctuations in their performance. The point is that trust, influence, and authority need not be fixed. They can be continuously adjusted as new evidence emerges.

Consider the recent Hugging Face incident, in which AI agents that were running cybersecurity evaluations bypassed restrictions of the testing environment, sought information about how they were being evaluated, and coordinated a cyberattack against an external open-source platform. A dynamic evaluation approach could monitor whether an AI system begins taking harmful actions while pursuing an assigned task, and rapidly reduce the system's access to tools or data or the ability to act autonomously. These capabilities could be restored only after sustained evidence of reliable behavior.

The same principle could be applied across the broader human-AI system. Reliable evidence for how well a human-AI system is performing a task could be used to adjust

various parameters, such as access to data, as conditions change. This shifts the discourse from whether an AI is safe enough to deploy to how trust, influence, and autonomy should be distributed across the human-AI system.

Many AI and social scientists are working to develop reliable and resilient human-AI systems. For example, the Assess Risks and Impacts of AI program at the US National Institute of Standards and Technology broadens AI evaluation

beyond the model to include interactions with human users in realistic settings. However, generating evidence for system performance can itself be an obstacle to evaluating whether it is safe. Performance cannot always be tested against known outcomes or independently audited decisions. Monitoring performance can itself create risks involving privacy, consent, and authority among the human participants. So any sustainable approach must address not only how trust and influence are adjusted, but what evidence justifies those changes, who can observe them, and who has the authority to act.

Instead of treating an AI model as a device that passes an initial test and is never checked again, regulators need to consider how AI performs in the real world alongside human users and how a system's permissions are continually monitored and adjusted on the basis of demonstrated reliability over time. This means developing safety protocols that shift from static guardrails to dynamic evaluation, and from AI models alone to the full human-AI system. □

Pietro Michelucci is executive director of the Human Computation Institute, Ithaca, NY, USA. pem@hcinst.org

INFECTIOUS DISEASES

Vaccine trial is a ray of hope in Congo's Ebola epidemic

Study will first test “mismatched” vaccine but Bundibugyo-specific shots may be added soon KAI KUPFERSCHMIDT

First responders in North Kivu province in the Democratic Republic of the Congo line up to receive an Ebola vaccine named Ervebo on a “compassionate” basis.

There are glimmers of hope amid the relentless bad news about the explosive epidemic of the Ebola Bundibugyo virus in the Democratic Republic of the Congo (DRC). After months of debates and preparations, a vaccine trial, named Tumaini—Swahili for “hope”—is expected to clear the final regulatory and ethical hurdles any time, and the first doses could be administered this week. The trial will first test Ervebo, a “mismatched” vaccine developed for another Ebolavirus species named Zaire. But two other vaccines, designed specifically to protect against Bundibugyo, may be added to the study in November.

Meanwhile, after more than 9500 reported cases and more than 4600 deaths, the epidemic appears to be slowing in Ituri, its epicenter and the hardest hit province. Both the number of newly reported cases and the percentage of tests that come back positive are going down, says Jean-Jacques Muyembe-Tamfun, who heads the DRC's National Institute of Biomedical Research: "It is not optimal, but it has improved."

And finally, a trial testing two potential Ebola therapeutics—an antibody cocktail named MBP134 and the antiviral remdesivir—has already enrolled more than 600 patients. There may soon be enough data to

see an effect, says Placide Mbala of the Africa Centres for Disease Control and Prevention, principal investigator on the trial. An effective treatment would be a big boost to the response, says epidemiologist Chikwe Ihekweazu, who heads the Health Emergencies Programme at the World Health Organization (WHO). “Every extra tool you have in the arsenal helps.”

Still, the challenges are enormous. The disease could still spread to more places. Earlier this month, Kenya announced its first Bundibugyo case, a 40-year-old Kenyan man who died in Nairobi after traveling from the DRC by way of Uganda. Four

family members and four health care workers have also tested positive and are in isolation. On 20 October, Nigeria reported a case as well, a woman who had traveled to Uganda, which had 20 cases earlier this year but declared its outbreak over in July.

In the DRC, two-thirds of the people who die of Ebola still do so in their communities instead of dedicated treatment centers, creating the risk of further spread. Contact tracing is still not working well; about 40% of newly identified cases aren't on the contact list of any known Ebola case. That's down from about 70% early in the outbreak, says Marie Roseline Belizaire, incident manager for the outbreak at WHO's Regional Office for Africa. "It's progress, but it's not enough."

And although cases in Ituri have gone down, they have trended upward in North Kivu, the second most affected province. WHO and other groups have scrambled to move more resources there. “I think it will be very important to see where the trajectory goes,” Ihekweazu says. With dozens of new cases reported each day, there will be no quick end to the outbreak, he warns. “The one game changer would be if we have a highly efficacious vaccine that we can deploy at scale.”

That's why the stakes in the vaccine trial are so high. Ervebo, developed more than 25 years ago, incorporates a surface protein of Ebola Zaire into a livestock virus that's innocuous to humans. It was first used during the devastating West African Ebola Zaire epidemic of 2013–16, where it showed complete protection in a trial in 2015. Animal studies suggest it may also work against Bundibugyo. The Tumaini trial will test that promise by giving the candidate vaccine to direct contacts of known Ebola cases, a “ring vaccination” design similar to the one used in the 2015 trial.

In that study, conducted in Guinea, entire rings of contacts were randomized to receive the Ebola vaccine either immediately or 3 weeks later. In the Tumaini trial, each person within a ring will be randomized. For now, half will receive the Ervebo vaccine on Day 1 and a typhoid vaccine 4 weeks later; for the other half, the sequence is reversed.

Randomizing individual people rather than entire rings should lead to efficacy data faster, says Ira

Longini, a biostatistician at the University of Florida who was involved in designing both trials. But the typhoid vaccine given to the control group could make it a little harder to detect any benefit from the Ebola vaccine because the typhoid shot might give the immune system a boost. That could protect some people in the control group from infection with Ebola and make any benefit of the vaccine seem a little smaller than it is.

The team started to explain the setup of the trial to people in the affected area 2 weeks ago, says Jean-Pierre Van geertruyden, an epidemiologist at the University of Antwerp and one of the trial's principal investigators. Complicating their outreach is the fact that Ervebo is already given on a “compassionate” basis to first responders in some parts of the country. It’s also used in health care workers in Ituri, in a separate trial called BRAVO that has no control group. Van geertruyden acknowledges that people might question why Ervebo is good enough to give to health care workers but needs testing on the rest of the population: “People might be a bit confused.”

Once Tumaini is up and running, the vaccine candidates specifically targeting the Ebola Bundibugyo virus will be added as they become available. Furthest along is a vaccine developed by researchers at the University of Oxford that contains a surface protein of Bundibugyo stitched into a chimpanzee adenovirus.

Data analyzed so far from ongoing phase 1 trials in the United Kingdom and Uganda suggest the vaccine can proceed to the next stage, says Oxford vaccinologist Teresa Lambe, who hopes it will “enter the trial as soon as possible.” A Moderna-made messenger RNA vaccine is closely behind. Van geertruyden believes both could be added to Tumaini in early November. It may take until February or March 2027 for efficacy data for the new vaccines to emerge, he says.

By then, the epicenter of the epidemic may have moved, and the trial would have to move with it. Organizers would have to shift their team, ensure they have housing and food, and keep the laboratory and refrigerators running in areas with poor infrastructure: “We have to follow the epidemic and that’s not easy,” Van geertruyden says. Perhaps by that point, the outbreak may be not just moving, but waning. □

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IN OTHER NEWS

NO MORE LEAP SECOND The International Bureau of Weights and Measures announced last week it was bidding adieu to the leap second—an awkward cousin of the leap year, the extra day added to the calendar every 4 years to account for the fact that Earth orbits the Sun once every 365.24 days. The leap second compensated for unpredictable variations in Earth’s rotation and was added to Coordinated Universal Time (UTC)—which regulates clocks worldwide relative to the fixed stars—only when atomic clocks and observations indicated UTC was off by 0.9 seconds. Since 1972, a leap second had been added 27 times, but its idiosyncratic nature caused problems with computer networks and websites. The bureau will now add a leap hour whenever UTC wanders by that much, which means the next adjustment won’t be for thousands of years. —Adrian Cho

DOJ TO FUND GENDER RESEARCH The U.S. Department of Justice is moving to fund research on gender dysphoria, the feeling of distress when a person's gender identity doesn't align with their sex assigned at birth. The 9 October funding notice says it will grant up to \$1 million for studies of "gender dysphoria, its treatment, and the perpetration of violence," including research on the prevalence of violent crime among people with gender dysphoria. The initiative has raised concern among scientists and activists who worry it is driven by political bias that could cause harm to transgender people, who studies show are at increased risk of being victims rather than perpetrators of violent crime. —Julia Vaz

WEST NILE SURGES IN EUROPE This summer, West Nile virus (WNV) spread farther into Europe and sickened more people than ever before. In a report published last week, the European Centre for Disease Prevention and Control reported 1715 locally acquired human infections including 130 deaths since May. The hardest hit countries were Italy and Greece. But with Belgium reporting its first ever cases of the mosquito-borne illness, the agency said “the virus is now circulating further north, a trend that is expected to continue in the coming years.” Most WNV infections cause no symptoms, but about one in five people get sick and about one in 100 develop severe neurological disease, which can be fatal.

—Kai Kupferschmidt

ARTIFICIAL INTELLIGENCE

Across fields, AI finds solutions hiding in plain sight

"BootLoops" software enabled researchers to quickly find and attack problems in 22 disciplines CELINA ZHAO

A BootLoops-powered analysis of the Voynich manuscript, a 15th century book full of undecipherable script, concluded it does not hold a hidden message.

Borrowing an idea from one research discipline to solve a thorny problem in another is an old scientific trick. Charles Darwin's theory of natural selection, for example, inspired algorithms in computer science that "evolve" solutions to complex problems.

But such clever leaps are fleetingly rare. Usually, “A physics researcher wouldn’t spend 6 months reading linguistics research in order to figure out how to repurpose linguistics methods,” says Georgia Channing, artificial intelligence for science lead at Hugging Face, an AI tools platform.

For AI, however, hopping between fields can be a breeze. Researchers highlighted that ability earlier this month with the release of 36 preprints produced with a suite of AI tools called BootLoops. The so-called harness can be used with any large language model (LLM), such as Anthropic's Claude or OpenAI's ChatGPT. And in just 3 months, researchers used Claude outfitted with BootLoops to cross-pollinate at a massive scale, spotting—and solving—problems in seemingly unrelated fields that share the same mathematical structures. The resulting papers range widely, from figuring out the age of sunspots to attempting to decipher a medieval manuscript.

In essence, BootLoops “kept noticing the same pattern: many fields have problems that a technique from mathematics, physics, or computer science would solve outright if anyone knew it existed," Matthew Schwartz, a physicist at Harvard University and visiting researcher at Anthropic who developed the tools, wrote in a 1 October blog post unveiling the preprints.

The project also helps bring AI to scientific disciplines that have been slower to adopt it, Schwartz and other researchers say. “It’s phenomenal that the technology is being saturated through more fields,” Channing says.

Researchers caution that BootLoops still needs extensive human involvement to produce useful results. They also add that it suffers from limitations common in AI-powered science.

Schwartz began to explore AI's research capabilities in December 2025 when he took on Claude Opus 4.5 as his virtual “graduate student.” With heavy hand holding, it managed to spin up a reasonable physics research paper in just 2 weeks. Intrigued, Schwartz started to give the LLM bigger challenges, eventually as ambitious as reinventing quantum mechanics. But “It just wasn’t ready,” he says.

Then, he thought: Instead of forcing AI to perform like a human researcher, why not play to its strengths?

One obvious strength was coding. Schwartz tasked Claude Fable 5 with writing code to solve a type of integral used in theoretical analyses of high energy particle collisions. It combed physics and math papers for other examples of the integrals, then built software to solve 30 of them, including 15 that had never before been solved. The tool became BootLoops.

He then unleashed it on the broader scientific literature, where it soon identified many similar unsolved problems in other disciplines. From there, Schwartz says, “The project exploded,” and he began to recruit experts from other fields to collaborate.

One of the resulting papers, co-authored by evolutionary biologist Scott Edwards of Harvard, involved building evolutionary trees from DNA data. BootLoops calculated that two possible trees of the evolutionary relationships of humans, chimpanzees, gorillas, and orangutans were equally likely—something past estimation strategies could not establish. “This is my first experience with Claude-based science, and I can definitely see the potential,” Edwards says.

BootLoops was also able to find an optimal way to rank health insurance plans offered under the U.S. government's Medicare program. The current classification system, based on metrics such as patient experience, uses an approximate clustering algorithm to set the cutoff between five possible ratings. Those cutoffs then determine the bonus the government pays insurance companies. BootLoops, however, was able to calculate precise optimal bins. The accompanying preprint suggests implementing those suggestions could save the taxpayers roughly \$1 billion from 2025 to '27.

Soon, collaborations expanded beyond math problems to other work suited to LLMs. In yet another project, Schwartz and a trio of linguists used AI agents to scour the academic literature and amass the largest ever standardized catalog of languages' stress and tone patterns, using BootLoops to check the agents hadn't skipped any additional stress systems a language could presumably use. The resulting database, called ACCSTACK, is more than eight times larger than the largest previous data set of its kind, documenting the sound systems of more than 6000 languages. ACCSTACK is "of a scale that's really far, far beyond what we've been able to do as just humans doing it," says preprint co-author Joe Pater of the University of Massachusetts Amherst.

But as BootLoops wandered farther afield, Schwartz found that although the LLM could tell him what it could calculate, it couldn't identify what scientists would really care about. Put simply, it lacked research taste. For example, Claude saw a chance to test ecology's neutral biodiversity theory—which holds that many genetic differences between individuals and populations are due to random variations. The AI generated a counterexample, based on data from a research island in Panama, that showed tree diversity was changing faster than expected by chance alone.

When Schwartz asked ecologist James O'Dwyer of the University of Illinois Urbana-Champaign to examine the results, O'Dwyer found them “interesting” but not field changing. “I don’t think it’s going to replace ecologists of any kind just yet,” he says. “But I do know that everything moved much faster with this collaboration.”

Not all researchers embraced the tools. One preprint analyzes the Voynich manuscript, a 15th century book full of undecipherable script that has perplexed scholars for centuries. The paper claimed the manuscript may not encode a hidden linguistic message after all. But in an online forum dedicated to the manuscript, some contributors complained that the paper was so dense as to be AI “slop.”

Schwartz acknowledges the need for caution: On colleagues' advice, he withheld some results that were insufficiently validated. But he believes researchers in many areas will benefit from working with discipline-spanning AI tools. "Once everyone catches up," he says, "this human-AI collaborative era will be very exciting."

MICROBIOLOGY

How the domestication of a killer bacterium led to Botox

Scientists inadvertently turned C. botulinum into a tool for medicine and the beauty industry, study finds JON COHEN

A lavish 1919 dinner party that ended up killing five people. An attempt to save the canning industry in the 1920s. A World War II biological weapons program and a CIA plot against Fidel Castro. A cosmetic product, best known as Botox, that erases facial wrinkles and exploded into a multibillion-dollar business.

A new analysis of more than 1000 bacterial genomes connects these disparate episodes in U.S. history in a piece of microbiological detective work. The study, published on 15 October in the Proceedings of the National Academy of Sciences (PNAS), shows how scientists unwittingly triggered the evolution of a dangerous bacterium into one with major medical and commercial advantages.

That microbe is Clostridium botulinum, whose neurotoxin disrupts nerve communication, paralyzing muscles and causing victims to suffocate. The toxin, called BoNT in shorthand, is one of the most lethal natural substances known. Under oxygen-free conditions—in preserved food, for example—C. botulinum spores can “wake up,” developing into toxin-producing bacteria.

That's what happened with spores trapped in jarred Californian olives during the “Great Olive Poisoning of 1919,” which included a widely publicized dinner hosted by Detroit industrialist Murray Sales and his wife that killed two of the couple's children, a guest, and two maids. Nine other people in two other states died.

The tragedies posed a major threat to the burgeoning canned food industry and triggered a new wave of microbiological research. Among the researchers who joined the fight was Ivan Clifford Hall, a bacteriologist at the University of California who amassed a collection of C. botulinum isolates.

One, named Hall A, became a laboratory workhorse, propagated over and over. In the process, it became “domesticated”—reshaped by human-driven evolution, like countless other plants, animals, and microbes. Hall A

Ivan Clifford Hall collected many Clostridium botulinum strains, including a lab workhorse now known as Hall A.

lost its ability to form spores, which made it easier for scientists to purify BoNT, and churned out exceptionally high levels of the toxin. Those characteristics made Hall's strain a favorite of U.S. military researchers, who in 1942 started to use it to create biological weapons and a botulinum vaccine.

The military shared Hall A with others. In the early 1960s, CIA launched a plot—ultimately scuttled—to assassinate Cuban leader Fidel Castro by contaminating a box of his cigars with BoNT. Around the same time, a military researcher took a Hall A subculture with him when he moved to the University of Wisconsin and shared it with a Californian ophthalmologist, who began to conduct monkey experiments to see whether BoNT could relax eye muscles, in hopes of finding

treatments for misaligned eyes, a condition called strabismus. “This really is a swords into plowshares type of story,” says microbiologist Paul Keim of Northern Arizona University (NAU), the new study’s first author.

In the 1980s, U.K. microbiologist Andy Pickett and others, working with drug companies, found that tiny doses of BoNT—mere billionths of a gram—produced by descendants of Hall A could treat strabismus in humans. In 1989, the U.S. Food and Drug Administration approved the purified toxin as a treatment for that disease and eyelid spasms. The drug, now made by a few dozen companies, became widely known by the trade name Botox after it was found to temporarily paralyze facial muscles that create lines around the eyes, forehead, and nose.

Pickett has been hired as an expert witness in several legal battles around BoNT ownership and manufacturing secrets, as has Keim. To help unravel the differences between the strains in dispute, Keim suggested lawyers also recruit Richard Lenski, an evolutionary biologist at Michigan State University who in 1988 launched a now-famous experiment to follow 12 identical populations of Escherichia coli and document how they evolved over decades. (The study is still running, nearly 85,000 generations later.)

As part of their work on the case, the researchers constructed family trees of C. botulinum based on publicly available genome sequences and ones they sequenced themselves. They found that the Army Hall A strain and its commercial descendants were on an “unexpectedly long branch” of the family tree, says Lenski, a co-author on the PNAS paper, suggesting strains in that lineage mutated far more rapidly than their cousins.

“That brought to mind what we have seen in our experiments” with E. coli, Lenski explains. In those studies, some lab-propagated strains that started to mutate faster than normal had a defect in a gene involved with DNA repair. At Lenski’s suggestion, Keim and NAU microbial genomicist Jason Sahl looked for similar defects in the Hall A relatives. Sure enough, they found one, a mutation in a gene named mutS.

Keim says the mutation likely arose while Hall was working with the strain. In the wild, it might soon have disappeared, he says, but it thrived in the lab, in part because scientists favored C. botulinum cultures that displayed the mutation's effects. The mutS variant prevents C. botulinum from wasting energy making spores, allowing them to grow well and produce unusually large amounts of the toxin. The bacteria's metabolic pathways are "fine-tuned now for living in the laboratory as opposed to living out in nature," Keim says.

“This work really fills in a fantastic hole of knowledge,” says Pickett, who’s now retired and was not directly involved in the study. He is delighted that the study also spotlights Hall, whom he sees as an unsung hero. Although some of Hall’s “incredible” collection of anaerobic organisms made it to other labs, much of it no longer exists. “No one wanted it,” Pickett says. Unraveling the genetics of the Hall A strain, he says, is “a good tribute to someone who is basically an enigma.”

ASTRONOMY

Microwave observatory peers into the infant universe

In Chile, Simons Observatory begins hunt for galaxy clusters and signs of cosmic inflation DANIEL CLERY

From a perch high in Chile's Atacama Desert, a cluster of telescopes is taking aim at the oldest light in the

universe, the cosmic microwave background (CMB), emitted just 380,000 years after the Big Bang. With greater sensitivity and sharper resolution than earlier CMB surveys, the Simons Observatory will deepen cosmologists' understanding of the universe's makeup and look for signs of "cosmic inflation," a hypothesized burst of exponential expansion in the universe's first moments. "To a first approximation, it's going to do what those [earlier surveys] did, but better," says theoretical physicist Marc Kamionkowski of Johns Hopkins University.

But the observatory is much more than a simple CMB experiment, says co-director Mark Devlin of the University of Pennsylvania. By using the CMB as a backlight, the observatory will also study how the universe has evolved since the light was created. It will discover tens of thousands of galaxy clusters and observe the distribution of matter across cosmic history. A community of thousands of scientists is waiting for the data, Devlin says. “You have to have a broad appeal.”

Moisture in Earth's atmosphere blocks microwaves, so observers have mapped the CMB with satellites and balloons, or from the ground at high, dry spots. Prime locations are the South Pole and

The Simons Observatory's Large Aperture Telescope will map the oldest light in the universe, the cosmic microwave background.

the Atacama, where the \$120 million project, funded mostly by the Simons Foundation, has built three small-aperture telescopes, each 0.5 meters across, and a 6-meter Large Aperture Telescope that is set to begin its survey of the sky this month.

Simons is starting up as CMB researchers adjust to the loss of a much larger planned experiment. Last year, the U.S. National Science Foundation and Department of Energy ended support for a “CMB-S4” experiment, a next-generation project in Chile and at the South Pole that was designed to seek signals of cosmic inflation. “We’re not as sensitive as the original CMB-S4 was planned to be, but we’re covering all of the same science … and we’re doing it now,” says Simons Observatory spokesperson Jo Dunkley of Princeton University.

The CMB, the glow of the superhot infant universe, was stretched by cosmic expansion and now looks like a faint microwave haze from all directions. It is mottled with tiny temperature fluctuations that correspond to concentrations of matter, including unseen dark matter, in the infant universe—seeds that would grow

under gravity into the cosmic web of galaxies, filaments, and voids. By precisely measuring those fluctuations, cosmologists have reconstructed the basic recipe of the universe: roughly 5% ordinary matter, 26% dark matter, and 69% dark energy, a mysterious force that is accelerating the expansion of the universe.

Simons will not only refine those numbers, but also use its map of CMB fluctuations to address other questions, including the mass of the neutrino, a ghostly particle that streams through space at high speeds. Neutrinos don't clump like slow-moving matter and dark matter, so they suppress the growth of the cosmic web. By comparing the early-universe pattern encoded in the CMB with the later distribution of matter, Simons researchers can constrain the mass of these elusive particles. “We should be able to actually have a positive measurement of this mass,” says cosmologist Seshadri Nadathur of the University of Portsmouth.

The observatory will also probe an event thought to have preceded even the CMB: a brief spurt of exponential growth during a fraction of the universe's first second. In that instant of “cosmic inflation” the universe would have ballooned from less than one-trillionth the size of a proton to about as big as a beach ball. Inflation would have ironed most unevenness out of the newborn universe, explaining why today it is remarkably smooth and homogeneous on large scales yet contains a web of galaxies on smaller ones.

The growth spurt would have caused spacetime to reverberate with gravitational waves that might have left an imprint on the CMB: swirls in the polarization of the light. Researchers operating a CMB telescope at the South Pole called Background Imaging of Cosmic Extragalactic Polarization 2 declared they had found such swirls in 2014, only to retract the claim a year later after discovering that much of the signal came from dust in our Galaxy.

Simons hopes to do better. Its small-aperture telescopes are optimized to see fluctuations on scales wider than $1^{\circ}$ , where the primordial polarization signal is expected to be strongest. They also observe at several wavelengths, helping distinguish the swirls from polarized emission from

galactic dust and other signals from the nearer universe. The first two of the scopes began observations almost 2 years ago, with the third joining in more recently. “From here on out, we should be digging down,” Dunkley says. “After 5 years or so, we might be able to see [the swirls].” Some models suggest it might take longer.

While the small telescopes chase inflation's polarization signal, the 6-meter mirror of the Large Aperture Telescope will create fine-scale maps of a large chunk of the CMB. It will funnel light onto a receiver packed with 60,000 detectors, which are cooled to one-tenth of a degree above absolute zero to register the faint CMB signal.

The maps could hold clues to what triggered inflation, Nadathur says. The standard version of inflation is driven by a single field mediated by a particle called an inflaton. But “maybe there was more than one type of field that was interacting in the early universe,” Nadathur says. The two scenarios would result in different distributions of fluctuation sizes in the CMB.

Simons researchers will also use the CMB as a backlight. Hot electrons in the thin gas between galaxies scatter CMB photons, changing their energy in a process known as the Sunyaev-Zeldovich effect. The distortions act as signposts for galaxy clusters, even when the galaxies are too distant or faint to see. An earlier telescope at the Atacama site found thousands of galaxy clusters this way. With its wide field of view, Simons should detect as many as 40,000, including clusters in the early universe that raise questions about cosmic structure formation, Devlin says. “How did you form such a big thing that early on? And what are the physics of that?”

Researchers also hope to exploit a related phenomenon called the kinematic Sunyaev-Zeldovich effect in which moving bodies of gas shift the wavelengths of CMB photons streaming toward Earth. Such “redshifts” or “blueshifts” could reveal the presence of dark matter without the usual signpost of visible stars. “We always assume that dark matter and [normal matter] are distributed in the same way in the early universe. Now we’ll be able to test that,” Kamionkowski says.

Devlin is looking forward to using the facility for so much more than studying the CMB. “I feel like we’re serving a community now that we weren’t accessing before. And that also is a lot of fun.” □

ECOLOGY Deep-sea life is still reeling from the BP oil spill

A 13-year study shows Gulf of Mexico ecosystems still haven't recovered ERIK STOKSTAD

After a deadly blowout on the Deepwater Horizon rig in 2010 sent oil gushing into the Gulf of Mexico, an emergency response team gambled on an unprecedented tactic. It sent robotic submersibles to the wellhead, 1500 meters below the surface, to inject chemical dispersants to break up the oil into tiny droplets and dissolve it. The hope was that by diluting the oil, the approach would minimize harm to wildlife. The move likely spared many seabirds, turtles, and shallow-water fish from oil that would otherwise have pooled at the surface. But it may have taken an unexpected toll in the deep sea.

A 13-year survey, begun the year after the spill, has discovered a steep, sustained decline in fish, crustaceans, and cephalopods in the deep waters of the gulf. The most likely cause is the oil spill, the team concludes this week in the Proceedings of the National Academy of Sciences, although it doesn't directly blame the dispersants.

“They have witnessed a major change in an ecosystem that we thought was isolated and perhaps protected,” says marine ecologist Bruce Robison of the Monterey Bay Aquarium Research Institute, who was not involved in the study. “I just don’t know whether the system itself is resilient enough to recover," he says. "That's a big question mark."

The study began 10 months after the disaster, which killed 11 crew members onboard the BP oil rig and released 5 million barrels of oil. Tracey Sutton, a biological oceanographer at Nova Southeastern University, organized a survey of the deep-sea ecosystem as part of a federal investigation into damages from the spill. Starting in February 2011, the team collected data from a research vessel equipped with sonar, which allowed it to estimate the abundance of schools of fish and crustaceans. The researchers also put down a trawling net that snagged marine life at various depths at 46 locations around the gulf. Working in day and night shifts, they pulled up and counted about 1200 species to create a snapshot of the ecosystem in the aftermath of the spill.

When the team returned 4 years later, it hoped to see signs of recovery. Instead, researchers found further, drastic declines. The populations of three major groups of animals in the survey—fish, crustaceans, and cephalopods—were far below levels recorded in 2011. The picture was no better in subsequent surveys. The numbers remained stubbornly low through to 2023.

Deep-sea fish, such as this snaketooth fish, have had steep declines.

Fish populations registered the largest declines, dropping by 64% compared with 2011. Because the team has no baseline data from before the spill, the declines may have been even greater than it reported.

The team didn't measure how much oil is still present in the ecosystem. But it suspects it continued to have an effect via the food web long after the spill. Years after the disaster, study co-author Isabel Romero, a chemical oceanographer at the University of South Carolina, found polycyclic aromatic hydrocarbons—a particularly toxic component of oil—in the eggs and tissue of deep fish.

The study offers “a sobering example of the unintended consequences of human activity at sea,” says Cynthia Smith, a conservation veterinarian who leads the National Marine Mammal Foundation and was not part of the effort. Jeffrey Drazen, a marine ecologist at the University of Hawaii at Manoa, is particularly impressed by the scale of the survey, which involved collecting samples with a trawl 2000 times, often at depths of more than 1 kilometer. “This is one of the most comprehensive sampling efforts ever conducted in the mesopelagic realm.”

It also has implications for life closer to the surface. Lanternfish—small fish with large eyes and glowing patches of blue, yellow, and green—experienced some of the steepest declines. The fish spend their days in the ocean depths and migrate upward at night to feed on zooplankton, where they are in turn eaten by tuna, swordfish, and whales. A scarcity of lanternfish, with many of the survivors possibly contaminated with hydrocarbons, could help explain a recent decline in whales in the gulf. Sperm whales are now about 30% less common there than before the spill, for example.

Steven Murawski, a marine ecologist at the University of South Florida, is surprised by the lack of recovery. He thinks an influx of animals from nearby populations, for example in the western or southern gulf, should have bolstered the depleted region. “There must be some cascading effect from the footprint of the oil spill to the larger community in general in the gulf,” he says.

Smith says the new study reinforces the need for a broader look at when and whether to use dispersants in oil spills. “Those decisions should consider all animals within the oil spill footprint, from the surface to the sea floor.”

It is also a cautionary tale about other industrial activities in the deep sea such as seabed mining, the authors say. “There’s this idea that populations in deep-sea environments are abundant and can’t be harmed,” says co-author Heather Bracken-Grissom, an evolutionary biologist at Florida International University. But the study indicates that’s not the case. “The deep sea is a much more fragile system than we thought,” Sutton says. □

GEOPHYSICS

Iron at Earth's heart may take a surprising form

X-ray experiments reveal cubic crystals that could complicate the picture of the inner core PAUL VOOSEN

Four years ago, a dozen scientists packed into a control room at the European X-ray Free-Electron

Laser (XFEL) Facility in Germany. A sliver of iron thinner than a human hair was squeezed to deep-Earth pressures between the tips of diamond anvils, then blasted to extreme temperatures by the x-ray laser. A surprising picture emerged on the consoles, says Sébastien Merkel, a geophysicist at the University of Lille who leads the \$2.5 million project, called HotCores. The crystal structure of the iron was cubic—the first time the arrangement had been seen at the dynamo that generates Earth's magnetic field. "If the structure is different, then the properties will be different," says Shuai Zhang, a high-pressure researcher at the University of Rochester.

The finding was difficult to publish. It finally appeared in August in the journal Physical Review B, after several high-profile journals turned it down, Merkel says. The delays may reflect resistance to reopening a question many researchers thought was settled. Yet to Jon Eggert, a materials physicist at Lawrence Livermore National Laboratory, "The data is very clear. I'm convinced they see BCC."

---

It reopens a topic that I thought was closed.

Sébastien Merkel

University of Lille

such high pressures and temperatures. The result seemed impossible, Merkel says. “It’s really the last thing we expected,” he says. “It reopens a topic that I thought was closed.”

For decades, experiments and computer simulations of Earth's inner core, an alien world of solid iron some 5000 kilometers below the surface, suggested the iron atoms there form close-packed hexagons. But word of the new result has quietly roiled the small community of inner-core researchers. If the structure is instead what is commonly called body-centered cubic (BCC), it could change how heat is conducted, altering when in geological history the inner core began to solidify and how heat and elements were released into the molten outer core. Those processes affect how the outer core churns, powering

Experiments that try to reproduce the extreme pressures and temperatures deep inside Earth come with serious complications. Diamond-anvil cells generate deep-Earth pressures but can introduce impurities that alter iron's structure, whereas conventional laser experiments can boost samples to high temperatures, but only for a single vanishing moment—too little time for further measurements.

By combining the XFEL with a diamond cell, the HotCores team could blast its samples with repeated, 30-femtosecond x-ray pulses. The x-rays act as both “pump and probe,” Merkel says. Each pulse heats the sample, and the x-rays scatter from its atoms to produce a snapshot of their arrangement—a diffraction pattern.

At first, the snapshots showed the expected hexagonal structure. But once pressures and temperatures rose above 2.3 million atmospheres and some $5700^{\circ}\mathrm{C}$ , a clear cubic signal emerged, Merkel says. The finding isn't definitive. Attempts to reproduce it in subsequent samples faltered when the diamond cell could not reach the same pressure. And unpublished

NEWS

Researchers prepare a sliver of iron for heating and squeezing to corelike conditions.

experiments using traditional laser shock techniques have yielded only hexagonal iron.

Yet Maurizio Mattesini, a geophysicist at the Complutense University of Madrid, feels vindicated by the result. “I’ve been suffering for such a long time,” he says. Mattesini argues that only cubic iron can explain some features seen in the seismic waves from earthquakes that pass through the inner core, such as a surprisingly slow speed. BCC, with a more loosely packed, less rigid structure than hexagonal iron, would hamper the waves, like soft sand slowing a runner. But other modelers have found plausible ways for denser hexagonal iron to slow seismic waves, too.

A paper published in 2021 by Yang Sun, a mineral physicist at Xiamen University, and colleagues had proposed that iron solidifying in the inner core would first crystallize into a cubic structure before settling into its final hexagonal form. “The phase that forms first does not have to be the phase that eventually dominates,” Sun says. The model could explain why the HotCores team saw BCC when the laser experiments did not. The sample heats and cools with each laser pulse, giving the transient cubic phase time to emerge. In conventional laser shock experiments, the sample experiences a single violent heating event.

Because the hexagonal and cubic phases can form under such similar conditions, they might both exist in the inner core, says Sally June Tracy, a mineral physicist at the Carnegie Institution for Science. Small changes in the core—for example, a dash of extra nickel and other light elements—could shift the balance to cubic, she says. Indeed, Merkel's team has since moved to testing these alloys with the x-ray laser. Although the work is unpublished, he says his team has found that iron with nickel and silicon tends to stabilize in the cubic form.

There's an irony to HotCores's discovery of cubic iron, Merkel adds. The first few lines of the team's grant proposal stated plainly that iron in the core is hexagonal. But now, what lies at Earth's heart is uncertain once again. "What's happening in the core?" Merkel says. "I don't know."

SCIENTIFIC COMMUNITY

Fired biologist wins \$6 million in defamation lawsuit

A jury ruled in favor of David Sabatini, dismissing accuser's claims of sexual harassment, retaliation PHIE JACOBS

Biologist David Sabatini, whose prominent career unraveled 5 years ago after an investigation found he had violated sexual harassment policies,

scored a major victory last week when a Massachusetts jury awarded him \$6 million—plus interest—in damages in his defamation case against Kristin Knouse, a former colleague at the Whitehead Institute for Biomedical Research. Her claims he sexually harassed her led one research institution to fire Sabatini and precipitated his resignations from Whitehead and the Massachusetts Institute of Technology (MIT), where he was a tenured faculty member.

Sabatini tells Science the hours leading up to the 16 October verdict were “the most nerve-wracking of my life.” To him, the jury’s decision represents “a clear vindication” that has brought him “a massive sense of relief.” The jury also rejected Knouse’s counterclaims of sexual harassment and retaliation.

The outcome came as a surprise to some legal experts, in part because two judges had earlier dismissed claims Sabatini filed against Whitehead and its director, Ruth Lehmann, and even some he filed against Knouse. After investigating Sabatini's conduct, Whitehead in 2021 concluded he had breached the institute's consensual relationships policy and its antiharassment policy. He had met Knouse while he was associated director at Whitehead and she an M.D.-Ph.D. student at Harvard University and MIT, where he was one of her instructors and served on her thesis committee. The two began a sexual relationship just before Knouse joined Whitehead as a fellow and started her own lab.

Although Knouse says she was coerced into the relationship by Sabatini, who at the time served as director of the Whitehead Fellows Program, he maintained it was consensual. He contended Knouse only leveled harassment accusations after he broke up with her to pursue another woman. A Suffolk County jury has now ruled in his favor, finding that Knouse defamed Sabatini and interfered with his ability to work.

“That’s a pretty big finding,” says Ann Olivarius, a lawyer who specializes in cases of sexual harassment. “Obviously, the jury really went against her in a big way." Olivarius was also surprised the jury awarded Sabatini such a hefty sum in damages. "That's really rare. This is a standout case."

The civil lawsuit verdict has no direct impact on the conclusions of Whitehead's probe, although Sabatini and his supporters view it as an exoneration. And some, including billionaire Bill Ackman, who has used his large social media platform to defend Sabatini and bankrolled his recent research, called on the institute to reconsider its findings and demanded Lehmann resign.

Knouse's attorney, Ellen Zucker, tells Science her client intends to appeal the decision. “The verdict is deeply disappointing,” she says, noting that several other women testified in court about “concerning interactions” with Sabatini. Requiring more than \$6 million in damages from an early-career scientist, Zucker argues, “is proof positive that the jury was not well-equipped to make appropriate decisions in this case.”

Sabatini rose to prominence with research into a molecular signaling pathway that regulates cell growth and metabolism and malfunctions in diseases such as cancer. At Whitehead, he won a prestigious position as a Howard Hughes Medical Institute (HHMI) investigator. In 2021, after an employee survey identified concerns in Sabatini's lab, Whitehead hired an outside law firm to investigate.

In addition to finding that Sabatini breached the institute's sexual relationships policy with Knouse, the investigation also concluded that Sabatini cultivated a sexualized lab environment and tried to influence the probe by misleading investigators and attempting to shape interviewees' testimony. As his official employer, HHMI fired Sabatini, who also relinquished his position and lab at Whitehead. Sabatini later resigned from MIT after three senior officials recommended his tenure be revoked.

Sabatini's lawyer, Lisa Arrowood, says the once high-flying biologist “became a complete pariah in the scientific community.” Sabatini has since made efforts to resurrect his career. In 2023, Ackman and an anonymous donor pledged a total of \$25 million to restart his lab. Later that year, Sabatini took a position at the Institute of Organic Chemistry and Biochemistry of the Czech Academy

of Sciences. The institute recently opened a branch in the Boston area, where Sabatini now has lab space.

In 2024, the U.S. Department of Health and Human Services (HHS) announced it was seeking to debar him from receiving any federal research funding because of the accusations. Sabatini confirmed that in September 2025 the agency did ban him from receiving National Institutes of Health grants for a period of 1 year. But that debarment was terminated early, in April, according to an HHS email provided to Science by Sabatini.

Sabatini has argued there was no power imbalance between himself and Knouse. “She had her own lab, she had her own money, she had her own students,” Arrowood says of Knouse. But the idea that Sabatini did not hold a position of power over Knouse, a much younger colleague early in her career, strikes Olivarius as “ridiculous.” “Look who he is, and look who she is. ... That's not an equal relationship."

Yet Regina Barzilay, a computer scientist at MIT who describes herself as a friend and colleague of Sabatini, says the original Whitehead probe was “extremely one-sided” and she is “overjoyed” that Sabatini had won his case.

To Zucker, however, the verdict against her client is emblematic of larger cultural issues: “This trial and this jury’s verdict seems to me to be a sad marker of our times, where it is still hard for women to be believed and even harder to hold powerful men to account.”

Sabatini, his lawyer says, plans to appeal the earlier summary dismissals of his claims against Whitehead and Lehmann, which included defamation and, for accepting Knouse's version of events over his, gender discrimination. According to Olivarius, both he and Knouse likely face an uphill battle. "Appeals are hard to win, always." □

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A lasting aftershock

The tsunami that hit Indonesia in 2004 following an undersea earthquake left 170,000 dead and forced more than half a million people from their homes. More than 20 years later, a new study has found, people who witnessed the devastation may have lasting health effects including metabolic imbalances. In a study posted last month on the preprint server bioRxiv, researchers tracked levels of thyroid hormone and other health markers in 3270 people in households from which they had baseline data dating before the disaster. The team found lower thyroid hormone levels among people from the areas worst hit by the tsunami, as well as more obesity, higher cholesterol, and other indicators of poor metabolic health. The researchers concluded that stress caused by the devastation—some of which is pictured here at a mosque in Banda Aceh 2 days after the tsunami—may have permanently altered the hormone's ability to regulate physiological functions. —Sara Reardon

EYES ON THE BALL

A “robo ump” that calls balls and strikes in Major League Baseball makes its World Series debut this week. It has to be near-perfect

JON COHEN, at Petco Park in San Diego

t 6 a.m. on 8 October, Kyle Wait and Tyler Danby towed Pelican cases and duffel bags filled with gear onto the home field of baseball's San Diego Padres. The night before, the team had lost a

heart-wrenching game here, silencing 47,712 roaring fans and eliminating the Padres from the playoffs.

Aside from 2 dozen pristine baseballs, known as pearls, the men brought no baseball gear into the still-dark ballpark. But their high-speed cameras, tripods, lasers, rulers, plumb lines, radars, and a custom-built, piston-powered cannon that fires baseballs had everything to do with a question key

Major League Baseball tested its Automated Ball-Strike Challenge

System during spring training in 2025.

to every game: whether a pitch is in the strike zone, crossing home plate at just the right height and depth, or misses the zone—a ball.

Wait and Danby, who both work at the Sports Science Laboratory run by Lloyd Smith at Washington State University (WSU), worried about

the darkness of the field, where most of the light towers were shut off, and the beer-flavored mist from the cleanup crew's power washing. At the invitation of Major League Baseball, they were about to do a “ground truth” of a technology introduced this year that represents one of the biggest changes ever in MLB's 123-year-old history: the Automated Ball-Strike (ABS) Challenge System, more commonly known as “robo ump.” And their cameras, which cost more than \$100,000 each, thrive on light and hate moisture.

After a flurry of emails and phone calls, the stadium lights started to blaze. The cleaners retreated. It was game on.

Over the next 3 hours, the two photographed 100 cannon-shot pearls crossing home plate at about 90 miles per hour, images they will analyze back at WSU to calibrate the park's camera-based ABS system. (Science style is to use metric measurements, but baseball decidedly does not.) “I love doing this,” said Wait, an erstwhile wildlife ecologist who once used cameras to track carnivores and has worked as a ground truth specialist checking MLB’s 30 stadiums for 7 years. “Perfecting our methods is just a constant battle,” Danby says.

The core confrontation in baseball is between a pitcher and a batter, but there's another important player in that drama—the home plate umpire, who decides in a split second whether an unswung pitch is a strike or a ball. Players and managers in the past could not, officially, challenge the ump's decision. But that didn't stop grown adults from swearing, wildly gesticulating, and acting like spoiled children when they disagreed with a call, risking ejection from the game. Given that three strikes end a batter's turn and four balls wins them a walk to first base, the stakes are high.

Even umps knew calls were regularly missed—19 in one 2022 game made especially memorable by a star slugger's temper tantrum over the incorrect calls. So MLB has turned to an ABS system made by Hawk-Eye Innovations that uses five cameras around the baseball field to check the umpire's calls. For an industry that grosses \$12 billion a year, with games, careers, and more billions in bets riding on the fate of pitches, the system has to be near-perfect. “People ask, ‘We know you use Hawk-Eye to grade the umpires, but who grades Hawk-Eye?’” says electrical engineer Clay Nunnally, a baseball scientist at MLB. “WSU grades Hawk-Eye.”

With MLB's ABS system, a pitcher, catcher, or batter can now challenge an umpire's call of a ball or strike by tapping the top of his helmet or cap within 2 seconds. A few seconds later, the pitch's trajectory appears in slow motion on the stadium's jumbotron, showing the precise location of the baseball when it crossed the halfway point of home plate (see graphic, p. 376). Teams start games with just two challenges, which are only retained if calls are overturned.

MLB's regular season this year saw 10,557 ball or strike challenges, and corrected calls changed games significantly. Three weeks ago, an extra-innings playoff contest ended on an ABS appeal, which turned a called ball into strike three. When a call gets overturned, fans sometimes go wild. But the robo ump calms down emotions on the field: Ejections over ball-strike disputes plummeted from 110 last season to 11, because the digital evidence leaves less room for contention.

Tracking a ball traveling not much faster than a car on a freeway for less than 60 feet might seem a simple assignment for today's technology. But the high stakes make fraction-of-an-inch precision crucial. Two ABS approaches, developed for different sports by a radar engineer and a computer scientist, competed for the major league job, with Hawk-Eye edging out its rival. And surprising variables can alter each system's accuracy. "It's not trivial to track the ball and figure out where it's at," Smith says. "There are a lot of things that come into play."

AT MLB'S START in 1903, the strike zone was a 3D concept. A baseball hit the zone if it crossed any part of home plate above the knees of a player and below his shoulders. For the Hawk-Eye ABS system this year, however, the strike zone is a 2D plane at the center of the plate that is adjusted for each player's height. MLB measures each player, without shoes on, at the beginning of the season. The measurement is done both by hand—using stadiometers or sliding wall rulers—and with lasers. It takes place between 10 a.m. and 12 p.m. to avoid the spinal compression that occurs over the course of a day.

ABS systems don't just capture the ball as it crosses home: They track its initial position, velocity, and acceleration throughout its half-second journey to the plate, calculating its trajectory toward the strike zone. “You gain overall precision in the measurement by using the full trajectory, rather than a single point,” says retired particle physicist Alan Nathan, a Smith collaborator who maintains a website called the Physics of Baseball.

Pitch-tracking technology first came to MLB ballparks 20 years ago, but originally just to help coaches and

players improve pitching and batting. It's been used as an ABS system in MLB's minor leagues for the past 5 years. "We test these things pretty significantly before we bring anything to the major league," says Joe Martinez, a former MLB pitcher who's now a vice president in the organization.

An early two-camera ABS system, PITCHf/x, used in the minor leagues between 2006 to '15, claimed an accuracy of half an inch and got TV viewers used to seeing whether a ball was truly in the strike zone. But then Fredrik Tuxen, an electrical engineer from

Denmark who knew nothing about baseball growing up, offered a more precise technology.

Tuxen had helped develop Doppler radars for the military to track missiles. Owners of golf driving ranges approached him and asked whether he could create a Doppler device to gauge the distance of their balls. A devoted golfer, Tuxen already knew it could be done: He had pulled out his clubs at the U.S. Army's Yuma Proving Ground 10 years earlier when he finished testing a missile-detecting radar. "After 2 hours, I managed to actually track a golf ball, but the problem was I had a \$2 million radar," he says.

Among the players who can challenge an umpire's strike or ball call, by tapping their heads, pitchers have the lowest success rate.

This led Tuxen in 2003 to co-found a company called Trackman, which developed a much cheaper radar that could fit into a large briefcase but still follow a golf ball. Sales took off. "People immediately said, 'Hey guys, you need to take this to baseball, they're crazy about data,'" he recalls.

The Trackman system sends out roughly 24,000 pulses of radio waves

The umpire's view of the strike differs from that of the cameras.

Catchers have the highest success rate with challenges.

In the zone

An ABS strike is defined as a pitch that crosses home plate's halfway point within a player-adjusted height range and inside its 17" width.

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Umping the umps

The camera-driven

Automated

Ball-Strike (ABS)

Challenge System

introduced by Major

League Baseball

this season allows

the pitcher, catcher,

or batter to contest

pitch calls made

by umpires.

during a pitch's brief flight. Receivers capture the reflections from the ball, which reveal its speed, position, and—by tracking the ball's stitched seams—how fast it spins. The aerodynamic forces that spin creates, known as the Magnus effect, can deceive batters by causing a ball to deviate from a straight path. Many players and coaches didn't immediately see the value of the machine. “For years, players have looked with their eyes and talked about stuff—‘This was a nasty pitch’ and all that—and to me as an engineer, that didn’t make sense,” Tuxen says. “I need numbers.”

By 2010, Trackman delivered the numbers, putting science into the art of pitching. It showed, for example, that an MLB pitcher's average curve-ball spins at 2450 revolutions per minute (rpm) and revealed the degree at which it tumbles or twists. Pitchers learned for the first time that a curve spinning faster than 2600 rpm was more likely to fool a batter to swing and miss—a strike.

Trackman initially provided entertainment for MLB broadcasts, distinguishing pitch types—the eye can't easily tell a cutter from a slider—and trajectories, as well as pitch locations. To improve Trackman, Tuxen hired Smith's team to do ground truths.

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Points of view

The ABS system designed by Hawk-Eye Innovations relies on five high-speed cameras around the ballpark. Because pitches can travel at more than 100 miles per hour, cameras might not capture the exact moment the baseball crosses midplate, so Hawk-Eye includes the trajectory of the ball in the equation that determines whether a pitch was a ball or a strike.

Then MLB decided to assess umpires with an ABS system. “That’s where I got involved,” Smith says. “If you’re going to use that to evaluate people, especially if there’s a union, you have to have some independent system that says, this actually works.”

Tuxen has been delighted to watch the robo ump gain traction in the sport. “It’s interesting when you have an old game like baseball, with all this culture around it, including having an umpire,” Tuxen says. “Now you have modern technology meeting it. How do you bridge that?”

MANY OF THE people who work on ABS systems played baseball themselves, but not Smith. “I would have been voted the least likely to be an athlete,” he says. He came to the game via his expertise in composite materials. Collaborating with Nathan, a lifelong amateur ball player, he began studies of the performance of different kinds of bats—wood, metal, and composite. The work involved firing baseballs at stationary bats, and Smith was hooked. “I kind of got into this by coincidence, but I found the research so interesting, and who wouldn’t enjoy a career building cannons?” he says.

MLB only allows wood bats, but colleges and other leagues permit other materials. That market is large, and the income from bat research allowed Smith to create the WSU sports lab, which has nearly 2 dozen staff. Together they have published more than 50 papers about baseball and softball, in journals ranging from Sports Engineering to Composite Structures. More than 2 dozen graduate students have come through with theses examining cricket bats, ice hockey sticks, shuttlecock drag, taekwondo, and the aerodynamics of baseball's oddest pitch, the knuckleball.

When Smith began to evaluate Trackman, his team soon discovered subtle factors can affect the radar results. The weight of a sellout crowd, for example, can cause a stadium to sag. “The radar orientation might change a 100th of a degree, but that translates into inches at the plate, and inches matter in baseball,” Tuxen says.

To improve accuracy, Trackman added a camera to its system, supplementing the radar with optical data. In 2015, MLB put Trackman in all 30 of its ballparks in conjunction with the rollout of its own data analytics platform, Statcast. Trackman data helped teams evaluate future players, and some professional pitchers bought units to sharpen their “stuff.” Professional baseball teams in South Korea and Japan began to use the radar system for analytics, too.

MLB didn't test Trackman as a robo ump until 2019, however, and the next year, it switched to Hawk-Eye, which relies entirely on cameras to track the ball. MLB won't comment directly on the decision, but Hawk-Eye was equally accurate, possibly cheaper, and provided more information. At the time, “it was much more sophisticated,” Tuxen acknowledges.

A U.K.-based company started in 2001 by computer scientist Paul Hawkins, Hawk-Eye first set out to adjudicate difficult calls in cricket, his first love. Purchased by Sony 10 years later, Hawk-Eye is now used in some 20 sports, including tennis, soccer, football, and rugby. For baseball, Hawk-Eye initially relied on 10 cameras, but added an 11th to detect the ball's spin and then another just because the computers could handle its data. Some of the cameras track player movements, but five focus on the ball, imaging its flight at 300 frames per second. "We're now at a point with optical tracking that we're measuring the actual orientation of the ball's seam," says Matthew Gaydon, a baseball tech manager at Hawk-Eye.

Even that fast frame rate may still miss capturing the ball at the moment it enters or misses the 2D strike zone now used by MLB. “The ball travels about 5 inches in between raw measurements and we’d have to be lucky to get an actual measurement right at the plane of the strike zone at midplate,” Nunnally says. So like Trackman, Hawk-Eye calculates a trajectory and extrapolates it across the strike zone.

By combing data from 3000 test pitches evaluated by WSU with both Trackman and Hawk-Eye, MLB has determined the median ABS “error” for both systems is now 0.17 inches. “Even though we call this ‘error,’ it is more a gauge of uncertainty,” Nunnally says.

MANY FACTORS can degrade Hawk-Eye's performance, and MLB had to pause its ABS system eight times this year during games. Hawk-Eye cameras can go out of alignment because of intense heat, the ground shifting under the ballpark, or having lenses cleaned during a game because of rain, fog, or sea spray. That's why WSU's team is here at Petco Park to evaluate how Hawk-Eye's five ABS cameras—four of them set on beams above the nosebleed

section, the highest tier of seats behind home plate, and one in the outfield—have held up.

During a ground truth test at Petco Park, Tyler Danby fires a fastball from the cannon to home plate.

The testers use two of their own cameras, which at 2500 frames per second operate much faster than the ABS ones. After using a level, laser, and a plumb at home plate to precisely calculate the height, width, and depth of a 3D strike zone, Wait and Danby record 100 pitches fired by the cannon on the mound, each accompanied by a boom and a puff of condensation as the compressed air expands and cools. At Hawk-Eye's control room in Atlanta, technicians simultaneously run Petco's ABS cameras. The technicians can remotely focus them if need be, combating changes in lighting from clouds or the Sun, which they did during each of the 24:30 games played in MLB this season.

The ground truthing goal is to test how accurately the system measures position, velocity, and spin. Danby

orients each pearl in the cannon's claw so the cameras can follow the seams and the writing printed on the ball, including the word “OFFICIAL” flanked by two stars. “To do spin rate, we track surface markers,” Wait explains.

The WSU team will calculate the “offsets” between its coordinates and the ones recorded by Hawk-Eye cameras, but the academic ball location evaluation is far slower than the ABS system’s in live play. “The crazy thing is, the pitch is thrown, and they know the [strike zone location] instantly,” Wait says. “We’ll do this, and I’ll tell you next week what the answer is.”

Hawk-Eye will then adjust its cameras to correct for imprecisions.

Gaydon thinks the automated ump revolution is just beginning. He expects Hawk-Eye technology will make its way down to high school games or even Little League contests, with smartphones in fixed locations providing the cameras. “I can’t wait for the day where the parent who’s invested everything into their 9-year-old starts arguing with the poor umpire, and he’s like, ‘I didn’t make the call. The camera way up there did,’” Gaydon says.

Besides making the umps' job less contentious, the ABS system has given them some heartening news. MLB's comparisons of human pitch calls with automated ones showed that this season, human umps were correct 93.5% of the time. Martinez, the former MLB pitcher, isn't surprised. "Everybody, even more so now than ever, appreciates the jobs the umpires do back there." □

Former FBI counterintelligence agent Tam Dao now works on research security at Rice University. 378

THE INSTIGATOR

A single FBI agent spurred NIH's campaign against foreign intervention on U.S. campuses. Now, he's studying the extent of the problem JEFFREY MERVIS

The National Institutes of Health (NIH) has spent the past decade compiling information on hundreds of U.S.-based scientists it believes tried to illegally

help their country of origin, most often China. But it's never been clear what triggered NIH's aggressive pursuit of these scientists, many of whom eventually lost their jobs or even went to jail, and why it was so much more extensive than efforts at other federal agencies.

Mystery solved. Science has learned that Tam Dao, an academic psychologist-turned-FBI special agent for counterintelligence, laid the groundwork for NIH's campaign. "I led the investigation that started all this," Dao says, acknowledging for the first time his pivotal role as the United States competes with China for global leadership in science.

Dao remains an important player in the debate over research security. Now head of campus safety and research security at Rice University, he will be tackling a question that arguably should have been asked before NIH plunged ahead: How often do foreign governments try to steal research at U.S. universities?

“Tam brought [the problem] to our attention,” agrees Michael Lauer, former head of NIH’s extramural research program, referring to several meetings starting in 2014 in which Dao told senior NIH officials he believed scientists at the MD Anderson Cancer Center had violated the confidentiality of the NIH peer-review process to benefit colleagues at Chinese institutions. “He had copies of their emails, text messages, and computers, which obviously we didn’t have access to,” Lauer recalls.

Dao's investigation of MD Anderson, which resulted in the firing of three scientists of Asian descent in 2019, was one of hundreds of counterintelligence cases Dao handled during his 11 years at FBI's Houston field office, from 2012 to '23. His efforts were part of a broader push by the U.S. government called the China Initiative, begun in 2018 during President Donald Trump's first term to root out espionage. And he convinced NIH there was a serious problem it needed to address.

Spurred on by what Dao had compiled and shared, Lauer assembled his own team to ferret out more information on questionable practices, including a failure to disclose foreign ties. That led to hundreds of U.S. universities getting letters from Lauer asking them to investigate one or more faculty members holding NIH grants and take appropriate action. The effort grew over the next few years, and as of June NIH says it has found 238 cases of undisclosed affiliations, including 197 instances of unreported grant support. As a result, 122 scientists have lost their jobs and 216 have been banned as peer reviewers.

While NIH's probes continued, the Department of Justice (DOJ), FBI's parent agency, ended the China Initiative in 2022 under then-President Joe Biden after acknowledging that many people believed it had unfairly targeted scientists of Chinese descent. And Dao's feelings about its methods and its impact are nuanced.

“I spent my whole [academic] career developing mental health inventories that don’t overdiagnose or are biased against Asian Americans,” he says. “So any accusation of targeting Asian Americans hits me at the core.”

He agrees with critics that the China Initiative damaged the reputations of many innocent scientists and “deterred good people from coming to the U.S.” But he also thinks it “has helped the country more than it has hurt the country by deterring bad people from coming here … and making the country safer.” And he strongly defends the government’s tactics.

“I’m pretty sure there are people out there who are racist and will target [those of Asian descent],” he says. “But the FBI looks at the behavior, not the ethnicity, of an individual, and that behavior has to provide what we call reasonable, articulable facts to support a case.”

DAO'S PERSONAL HISTORY makes him both an unlikely candidate—and a perfect fit—to influence government policy on research security. Born in what was then Saigon on 5 April 1975, he and his family were evacuated just days before the city fell to the North Vietnamese on 30 April. “We were told to go to a certain place at a certain time,” Dao recalls learning from his father, a translator for the U.S. government.

Housed temporarily in a re-location center at Fort Chaffee in Arkansas, Dao's family eventually ended up in Houston, where they struggled to make ends meet. His parents worked minimum-wage jobs, and during the summers he and his three brothers fended for themselves. "Today that would be considered child abuse," Dao says. But his parents "had no choice."

They also put a priority on education. Following in the footsteps of his two older brothers, Dao graduated from the University of Texas (UT) at Austin. After 2 years at a well-paid but unfulfilling job managing real estate, the desire to make a bigger contribution to society led him back to school and a Ph.D. in counseling psychology from Florida State University. In 2009, he joined the faculty of the University of Houston, where he specialized in personality assessments.

His department was willing to sponsor him for tenure after only 3 years, Dao says, but he felt it was time to show his appreciation for “everything this country has done for my family." He applied for an FBI job, even though he lacked training in law enforcement—"I didn't even know how to shoot a gun"—and was beyond the age limit of 37 for new agents. He received an age waiver, survived the grueling boot camp, and was assigned to the Houston FBI office in 2012. After a few years he moved into counterintelligence, investigating whether U.S.-based academic scientists might be helping foreign entities illegally acquire research funded by the U.S. government.

One of his first counterintelligence cases involved MD Anderson, part of the UT system. But when Dao presented his findings to then-NIH Director Francis Collins; his top deputy, Lawrence Tabak; and Lauer, “we were all rather skeptical that there was any problem,” Lauer recalls. Dao says: “They said I was not credible, and that NIH-funded scientists had been trained not to do those things.”

A major reason for that skepticism was what Lauer calls “a culture gap” between the two agencies. “The kind of people who work for the FBI … come from very different backgrounds and have different perspectives about how the world works,”

Any accusation of targeting Asian Americans hits me at the core.

Tam Dao, Rice University

he explains. “And we’re not used to dealing with them.”

Dao wanted to bridge that gap using the currency of science: evidence. He got permission to share with NIH the information he and other FBI agents had amassed—an unusual approach that Dao says required months of delicate negotiations with his bosses.

The research on mental health assessments that Dao had carried out also established some common ground with the NIH officials. “He had been applying various modern statistical techniques to problems that were similar to the statistical techniques I had been using when I was studying cardiovascular disease,” recalls Lauer, who worked at the Cleveland Clinic before coming to NIH in 2007. “So there was a connection. He’s also a really nice person.”

Once NIH leadership had come around to Dao's conclusion, Collins sent a letter to some 10,000 institutions that NIH funds. Dao helped craft that August 2018 bombshell, which warned that “NIH is aware that some foreign entities have mounted systematic programs to influence NIH researchers and peer reviewers and to take advantage of the long tradition of trust, fairness, and excellence of NIH-supported research activities.”

The subsequent flurry of letters from Lauer sent universities scrambling to investigate possible involvement by their faculty in what NIH labels foreign interference. The phrase encompasses violations of rules that govern peer review or the requirement of grantees to disclose ties to foreign institutions. But many university administrators complained they lacked access to what NIH—through Dao—already knew about their cases. That ignorance, Dao says, contributed to the perception that Asian scientists were being unfairly targeted. He decided once again that what was needed was greater transparency.

“Traditionally, the FBI would do its own investigation [without involving the institutions],” Dao explains. “But when you do that, you’re at risk of bias. I didn’t like that approach. So I started to give them the classified stuff. I would say, ‘Here it is. You decide whether you have a problem.’” Dao estimates he held such briefings for more than 300 universities and medical centers during his FBI years.

He believes sharing FBI information with institutions has improved research security on campus. One important ingredient, he says, is bringing in faculty with the expertise to decide whether a breach, if it had occurred, could pose a threat to national security. Dao says his FBI colleagues don't possess such expertise.

“Most agents are trying to protect something that they don’t even understand,” Dao explains. “For example, what aspects of quantum pose a national security risk? Most FBI agents would have no idea. Neither do I, for that matter.”

TO MANY POLITICIANS from both parties, the MD Anderson case was all the proof they needed that academic institutions weren't doing enough to combat the perceived threat. A steady stream of DOJ press releases touting the indictments of individuals or settlements with institutions in cases involving so-called “malign foreign influences” suggested the problem was huge—and growing.

But many of the cases involving academics were later dropped or ended in losses by the government.

Dao's current project, funded last month by the National Science Foundation (NSF), is the first rigorous attempt to quantify the problem. It's part of NSF's new Research on Research Security Program, mandated by a 2022 law giving the agency increased responsibility for improving research security at U.S. universities and academic medical centers.

Dao and his team hope to survey as many as 1600 faculty members, divided into STEM—science, technology, engineering, and math—or non-STEM fields and by whether their institution conducts more or less than \$50 million a year in research. Those distinctions could be important, Dao says. “What if the rate among non-STEM faculty is much higher?” he asks. “Or what if we learn that the problem is rare at most top-ranked institutions?”

The study will use a definition of foreign influence that covers four types of inappropriate behavior by foreign governments: offering incentives or rewards, demanding that any collaboration remain secret, coercing scientists to participate, and the outright theft of intellectual property. Dao says the survey methodology can collect accurate information about the type and frequency of any questionable behavior without linking the answers to an individual respondent. However, he acknowledges that the chilling effect of the China Initiative could make faculty less willing to report any contacts, much less any missteps.

Dao hopes the results of his survey, to be fielded in the coming months, will address what he sees as two flaws in the current political debate over foreign influence. One is an inherent bias among law enforcement agencies to inflate the problem because they see so many examples of possibly illegal behavior. The second is the reluctance of scientists to consider that their peers are capable of such misconduct.

Dao promises to avoid both tendencies. “People who know me know that I’m driven by data,” he says.

Lauer, for one, trusts Dao to be able to walk that fine line and establish a baseline for foreign influence on U.S. campuses. “Tam is an extraordinarily capable person, and he is quantitatively oriented,” Lauer says. “So I think he would be the obvious person to attempt to answer the question.”

COMMENTARY

Barnes Ice Cap in Baffin Island, Nunavut, Canada, which is the last remnant of a continental glacier, has been receding since 1960.

PERSPECTIVES

GLACIOLOGY

Has the next ice age already come and gone?

The last remnant of a continental glacier shows that global warming may have forestalled the next glaciation

Shaun A. Marcott

Like a metronome, Earth has experienced ice ages on predictable “beats” driven by its planetary orbit around the Sun over the past 2 million years (1). However, future anthropogenic greenhouse gas emissions could place a decisive end to this cycle, forestalling the next ice age for hundreds of thousands of years (2). On page 455 of this issue, Young et al. (3) report the history of Barnes Ice Cap in northeastern Canada in response to natural and anthropogenic climate changes over the past 4000 years. The ice cap is the last remnant of the Laurentide Ice Sheet, a massive continental glacier that once covered nearly 30% of North America during the peak glacial period. The study suggests the glacier began to grow 2000 years ago but started losing ice by 1960 because of preindustrial global warming, likely signaling the end of the next ice age.

The Laurentide Ice Sheet has been growing and shrinking in step with each ice age cycle (4). At the peak of the last glacial maximum [\~20,000 years ago (5)], the ice sheet covered most of Canada and parts of the northern United States. By contrast, during the present interglacial interval (a geologic epoch of warmer global average temperature), it has mostly disappeared. Young et al. used a combination of geologic dating techniques to determine when Barnes Ice Cap was advancing and retreating during the past 4000 years. Surface exposure dating, which is a commonly applied method in alpine terrains (6), determines the duration of time when a rock surface was exposed to the atmosphere and cosmic radiation. Uncovered rocks interact with the cosmic rays, creating a steady buildup of rare isotopes, such as beryllium-10 ( $^{10}$ Be), at known rates. Young et al. measured the ${}^{10}$ Be isotope in both bedrock surfaces that have been newly exposed by the retreating ice and the surface of boulders that lie atop an extensive network of moraines (distinct ridges of unconsolidated debris) left behind when the glacier retreated. Nearly half of the obtained ${}^{10}$ Be ages contained isotopes that were inherited from prior exposures to cosmic rays, which is a common complication in polar or high-latitude environments where the glaciers' base remains frozen to the bed and erodes very slowly (7). Young et al. used a second chronologic technique that measures radioactive carbon-14 ( ${}^{14}$ C) isotopes from previously ice-entombed vegetation that have been preserved below the low-eroding ice. Dead vegetation covered by the glacier no longer takes up ${}^{14}$ C, thus providing an exact time stamp of when the glacier advanced over the materials.

By combining the measured dates with prior work in the region [e.g., (8)], Young et al. found that Barnes Ice Cap achieved its minimum dimension \~3600 years ago and then started to regrow around 2000 years ago. The advancing ice demarcates the beginning of the next glaciation driven by regional cooling from a decline in the amount of incoming solar radiation in summer (9). By the late 1950s, Barnes Ice

Cap had reached its maximum historical position. However, the mass balance of the glacier tipped into the negative in 1960 (10), and the ice cap began its historical marginal retreat. This retreat marks the demise of the next glaciation, following the regular ice age cycle.

Young et al. offer an important benchmark into how an ice sheet responds to climate change, potentially providing information about the beginning of prior glacial periods (11). Identifying glacial inceptions is challenging because the initial ice bodies at the commencement of an ice age are often too small to be detected with traditional methods (12), and pinpointing the exact nucleation location of a massive ice sheet is difficult. Young et al.'s newly acquired chronological data provides a way to determine the precise timing and rate of glacial inception, demonstrating how quickly the glacier responds to shifts in summer temperature. The authors argue that a series of climate feedbacks, such as changes in sea ice, from progressive cooling temperatures likely helped accelerate the observed regrowth of the remnant Laurentide Ice Sheet 2000 years ago. This aligns with previous work that recognizes changes in the amount of incoming solar radiation in summer as a key initial driver of past glaciations (13). It also highlights that other climate effects, such as changing albedo (the amount of the solar radiation reflected by the land surface) from snow and ice cover, are equally important in initiating glacial inceptions (14).

Will another ice age ever transpire? The next glacial inception is generally considered unlikely to occur in the next predicted cycle, but ultimately how many skipped glacial cycles occur is left to choices made by humanity and tied to the future carbon emissions (2). Humans are now geologic agents capable of thwarting millions of years of natural glacial cycles and offsetting Earth's climate for hundreds of thousands of years to come. The absence of future glacial cycles will be profound in the context of the geologic history of the past 2 million years and will have ramifications that will extend to other biological and physical systems that co-evolved with the ice ages (15). The study of Young et al. provokes some pause for thought about what an ice-free world might mean as the pendulum of the ice ages comes to rest.

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REFERENCES AND NOTES

1. J. D. Hays, J. Imbrie, N. J. Shackleton, Science 194, 1121 (1976).

2. D. Archer, A. Ganopolski, Geochem. Geophys. Geosyst. 6, Q05000 (2005).

3. N. E. Young et al., Science 394, 455 (2026).

4. A. S. Dyke et al., Quat. Sci. Rev. 21, 9 (2002).

5. P.U. Clark et al., Science 325, 710 (2009).

6. K. Nishiizumi et al., J. Geophys. Res. 94, 17907 (1989).

7. P.T. Davis, J. P. Briner, R. D. Coulthard, R. W. Finkel, G. H. Miller, Quat. Res. 65, 156 (2006).

8. G.H. Miller et al., Clim. Past 19, 2341 (2023).

9. B. S. Lecavalier et al., Proc. Natl. Acad. Sci. U.S.A. 114, 5952 (2017).

10. O.H. Loken, R. B. Sagar, Int. Assoc. Sci. Hydrol. Publ. 79, 282 (1967).

11. J. D. Ives, J. T. Andrews, R. G. Barry, Naturwissenschaften 62, 118 (1975).

12. A. C. Mix, W. F. Ruddiman, Quat. Res. 21, 1 (1984).

13. M. Milankovitch, Kanon Der Erdbestrahlung Und Seine Andwendung Auf Das Eiszeitenproblem (Royal Serbian Academy, 1941).

14. W.F.Budd, I.N.Smith, Geogr. Phys. Quat. 41, 279 (1987).

15. K. D. Burke et al., Proc. Natl. Acad. Sci. U.S.A. 115, 13288 (2018).

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ACKNOWLEDGMENTS

The author acknowledges support from the US National Science Foundation and the University of Wisconsin–Madison.

10.1126/science.aem3295

METABOLISM

Putting glucose metabolism under electronic control

An electronic device controls the redox mechanisms that regulate glucose concentrations in mice

W. E. Bentley $^{1}$ and G. F. Payne $^{1}$

Electrodes have been important tools for biological discovery and disease treatment. Luigi Galvani and Alessandro Volta discovered “animal electricity” decades before the theory of bioelectricity was accepted, and Alan Hodgkin and Andrew Huxley studied how action potentials propagate electrical signals in cells before the structure of DNA and the genetic code were resolved. Today, electrical measurements are routinely used to assess cardiovascular health (e.g., electrocardiograms) and brain activity (e.g., electroencephalograms). Electrodes also enable minimally trained individuals to perform life-saving interventions using publicly available defibrillators. In all these examples, an electrode influences ion-based electrical processes in an animal’s body. On page 400 of this issue, Maity et al. (1) report an implantable electrode that interfaces with biology through an entirely different mechanism based on reduction-oxidation (redox) reactions. This approach, which they tested in mice, targets type 2 diabetes, a debilitating disease that affects millions of people worldwide.

Redox reactions are ubiquitous in biology. They can occur in isolation, such as those that generate reactive oxygen species, but they can also assemble into spatially organized pathways in the cell, such as the respiratory electron transport chain in mitochondria. Redox reactions are also embedded within metabolic networks that balance the production and degradation of complex molecules (anabolism and catabolism, respectively). In addition to metabolism, redox processes are involved in regulatory and protein interaction networks that transduce environmental, social, and lifestyle exposures into biological responses $(2-5)$ . For example, electrodes can provide the cues that act on redox-responsive transcription factors and thus affect gene expression $(6)$ , a concept known as “electrogenetics” $(7, 8)$ . Maity et al. used an electrode that interacts with the body’s biological processes at a metabolic level: It oxidizes glucose electrochemically. This approach could become a drug-free intervention to treat type 2 diabetes and obesity.

How an electrode influences biological redox mechanisms is fundamentally different from how it monitors or affects the movement of ions. The charged particles in a redox network are electrons that flow through electron transfer reactions. This poses several challenges for using electrodes to influence redox biology (9). Because they target localized reactions, redox-based interventions are usually more invasive than ion-based interventions that rely on electric fields generated from electrodes applied to the surface of the skin. In the study of Maity et al., the electrodes that enabled electrochemical glucose oxidation were implanted subcutaneously in mice. Redox reactions also often require a high amount of energy for activation, which biology overcomes using enzymes, proteins that trigger specific molecular reactions. To address this challenge, Maity et al. developed a nonbiological graphite felt matrix with platinum-decorated gold nanoclusters as an electrocatalyst that promotes the selective electrochemical oxidation of glucose. Implanted electrodes are also sensitive to damage, which reduces their active lifetime. To preserve the electrode's performance over several days and even weeks, Maity et al. encapsulated it in a protective three-layer structure composed of cellulose, alginate, and albumin. Because glucose oxidation occurs at the electrode's surface, the oxidation rate scales with the electrode's surface area, whereas the need to remove excess glucose from blood scales with the animal's volume. Maity et al. used a 0.5-cm $^{2}$ electrode to control blood glucose concentrations in their mice studies. To ensure that the electrochemical stimulation was sufficiently harmless while conferring benefits, the intervention used low voltages (<1 V). This was sufficient to generate gluconate (a product of glucose oxidation), which is cleared by the kidneys, and to promote a shift from glucose-based to fat-based metabolism.

Maity et al. integrated these electrochemical capabilities into a wireless electrocatalytic closed-loop health optimization device, which they coupled to a commercially available continuous glucose-monitoring system. This setup converts biological information (glucose concentrations) into an electrical signal. This signal is analyzed through standard electronic technologies to generate an electrical response that is used to guide the electrode's intervention (oxidizing glucose).

Efforts to scale up this approach for human intervention would need to consider how to accommodate a greater blood volume and ensure stability in a different immune and metabolic milieu. An implantable electronic device that automatically detects and corrects excessive glucose concentrations, just as implantable defibrillators detect and correct life-threatening arrhythmias, could have advantages over current devices that detect glucose levels and release insulin to treat diabetes. These advantages include the possibility of human-and drug-free (rather than hormone-mediated) operation. The electronic nature of such a device would also facilitate communication with a smartphone for health monitoring and human-independent learning, which would enable personalized diabetes management. Existing bioelectronics devices provide notable access to the nervous and neuromuscular systems. A redox-based version of bioelectronics could reach other physiological systems, such as the immune and endocrine systems and the gastrointestinal tract, which are not so heavily dependent on ion-based electrical regulation but are strongly influenced by redox networks. Therefore, future electronic intervention devices might help to manage diseases other than diabetes, modulate human-microbiome interactions, or maintain redox homeostasis in stress conditions, among many other applications.

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REFERENCES AND NOTES

1. D. Maity, P. Guha Ray, P. Buchmann, G. Charpin-El-Hamri, M. Fussenegger, Science 394, eady8560 (2026).

2. D. P. Jones, H. Sies, Antioxid. Redox Signal. 23, 734 (2015).

3. H. Sies, R. J. Mailloux, U. Jakob, Nat. Rev. Mol. Cell Biol. 25, 701 (2024).

4. H. Sies, D. P. Jones, Nat. Rev. Mol. Cell Biol. 21, 363 (2020).

5. D. P. Jones, Free Radic. Biol. Med. 217, 179 (2024).

6. W. Weber et al., Nucleic Acids Res. 37, e33 (2009).

7. T. Tschirhart et al., Nat. Commun. 8, 14030 (2017).

8. J. M. Lawrence et al., Sci. Adv. 8, eabm5091 (2022).

9. E. Kim et al., Adv. Sci. 12, e10184 (2025).

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ACKNOWLEDGMENTS

The authors acknowledge support by the Defense Threat Reduction Agency (grant HDTRA1–19–0021), the Gordon and Betty Moore Foundation (grant GBMF11395), and the National Science Foundation (grant 2607564).

10.1126/science.aem0762

CELL BIOLOGY

A cell death ballet in two acts

Two proteins that permeabilize mitochondria promote cell death through distinct mechanisms

Cristina Muñoz-Pinedo $^{1}$ and Seamus J. Martin $^{2}$

Complex multicellular organisms require ongoing replacement of cells for many reasons, including aging, infection, and injury. In many situations, cell death occurs in response to stress through a regulated process called apoptosis (1). A key pathway to apoptosis involves two related proteins, Bcl-2-associated X protein (BAX) and Bcl-2-homologous antagonist killer (BAK), that form pores in mitochondria (2, 3). This releases cytochrome c into the cytosol to trigger activation of caspase proteases that coordinate apoptosis (4). BAX-BAK pores can also lead to delayed release of mitochondrial DNA (mtDNA) into the cytosol and the production of type I interferons (IFNs), which is a classical antiviral immune response (5, 6). On page 401 of this issue, Yang et al. (7) report two distinct BAX-BAK complexes—one for cytochrome c release that promotes immunologically silent caspase-dependent apoptosis and another that promotes mtDNA release, caspase-independent cell death, and IFN production to stimulate inflammation.

An overarching objective of apoptosis is the surgical removal of

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Dual acts at the mitochondria

In response to cell stress, distinct BAX-BAK complexes assemble to facilitate the release of factors that trigger distinct cell-death pathways. Complex I is immune silent, whereas complex II activates a robust immune response.

ANT1, adenine nucleotide translocator 1; BAK, Bcl-2–homologous antagonist killer; BAX, Bcl-2–associated X protein; cGAS, cyclic GMP-AMP synthase; IFN α/β, interferons α and β; PHB1,2, prohibitins 1 and 2; STING, stimulator of interferon genes; VDAC1,2,3, voltage-dependent channels 1, 2, and 3.

cells from tissues with minimal collateral damage to neighboring cells and the avoidance of inflammation (1, 8). This is largely facilitated by the swift recognition and removal of apoptotic cells by phagocytic cells before the loss of plasma membrane integrity, which precludes the release of proinflammatory molecules from dying cells (1, 9). For these reasons, apoptosis is typically immunologically silent. This is augmented by caspase-mediated inactivation of proteins that play key roles in promoting immune responses, such as cyclic GMP-AMP synthase (cGAS), interferon regulatory factor 3 (IRF3), and interleukin-33 (IL-33) (1, 10). Consequently, when apoptosis-associated caspase activity is suppressed—either pharmacologically or by pathogen-encoded caspase inhibitors—this can convert an otherwise immunologically silent mode of cell death event into a proinflammatory one (1, 5, 6, 8).

Diverse forms of cell stress, including DNA damage, protein misfolding, and viral infection, promote activation of BAX and BAK, which leads to mitochondrial cytochrome c release and formation of the apoptotic protease-activating factor 1 (APAF1)-caspase-9 apoptosome—a protein complex that activates “executioner” caspase-3 and caspase-7 downstream (4). This results in controlled cellular demolition through caspase-mediated proteolysis of hundreds of proteins, producing the classical apoptotic phenotype (1, 11). Because of the importance of BAX-BAK-mediated mitochondrial permeabilization for cell fate, the intricacies of this process have been intensively studied (2, 3, 12–14). Consequently, it is very well established that cell stress-initiated activation of one or more BH3-only proteins (those bearing a Bcl-2 homology domain 3) mobilizes BAX and/or BAK, resulting in their progressive oligomerization within the mitochondrial outer membrane to form pores or channels that permit cytochrome c efflux. BAX-BAK pores can subsequently coalesce to form macropores that have been implicated in mtDNA release, but how this occurs has been the subject of debate (12–14). BAX-BAK-dependent mtDNA release has important consequences because this can activate the cGAS-stimulator of interferon genes (STING) pathway to trigger the production of antiviral IFNs, but this is typically counteracted by caspase-mediated proteolysis of cGAS and IRF3 (10). However, in cells that lack APAF1 or where caspase activity is suppressed, mtDNA-driven IFN production is unleashed (5, 6).

Previous studies proposed that apoptosis-associated mtDNA release results from BAX-BAK macropore-driven herniation of the mitochondrial inner membrane through the outer membrane, leading to eventual rupture of the inner membrane and mtDNA release through such hernias (12, 13). However, Yang et al. provide evidence for the formation of two distinct BAX-BAK complexes in mitochondria: complex I, which has a low molecular weight (\~160 kDa) and facilitates cytochrome c release, and complex II, which has a high molecular weight (\~600 kDa)—comprising BAX, BAK, voltage-dependent anion-selective channel proteins 1 to 3 (VDAC1, VDAC2, and VDAC3), adenine nucleotide translocator 1 (ANT1), and prohibitins 1 and 2 (PHB1 and PHB2)—and is essential for mtDNA release and activation of the cGAS-STING pathway. In an unexpected twist, the study suggests that complex II is required for cell death (which the authors call baciptosis) under conditions where apoptosome-mediated caspase activation is suppressed (see the figure).

Yang et al. demonstrate that mammalian cells that are deficient in complex II (lacking VDAC1, VDAC2, or PHB2) can still release cytochrome c and undergo BAX-BAK-dependent mitochondrial herniation but exhibit greatly attenuated mtDNA release and IFN production. Precisely how mtDNA release is facilitated by complex II is not clear, although evidence suggests that BH3-only proteins can induce conformational remodeling of VDAC channels within this complex, leading to calcium influx and mtDNA efflux. Unexpectedly, the authors observed that mtDNA release is required for caspase-independent cell death. Cells deficient in VDAC1 or VDAC2 exhibited BAX-BAK-dependent cytochrome c efflux, but not mtDNA release, and survived for several days under conditions where downstream caspase activation was suppressed. Ablation of mtDNA also attenuated caspase-independent cell death under conditions where complex II was present. The study's findings challenge the prevailing view that caspase-independent cell death is a passive consequence of mitochondrial outer membrane permeabilization and cytochrome c release leading to mitochondrial dysfunction. However, how cytosolic mtDNA instigates caspase-independent cell death remains to be determined, although the cytosolic DNA sensors cGAS, Z-DNA binding protein 1 (ZBP1), and interferon-inducible protein 16 (IFI16) do not appear to be involved.

The study of Yang et al. suggests that BAX-BAK activation can result in two distinct modes of cell death, each guided by distinct BAX-BAK complexes that promote either cytochrome c-initiated caspase activation leading to apoptosis or mtDNA-initiated activation of an unknown cytosolic effector or effectors resulting in caspase-independent cell death. Notably, whereas the former mode of death is immunologically silent, the latter is accompanied by a robust antiviral immune response (5–7). The complex II-mediated route to cell death may have evolved as a backup to counter viruses and other pathogens that harbor caspase inhibitors to suppress the apoptosome route to cell death. Such an eventuality would warrant the initiation of a strong inflammatory response, which apoptosis typically mitigates against (1, 8), as well as a fail-safe route to cell death that operates independently of caspases. Thus, assembly of complex II to drive mtDNA release could be viewed as a form of effector-triggered immunity that is initiated in response to the detection of pathogen activity (i.e., caspase inhibition) as opposed to the detection of pathogen-associated molecular patterns, which is the predominant form of immunity in higher organisms (15). There are also instances where APAF1 expression is epigenetically silenced in certain cell types, such as neurons and cardiomyocytes, or in certain cancers, where complex II-initiated caspase-independent cell death may also play a role.

Questions that remain unresolved by the current study include the identity of the nucleic acid sensor that initiates cell death on detection of mtDNA in the cytosol. How complex II promotes mtDNA efflux and whether it is inhibited by caspases also remains to be clarified. The mechanism of mitochondrial permeabilization identified by Yang et al. sets an exciting stage for the next steps in the BAX-BAK cell death ballet. □

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REFERENCES AND NOTES

1. S. J. Martin, C. M. Henry, S. P. Cullen, Mol. Cell 46, 387 (2012).

2. H. L. Glover, A. Schreiner, G. Dewson, S. W. G. Tait, Nat. Cell Biol. 26, 1434 (2024).

3. P. E. Czabotar, A. J. Garcia-Saez, Nat. Rev. Mol. Cell Biol. 24, 732 (2023).

4. X. Jiang, X. Wang, Annu. Rev. Biochem. 73, 87 (2004).

5. M.J. White et al., Cell 159, 1549 (2014).

6. A. Rongvaux et al., Cell 159, 1563 (2014).

7. S. Yang et al., Science 394, eaea2181 (2026).

8. M. Beltrán-Visiedo et al., Nat. Rev. Mol. Cell Biol. 26, 884 (2025).

9. I. K. H. Poon, K. S. Ravichandran, Annu. Rev. Pharmacol. Toxicol. 64, 339 (2024).

10. X. Ning et al., Mol. Cell 74, 19 (2019).

11. R. C. Taylor, S. P. Cullen, S. J. Martin, Nat. Rev. Mol. Cell Biol. 9, 231 (2008).

12. K. McArthur et al., Science 359, eaao6047 (2018).

13. J. S. Riley et al., EMBO J. 37, EMBJ201899238 (2018).

14. K. Cosentino et al., Mol. Cell 82, 933 (2022).

15. B. C. Remick, M. M. Gaidt, R. E. Vance, Annu. Rev. Immunol. 41, 453 (2023).

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ACKNOWLEDGMENTS

S.J.M. acknowledges support from the European Research Council advanced grant program (DESTRESS, AdG 101020534).

10.1126/science.aem1247

$^{1}$ Institut d'Investigació Biomèdica de Bellvitge (IDIBELL), Barcelona, Spain. $^{2}$ Molecular Cell Biology Laboratory, Department of Genetics, Smurfit Institute of Genetics, Trinity College, Dublin, Ireland. Email: martinsj@tcd.ie

The cognitive power of the avian brain

Carrion crows make decisions faster than monkeys and humans Michael Colombo and Oriane Poutrain-Sorel

Once regarded primarily as creatures of instinct and simple learning, birds are revealing cognitive abilities that rival and sometimes surpass those of primates. Even the pigeon, an animal not typically associated with high cognitive skills, can distinguish between images of cancerous and healthy

cells, represent the concepts of same and different, perform numerical discriminations, and tell the difference between words and nonwords in ways that resemble aspects of human reading. Corvids (crows, ravens, scrub jays, and rooks) show even more impressive abilities, such as self-recognition, tool use, problem solving, episodic memory, theory of mind, and planning for future events, at levels that often exceed similar abilities in primates. On page 445 in this issue, Schmidbauer and Nieder (1) report that carrion crows can make ultrafast and accurate decisions.

These findings add to the growing appreciation of the abilities of the avian mind.

Having the same operating principles narrows the cognitive gap between birds and primates, but it does not fully explain the high levels of cognition and fast decision-making abilities of birds. Another explanation is that although small, the avian brain has a disproportionately large number of neurons. A rhesus monkey brain is eight times larger than that of a raven (another species of corvid with impressive cognitive abilities), but it only has three times the number of neurons (6.3 billion versus 2.2 billion). The source of this disparity is the size of neurons: Bird brain neurons are smaller than those in the primate brain, and therefore more neurons can be packed into the same volume of tissue (see the figure) (6).

However, if the rhesus monkey brain has three times the number of neurons as the raven brain, should that not still confer a cognitive

Schmidbauer and Nieder trained carrion crows to report whether random dots appearing on a computer screen moved either up or down, or left or right. Once the dots began to move, the crows reported their direction by pecking a target that appeared above or below the dots moving up and down, or on either side of the dots moving left and right. The crows took \~235 ms to make their decision and respond, a speed that is twice as fast as that of rhesus monkeys (2) and humans (3) performing a similar task. Furthermore, the accuracy of the crows' decisions remained very high. Schmidbauer and Nieder also measured the crows' neuronal activity in the nidopallium caudolaterale, an area of the brain that is functionally equivalent to the primate prefrontal cortex. They noted that direction-selective neurons activated \~70 ms after the onset of the moving dot stimuli and \~170 ms before the birds produced a response.

What factors account for the ultrafast decisions of crows and their impressive cognitive abilities? Researchers often attribute the cognitive performance of pri-

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Punching above one's weight

Birds display high cognitive skills despite having much smaller brains than mammals. Birds do not have a layered brain organization but have smaller neurons that are arranged in clusters. A high neuronal density and short interneuron distances support fast information processing and decision-making.

Carrion crow

Corvus corone

Rhesus macaque

Macaca mulatta

mates to a large brain with billions of neurons and to a cortex that processes information through recurrent (repetitive) neural circuits that span six cortical layers. However, birds' brains are much smaller and have no cortex, which would suggest they have far less computational power. How then can their cognitive abilities and decision-making speed match or exceed those of primates? Part of the answer lies in their brain architecture. In contrast to the layered organization of the primate cortex, neurons in the avian pallium (which contains the nidopallium caudolaterale), an area broadly analogous to primate cortex, are arranged in clusters (4). Despite this difference, the repetitive neural circuitry of the primate brain is also present in the avian brain, with radially organized fibers that process sensory information connecting to tangentially running fibers that associate information across different brain regions (5). Functional abilities arise from this circuitry, regardless of the brain's overall architecture. Thus, the avian brain processes information in a manner similar to that of the primate brain.

advantage to the monkey? Not necessarily. Birds have proportionally more of their neurons in the pallium compared with the proportion of brain neurons in the primate cortex (6, 7). For example, monkeys have approximately 1.7 billion cortical neurons, whereas ravens have 1.2 billion pallial neurons (6). This would place ravens on nearly the same cognitive playing field as monkeys. The difference further diminishes when the comparison focuses on the number of neurons in the subregions of the cortex or pallium that are most involved in cognition, such as the prefrontal cortex of primates and the nidopallium and mesopallium of the avian brain. For example, rooks (a corvid species smaller than a raven) have the same number of neurons as chimpanzees—around 600 million—in these specialized regions involved in cognition (7).

The densely packed neuronal arrangement of birds' brains not only makes the brain compact, but it also makes it fast. Higher neuronal densities result in shorter distances between neurons, which leads to faster conduction times and a higher speed of information processing (6, 7). These effects are likely to explain the ultrafast decisions of carrion crows in the study of Schmidbauer and Nieder. Together with other emerging evidence on the remarkable cognitive abilities of birds, these findings prompt a rethink about the power that is packed into the small avian brain. □

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REFERENCES AND NOTES

1. P. Schmidbauer, A. Nieder, Science 394, 445 (2026).

2. T. Hanks et al., eLife 3, e02260 (2014).

3. J. Palmer et al., J. Vis. 5, 376 (2005).

4. H.J. Karten, Ann. N. Y. Acad. Sci. 167, 164 (1969).

5. M. Stacho et al., Science 369, eabc5534 (2020).

6. S. Olkowicz et al., Proc. Natl. Acad. Sci. USA 113, 7255 (2016).

7. F. Ströckens et al., J. Comp. Neurol. 530, 1588 (2022).

10.1126/science.aem0341

BOOKS ET AL.

REFLECTION

The microscope and the metaphor

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Science shows us what to do to save the planet—poetry helps us understand why we should

Phillip Levin $^{1}$ and David Hassler $^{2}$

In January 2017, as the incoming Trump administration removed climate change information from the White House website and imposed new restrictions on communications by federal scientists, poet Jane Hirshfield responded not with an essay or a protest speech but with a poem. Three months later, this poem, “On the Fifth Day,” appeared as a full-page advertisement in The Washington Post, a week before Hirshfield recited it during the March for Science on the National Mall (1).

The poem did not provide new evidence about climate change or biodiversity loss. Science had already done that. Instead, it reminded people why that evidence mattered. It gave voice to grief, responsibility, hope, and wonder at a moment when scientific facts alone seemed insufficient. As Hirshfield has often said, the microscope and the metaphor are both instruments of discovery.

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POETRY ARTICULATES WHY EVIDENCE MATTERS

The relationship between poetry and science is often framed in terms of communication: Poetry and other art forms can help explain science to broader audiences. While this certainly is true, it understates the unique contributions each can bring to the conversation.

Science helps us understand what is happening, why it is happening, and which interventions are most likely to make a difference. Poetry can address a different challenge: helping people care enough to engage by activating emotion, imagination, identity, memory, and values—the qualities that often determine whether science becomes personally meaningful (2, 3).

Rather than just serving as a way to communicate science, poetry can help create the emotional and cultural conditions that make such knowledge meaningful. Put simply, science can help us ask “What should I do?” and “How will I know if it worked?” whereas poetry and other art forms can help us ask “Why should I care?”

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FOSTERING CONNECTION FOR CONSERVATION

A growing body of research supports the complementary relationship between poetry and other art forms with conservation science in particular. People attending programs that intentionally combine art and science report learning more about biodiversity while expressing greater willingness to participate in conservation-related activities (4). Arts-based conservation education has also improved understanding while correcting misconceptions about threatened species (5). More broadly, studies suggest that artistic experiences can foster empathy, curiosity, and emotional connection in ways that make scientific information more memorable and relevant [e.g., (6)]. Reviews of environmental art likewise suggest that aesthetic experiences can strengthen connections to nature and increase intention to engage in proenvironmental behavior (7).

None of this suggests that poetry or other art forms can replace conservation science. Rather, the evidence points toward a productive complementarity: Art can strengthen motivation to engage, while science provides evidence that can help channel that motivation toward effective action. This relationship echoes a broader body of work arguing that conservation depends not only on ecological knowledge but also on human values, experiences, and relationships.

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POETRY BROADENS WHAT COUNTS AS KNOWLEDGE

Conservation decisions are rarely based on ecological information alone. They are also shaped by history, culture, identity, memory, and lived experience. These forms of knowledge can be difficult to capture in maps, models, or journal articles, yet they can strongly influence whether conservation efforts succeed or fail. Artistic practices—including storytelling, poetry, photography, performance, and other creative methods—offer ways to make lived experience, cultural memory, and place-based knowledge visible without requiring them to conform to scientific conventions (8).

The boundary between scientific and artistic ways of knowing is permeable. Scientists increasingly use poetry and other creative forms to explore dimensions of their work that conventional scientific writing cannot capture: grief, wonder, uncertainty, attachment, and awe. Such work does not replace scientific inquiry; it reveals something about the human experience of conducting it.

To this end, as I (Levin) began working with 100s of colleagues on The Nature Record—the first-ever scientific assessment of nature in the US (9)—in 2024, my coauthor (Hassler), along with poets Luisa A. Igloria and Aileen Cassinetto, developed a companion anthology of poetry entitled The Nature of Our Times: Poems on America's Lands, Waters, Wildlife, and Other Natural Wonders (10). The anthology brings together voices from the arts, ecology, academia, and Indigenous communities, including marine ecologist Maya Zeff, whose poem “I translate the sea” lyrically captures the mutualisms that define marine ecosystems, and wildlife ecologist Lara Volski, whose poem “The Monarch Bear” incisively describes the reciprocal influence of people and animals on one another (see sidebar). Zeff and Volski’s work illustrates how scientific observation and poetic attention can emerge from—and contribute to—the same sustained engagement with the natural world.

The importance of multiple ways of knowing is particularly evident in work with Indigenous peoples and local communities. Arts-based approaches here have helped document cultural connections to the ocean, illuminate histories embedded in landscapes, and create space for multiple forms of knowledge to inform conservation planning (11).

In 2020, Anishinaabe poet, scholar, and environmental activist Kimberly Blaeser founded In-Na-Po—Indigenous Nations Poets—a national Indigenous poetry community committed to mentoring emerging writers, nurturing Indigenous poetic practices, and raising the visibility of Native writers (12). Blaeser and In-Na-Po have collaborated with other organizations that connect poetry, Indigenous knowledge, language, community, and relationships with the natural world. Their 2023 mentoring retreat in Door County, Wisconsin, produced “Poems for a Tattered Planet,” a series of poetic films created in collaboration with Overpass Light Brigade (13). Rather than competing with scientific evidence, such collaborations can enrich the knowledge available to conservation, contributing to a more complete understanding of the ecological and social systems conservation seeks to sustain.

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SCIENCE HELPS DIRECT ACTION

Motivation alone is not enough. The history of conservation is full of well-intentioned actions that failed because they were based on incomplete understanding or ineffective interventions. Science provides an evidence-based foundation for deciding where to act, which actions are most likely to succeed, how to evaluate trade-offs, and whether desired outcomes are actually achieved. Whereas poetry can help generate the public will to conserve nature, science ensures that effort is directed toward actions that benefit biodiversity rather than simply making us feel that we have done something useful.

The relationship is therefore reciprocal rather than hierarchical. Art without science risks inspiring ineffective action; science without art often struggles to inspire action at all. Neither is sufficient by itself.

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THE NEXT FRONTIER

Despite the growing interest in art-science collaborations, rigorous evidence about their long-term conservation effects remains limited. Much of the recent literature consists of conceptual frameworks, synthesis papers, project descriptions, and reflections on emerging practice rather than evaluations of conservation outcomes [e.g., (14)]. This work nevertheless identifies promising new roles for artists—not simply as communicators of scientific findings but as collaborators who can help shape research questions, reveal overlooked perspectives, and catalyze new forms of problem solving.

An important next step is to test the full pathway from artistic experience to motivation, from motivation to evidence-based decisions, and ultimately to lasting changes in human behavior and biodiversity. Comparative and longitudinal studies will be important for identifying which artistic approaches are most effective for different audiences and conservation contexts, and under what conditions art-science collaborations generate outcomes beyond those achieved through conventional conservation communication or engagement alone $(7, 14)$ .

It is within this emerging field that the Wick Poetry Center at Kent State University will convene the first Poets for Science Gathering in November 2026 (15). The gathering will bring together poets, scientists, educators, clinicians, students, environmental advocates, policymakers, artists, and the public to explore the meeting ground between science and poetry.

The meeting will celebrate art-science collaborations but also challenge them. When does a poem (or, in other contexts, performance art, visual art, or story) change not only what someone feels but what they do? Which collaborations produce lasting effects, for whom, and under what circumstances? And can those changes ultimately be linked to healthier ecosystems and more resilient communities?

Science reveals how the natural world works and how it is changing. Poetry reminds us why that world matters. Conservation needs the tools of both—the microscope and the metaphor. Understanding how they work together may become one of the field's most important questions.

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REFERENCES AND NOTES

1. J. Hirshfield, "On the Fifth Day," The Washington Post, 14 April 2017.

2. D. J. Curtis, N. Reid, I. Reeve, S. A. P. I. EN. S. 7, 1655 (2014).

3. S. Dupont, J. Mar. Biol. Assoc. U.K. 97, 1211 (2017).

4. O. Opermanis, S. N. Kalnins, A. Aunins, J. Nat. Conserv. 28, 67 (2015).

5. M. Franquesa-Soler, L. Jorge-Sales, J. F. Aristizabal, P. Moreno-Casasola, J. C. Serio-Silva, PLOS ONE 15, e0228382 (2020).

6. P.-C. Wang, C.-Y. Yu, Sustainability 10, 1098 (2018).

7. A.-S. Tribot, D. Faget, T. Richard, T. Changeux, Biol. Conserv. 276, 109791 (2022).

8. R. E. Brennan, Ocean Coast. Manag. 162, 110 (2018).

9. The Nature Record; https://naturerecord.org/.

10. L.A. Igloria, A. Cassinetto, D. Hassler, Eds., The Nature of Our Times: Poems on America's Lands, Waters, Wildlife, and Other Natural Wonders (Paloma Press, 2025).

11. M. Strand, N. Rivers, B. Snow, Front. Mar. Sci. 9, 886632 (2022).

12. Indigenous Nations Poets, About In-Na-Po; https://www.indigenousnationspoets.org/about-us.

13. Indigenous Nations Poets, "Poems for a Tattered Planet" (2023); https://www.indigenous-nationspoets.org/poems-for-a-tattered-planet.

14. I. Jarić et al., Front. Ecol. Environ. 23, e70012 (2025).

15. Poets for Science Gathering, Wick Poetry Center, Kent State University, 12 to 14 November 2026; https://poetsforscience.org/gathering-2026/.

10.1126/science.aej4196

LETTERS

Edited by Jennifer Sills

Teams compete to raise tipis at the University of Regina in Saskatchewan, Canada. This annual event reflects the longstanding partnership between the University of Regina and the First Nations University of Canada.

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Indigenous higher education needs support

Indigenous knowledge systems are central to addressing conservation challenges. Indigenous universities provide spaces where Indigenous languages, knowledge systems, and worldviews thrive. Such universities deserve reliable support from their countries' governments.

From stewardship of protected areas to environmental governance, Indigenous voices have reshaped scientific and policy discussions about humanity's responsibilities toward Earth (1, 2). Institutions such as the First Nations University of Canada, Tribal Colleges and Universities in the United States, and the Federal Indigenous University in Brazil help to revitalize and sustain languages, cultures, and knowledge systems that have guided human-environment relationships for generations (3–5). These Indigenous-led institutions also develop local expertise by training specialists who can bridge knowledge systems to address complex social-ecological interactions, thus strengthening research, governance, and local stewardship capacity (3).

Despite their important role, Indigenous universities remain highly dependent on unstable political support. In Brazil, the establishment of the Federal Indigenous University represents a historic investment in Indigenous-led higher education (6), but elsewhere, institutions continue to struggle. Amawtay Wasi University, the first intercultural university in Ecuador, has faced drastic budget and staff reductions, compromising its operations (7). In Mexico, intercultural universities have faced chronic resource limitations, as well as limited institutional autonomy owing to political interference (8, 9). The Indigenous Universities of Bolivia (UNIBOL) have also faced governance, infrastructure, and budgetary constraints (10), and the University of the Autonomous Regions of the Nicaraguan Caribbean Coast (URACCAN) in Nicaragua continues to operate under historical marginalization, ongoing challenges to Indigenous autonomy, and limited resources (11).

As Indigenous and allied scholars from institutions across the Americas, we applaud the development of new Indigenous universities and urge governments to move beyond symbolic commitments and invest in the long-term stability, autonomy, and growth of Indigenous-led higher education. In the United States, the Tribally Controlled Colleges and Universities Assistance Act of 1978 established a federal framework supporting Tribal Colleges and Universities, a network of Indigenous-led institutions that support language revitalization, cultural preservation, and training (5). Similarly, New Zealand strengthened long-term support for Māori-led wānanga by replacing annual grants with an ongoing statutory funding mechanism to provide greater funding certainty (12). Together, these examples demonstrate how long-term legislative and funding commitments can support the stability, autonomy, and growth of Indigenous-led higher-education institutions. Governments across the Americas should establish long-term funding mechanisms, strengthen institutional autonomy for intercultural and Indigenous-led organizations, and support Indigenous educational sovereignty.

Bruno Eleres Soares $^{1,2}$ , Thaïs Bernos $^{3}$ , Rodrigo F. R. Carmo $^{4}$ , Lucas Colares $^{5}$ , Jaime Grimm $^{6}$ , Alessandra Higa $^{7}$ , Anna-Leah King $^{8}$ , Andrew M. Miller $^{9}$ , Robert Newman $^{10}$ , Andrea M. D. Ortiz $^{11}$ , Andrea Sterzuk $^{8}$ , Vincent Ziffle $^{12}$

$^{1}$ Institute of Environmental Change & Society, University of Regina, Regina, SK, Canada. $^{2}$ Programa de Pós-Graduação em Ecologia, Universidade Federal do Rio de Janeiro, Rio de Janeiro, RJ, Brazil. $^{3}$ Rubenstein School of Environment and Natural Resources, University of Vermont, Burlington, VT, USA. $^{4}$ Departamento de Biologia, Universidade Federal Rural de Pernambuco, Recife, PE, Brazil. $^{5}$ Coordenação de Zoologia, Museu Paraense Emílio Goeldi, Belém, PA, Brazil. $^{6}$ Department of Biology, University of Victoria, Victoria, BC, Canada. $^{7}$ Department of Math, Science, and Technology, Oglala Lakota College, Kyle, SD, USA. $^{8}$ Faculty of Education, University of Regina, Regina, SK, Canada. $^{9}$ Department of Indigenous Studies, First Nations University of Canada, Regina, SK, Canada. $^{10}$ Department of Biology, University of North Dakota, Grand Forks, ND, USA. $^{11}$ Departamento de Geografia, Universidad de Concepción, Concepción, BI, Chile. $^{12}$ Department of Indigenous Knowledge and Science, First Nations University of Canada, Regina, SK, Canada. Email: soares.e.bruno@gmail.com

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REFERENCES AND NOTES

1. S.J. Bruce, Conserv. Biol. 40, e70254 (2026).

2. E. S. Brondízio et al., Annu. Rev. Environ. Resour. 46, 481 (2021).

3. S. Brant, K. Williams, D. Longboat, Front. Educ. 11, 1702361 (2026).

4. K. Leonard, J. Comp. Int. Hig. Educ. 13, 90 (2021).

5. E. S. Huaman, B. Chiu, C. Billy, Educ. Pol. Anal. Archiv. 27, 101 (2019).

6. Presidência da República, Lei No. 15.418, de 28 de maio de 2026. Cria a Universidade Federal Indígena (Unind) (2026); https://www.planalto.gov.br/ccivil\_03/\_ato2023-2026/2026/lei/I15418.htm.

7. R. Revelo, "Consejo de Educación Superior aprueba intervenir la Universidad Amawtay Wasi, centro educativo habla de denuncia falsa," Primicias (13 July 2026); https://www.primicias.ec.

8. M. Lloyd, Intercult. Educ. 35, 402 (2024).

9. S. Schmelkes, Intercult. Educ. 20, 5 (2009).

10. M. M. Chundary, Rev. Educ. Sup. Soc. 36, 195.

11. J. Cupples, K. Glynn, Singap. J. Trop. Geo. 35, 56 (2014).

12. New Zealand Ministry of Education, Education Report: Providing Greater Funding Certainty to Wananga (24 April 2024); https://web-assets.education.govt.nz/s3fs-public/2026-02/MARKED\~1.PDF.

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India needs a tree conservation plan

India holds 2603 known tree species, 650 of which are endemic, and 469 of which have already been assessed as threatened (1, 2). In October 2025, India's Ministry of Environment, Forest, and Climate Change launched the National Red List Assessment, a 5-year, nearly US\$10 million effort to evaluate roughly 11,000 species, including 7000 plants, against International Union for Conservation of Nature (IUCN) Red List criteria (3). However, identifying risk is not the same as acting on it. India should augment its substantial assessment investment with a conservation plan for the species found to be vulnerable.

Other countries have already built National Conservation Action Plans for their threatened trees. For example, Guinea, Gabon, Ghana, and Kenya, all of which have far fewer tree floras than India has (1), have each implemented and budgeted for time-bound frameworks that assign priority species to specific institutions for seed banking, habitat protection, or field research (4–8). Guinea's plan covers 76 threatened species. Colombia, the second-most tree-rich country in the world, also has a plan, which covers 701 threatened species (8). Every plan ties conservation action directly to Red List data and includes a formal review cycle.

India should build a similar system, timed to the 2030 deadline it has already set for its National Red Data Books. Existing programs such as the Green India Mission and Compensatory Afforestation Fund support tree planting at scale but do not designate funding or institutional responsibility for named threatened species (9). Every species assessed as threatened should be added automatically to a standing action list rather than awaiting separate political approval. The plan should set explicit conservation targets, such as seed-banked backup for a defined share of threatened species. In addition, the plan should include a 5-year review synchronized with the Red Data Book timeline, so that species assessment and conservation action remain on the same schedule rather than drifting apart.

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Anurag Dhyani

Jawaharlal Nehru Tropical Botanic Garden and Research Institute, Thiruvananthapuram, Kerala, India. Email: anuragdhyani@gmail.com

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REFERENCES AND NOTES

1. Botanic Gardens Conservation International (BGCI), "State of the world's trees" (BGCI, 2021).

2. M. Rivers, A. C. Newton, S. Oldfield, Plants People Planet 5, 466 (2023).

3. Ministry of Environment, Forest and Climate Change, Government of India, “National Red List Assessment of Indian flora and fauna: Vision 2025–2030” (2025).

4. C. Couch, Herbier National de Guinée, "Plan d'Action National de Conservation pour les Arbres Menacés de Guinée" (Royal Botanic Gardens, Kew, and Herbier National de Guinée, 2023); https://www.herbierguinee.org/uploads/2/6/3/0/26303479/panc\_arbres\_menaces\_guinea\_v2b\_2023.pdf.

5. GaboTREE Project, “Plans d’actions de conservation multi-espèces des espèces d’arbres les plus menacées du Gabon” (Fondation Franklinia, 2023); https://www.tropicos.org/projectimages/Gabon/GaboTREE/PACarbres.pdf.

6. BGCI, IUCN SSC Conservation Planning Specialist Group, CSIR-Forestry Research Institute of Ghana, "Planning conservation action for Ghana's threatened tree species" (BGCI, 2023); https://www.bgci.org/wp/wp-content/uploads/2023/03/PCAGhanaMedRes.pdf.

7. Y. Harvey-Brown, K. Shaw, Eds., "Planning Conservation Action for Kenya's Threatened Trees" (BGCI, 2020).

8. C. Lopez-Gallego et al., "Plan de acción para la conservación de los árboles de Colombia" (2024).

9. Ministry of Environment, Forest and Climate Change, Government of India, "Year-End Review 2025" (2025).

10.1126/science.ael9835

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AI biosecurity must include agriculture

Advances in biological artificial intelligence (AI) have brought biosecurity to the center of public debate, and the US Congress is now considering the Biosecurity Modernization

and Innovation Act (1). Yet this debate, like biosecurity more broadly, remains focused largely on human health and overlooks the importance of pathogens that affect crops and livestock. The United States and governments worldwide should prioritize crop and livestock protection by minimizing the likelihood of deliberate pathogen attacks and making the targets less vulnerable to harm.

Agricultural pathogens can threaten food security, economies, and political stability. Southern corn leaf blight destroyed roughly 15% of the US corn crop in 1970, and Panama disease devastated global banana production and severely harmed the economies of several countries, fueling labor strikes and political upheaval across Central America (2–6). Genetic uniformity, dense production systems, and globally connected supply chains in modern agriculture amplify these risks.

Agricultural pathogens also present distinctive risks for misuse. Many important agricultural host-pathogen systems are well characterized, experimental materials are readily accessible, and host specificity can reduce risk to the developer (7–10). Unlike transmissible human pathogens, they may also allow harm to be concentrated in particular crops, livestock populations, or environments, potentially reducing blowback. AI could exacerbate agricultural products' vulnerability to targeted attacks.

Agricultural biosecurity therefore needs a continuous array of defenses spanning prevention through response. The US Department of Agriculture has already called for treating farms and food systems as national security assets (11); that effort deserves strong support and expansion. DNA synthesis screening should cover high-consequence agricultural pathogens as rigorously as human pathogens. AI evaluations should explicitly test capabilities relevant to agricultural misuse.

Biological surveillance should expand to encompass fields, herds, wildlife, vectors, and traded commodities. Governments should also strengthen agriculture-specific diagnostics, veterinary vaccines, resistant cultivars, quarantine capacity, and rapid-response pipelines. Layered defenses can preserve legitimate research while preventing deliberate misuse.

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Jonathan Feldman $^{1,2}$ , Tal Feldman $^{3}$ , Pardis C. Sabeti $^{2,4,5,6}$

$^{1}$ College of Computing, Georgia Institute of Technology, Atlanta, GA, USA. $^{2}$ Broad Institute of MIT and Harvard, Cambridge, MA, USA. $^{3}$ Yale Law School, New Haven, CT, USA. $^{4}$ Department of Organismic and Evolutionary Biology, Harvard University, Cambridge, MA, USA. $^{5}$ Department of Immunology and Infectious Diseases, Harvard T. H. Chan School of Public Health, Harvard University, Boston, MA, USA. $^{6}$ Howard Hughes Medical Institute, Chevy Chase, MD, USA. Email: pardis@broadinstitute.org

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REFERENCES AND NOTES

1. US Congress, Senate, Biosecurity Modernization and Innovation Act of 2026, S. 3741, 119th Congress, 2nd Session January 2026; introduced in the Senate on 29 January 2026.

2. S. Marquardt, Am. Hist. Rev. 106, 49 (2001).

3. L.A. Tatum, Science 171, 1113 (1971).

4. P. Balint-Kurti, J. Pataky, Phytopathology 114, 2007 (2024).

5. R. C. Ploetz, Crop Prot. 73, 7 (2015).

6. R. Harding et al., Plant Biotechnol. J. 23, 3628 (2025).

7. T. Nobori, Cell Host Microbe 33, 1227 (2025).

8. M. Urban et al., Nucleic Acids Res. 50, D837 (2022).

9. C. Verdonk, KK Gagalova, S. Raffaele, MC Derbyshire, Comput. Struct. Biotechnol. J. 27, 2881 (2025).

10. A. W. Woodward, B. Bartel, Genetics 208, 1337 (2018).

11. US Department of Agriculture, "National farm security action plan," technical report (US Department of Agriculture, July 2025).

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COMPETING INTERESTS

P.C.S. is an inventor on intellectual property related to pathogen diagnostics and vaccines and a founder and shareholder at Delve Bio and Lyra Labs.

CLIMATE FINANCE

Fiscal discipline without physical resilience

Reforms could shift fiscal discipline and resilience investment into reinforcing forces rather than competing ones

Aayushi Mishra $^{1}$ , Advait Arun $^{2}$ , Evan Kodra $^{1}$ , Auroop R. Ganguly $^{1,3}$

As extreme weather intensifies, climate-vulnerable nations face two threats: debt default and physical exposure. The International Monetary Fund (IMF) and multilateral development banks manage the first threat well, rewarding fiscal discipline through credit ratings and lending terms, but

no equivalent mechanism rewards resilience investment. This gap can compound over time if a disaster strikes an underprepared economy, and resulting borrowing crowds out the next round of resilience investment—something prior work has modeled as a climate-debt doom loop. What hasn't yet been documented is how the loop unfolds in real time within a single country during a disaster. We trace this empirically using Hurricane Melissa in Jamaica in October 2025 and propose reforms—embedding resilience into debt sustainability analysis, scaling Resilience and Sustainability Trust (RST) funds, and adopting Climate Resilience Debt Clauses (CRDCs)—that could shift fiscal discipline and resilience investment into reinforcing forces rather than competing ones.

Between 2013 and 2024, Jamaica reduced its public debt (i.e., money owed both through loans from international lenders and bonds sold in financial markets) from roughly 144% of its gross domestic product (GDP) to 72% by 2023 (1), with a target of 60% by fiscal year (FY) 2027–2028. This debt reduction happened through years of disciplined spending restraint, primary surpluses, and rigid fiscal rules. Jamaica adopted these rules voluntarily, under its own Fiscal Responsibility Framework, rather than as an IMF condition. Maintaining them also kept borrowing costs low, giving the government further reason to stay the course. In September 2025, Jamaica's sovereign debt rating was upgraded by S&P Global to signal broad institutional confidence in its fiscal trajectory. Then Hurricane Melissa struck a few weeks later as a Category 5 storm, causing an estimated US\$12.2 billion in total damage, losses, and costs (roughly 56.7% of 2024 GDP) (2). Insurance payouts covered a small fraction of losses, with a large share of recovery financing being in the form of new sovereign borrowing. Within weeks, the hard-earned fiscal space that the debt reduction had created was once again under pressure.

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CLIMATE-DEBT DOOM LOOP

There are many possible reinforcing mechanisms that can initiate a climate-debt doom loop, particularly for slower moving, chronic climate effects on growth and fiscal capacity (3). For the acute, disaster-driven version of the loop that is our focus here, the loop goes through three reinforcing mechanisms: institutional pressure to prioritize debt service over capital investment, a structural gap between disaster risk financing and actual recovery costs, and postdisaster borrowing that recreates the fiscal constraints that precluded investing in resilience in the first place. Here, we track each step of the loop in the weeks after Hurricane Melissa hit Jamaica in 2025, using Jamaica's public financial and disaster loss data as was reported (fig. S1). Two questions guide this tracing, drawing on disaster risk assessment and risk management research, and on mechanism design, respectively: first, how accurately disaster risk tools like insurance and catastrophe bonds capture real losses, and second, how institutional incentives could be redesigned to reward resilience building just as consistently as they reward debt repayment currently.

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Underinvestment in physical resilience

In FY2024–2025, Jamaica allocated approximately US\$3.15 billion to debt service (\~15.8% of GDP), roughly six times its US\$510 million in total public capital expenditure (\~2.5% of GDP) [see supplementary materials (SM)]. This fiscal structure left coastal defenses underbuilt relative to physical risk, drainage infrastructure systems deferred, and critical systems underinvested in.

This imbalance reflects, in part, how sovereign creditworthiness is currently assessed. Although some credit rating agencies have begun to incorporate climate risk into their supplementary reports, these factors remain peripheral to their core decision-making. The fundamental framework of a sovereign credit rating is still based on a narrow and near-term liquidity logic: Rating agencies prioritize the size of the primary surplus, the pace of debt-to-GDP reduction, and how strictly a nation applies fiscal rules. This same incentive structure likely applies far beyond Jamaica, especially given evidence that climate vulnerability can materially affect sovereign creditworthiness (3, 4). Although dedicated resilience funds like the Green Climate Fund (GCF) exist, they are often narrow in scope and small relative to the broader physical resilience needs discussed here. They also do not address the debt service pressure or the rating agency incentives that exacerbate the doom loop. For example, Jamaica's first ever GCF investment was approved in 2026 for \$50 million for mostly farming resilience projects (see SM). Put differently, though there is resilience funding available, it may be both too small and disconnected from the mainstream systems that determine a government's fiscal flexibility.

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A structural protection gap

Jamaica's postdisaster financing gap cannot be explained by underinvestment alone. Even countries with robust resilience infrastructure face residual losses due to extreme events, which disaster risk financing instruments like catastrophe bonds and parametric insurance are designed to address (5). Both instruments pay out on the basis of predefined physical measurements like wind speed, storm track, and central pressure exceedances, instead of assessed damages, though the money moves through different markets. With parametric insurance, Jamaica buys a policy directly from a regional insurer [such as the Caribbean Catastrophe Risk Insurance Facility (CCRIF)], which calculates

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The protection gap

For hurricanes Beryl and Melissa, catastrophe (CAT) bonds and parametric insurance through the Caribbean Catastrophe Risk Insurance Facility (CCRIF) covered under 3% of losses. | Hurricane Beryl (Category 4, July 2024) | Hurricane Melissa (Category 5, October 2025) | Total losses | US$1 billion | US$12.2 billion | Losses (% of GDP) | ~5% | ~57% | CAT bond payout | US$0 million | US$150 million | CCRIF + other payout | ~US$27 million | ~US$92 million | Coverage ratio | ~3% | ~2% | a payout that scales with the storm's measured severity once losses cross a set threshold (see SM). A catastrophe bond works through capital markets instead: for example, the World Bank issues the bond to outside investors, who lose a share of their principal on a similar sliding scale if the storm crosses the same kind of threshold, with the money flowing to Jamaica. Either way, the payout is rapid and objective, but it is also decoupled from the disaster's actual cost. The gap between what a parametric instrument pays and the actual cost of the disaster is known as basis risk.

Jamaica's two recent storms illustrate the consequences. Hurricane Beryl (July 2024), caused an estimated US\$1 billion in damages. Yet, Jamaica's World Bank catastrophe bond paid nothing because its measured intensity fell short of the bond's minimum payout threshold, and the CCRIF covered only US\$26.6 million (2.7% of losses). By contrast, Melissa met every trigger, resulting in a full US\$150 million

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Decomposition of the post-Melissa increase

Relative to the pre-Melissa debt-to-GDP ratio, the estimated post-Melissa increase is driven by a numerator effect from recovery borrowing and a denominator effect from lost output, following standard debt-ratio accounting. | Stage | Public Debt(% of GDP) | Pre-Melissa baseline | 60% | Recovery borrowing | +6.4 pp | GDP shortfall (lost output) | +2.1 pp | Post-Melissa peak | 68.5% | pp, percentage points.

payout; when combined with other aid through the CCRIF, the total coverage amounted to US\$242 million (2% of losses) (see the first table).

In both cases, the instruments performed exactly as specified, yet for sovereign nations, this results in a gap between contractual performance and fiscal adequacy: Jamaica's disaster risk financing strategy worked, instruments triggered and paid as designed, yet most of the losses were left uncovered. Current institutional architecture has no mechanism to reconcile these two frameworks at present (6).

Expanding parametric coverage carries recurring costs of annual premiums, paid regardless of whether a storm strikes. When concessional borrowing (more generous terms than market lending) is available after a disaster, the long-run costs might be comparable to insurance premium costs. However, parametric instruments offer two key advantages over postdisaster borrowing. Payouts arrived within 3 to 14 days of landfall, and the World Bank catastrophe bond's payout was confirmed within 10 days, compared with the roughly 3 months Jamaica waited for its IMF disbursement to be approved (see SM). Parametric payouts also do not add to the sovereign debt stock. The second advantage is crucial, as every dollar borrowed after a disaster compounds through interest and crowds out future capital spending, whereas an insurance payout does not.

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Debt-financed recovery

With parametric instruments covering under 2% of the losses, the government's recovery financing came overwhelmingly from new borrowing, roughly US\$3.6 billion (\~18% of pre-Melissa GDP). This single-year borrowing already exceeds the \~15% of GDP flow-financing threshold that the IMF's debt sustainability framework treats as a risk marker for emerging-market sovereigns and approaches the 20% threshold that is applied to advanced economies (see SM). The new post-Melissa debt is spread across the IMF, World Bank, and three regional development banks at mostly undisclosed terms (see SM).

We modeled total nominal obligations (principal plus interest) under terms ranging from concessional to near-market pricing: US\$4.9 billion to US\$5.7 billion (24 to 29% of pre-Melissa GDP). At concessional rates, their net present value falls below the principal, so lending is a real fiscal concession. What binds Jamaica, though, is the annual cash payment, not its discounted value, because those payouts are what compete with the capital budget each year. At peak repayment, the new debt service alone would approach, or exceed, Jamaica's entire annual capital budget (see SM).

This closes the doom loop: Postdisaster borrowing crowds out precisely the predisaster investment that would have reduced losses. Combined, this recovery borrowing and the disaster's dampening effect on output are projected to push Jamaica's debt-to-GDP ratio to a peak of $\sim 68.5\%$ , an 8.5 percentage-point increase over the $\sim 60\%$ trajectory Jamaica was on track for absent the storm (see the figure and the second table).

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The scale of the investment gap

Using benefit-to-cost ratios from disaster risk literature, we estimate that annual predisaster resilience investment of between US\$360 million and US\$900 million (1.8% to 4.5% of GDP) could have offset that new borrowing entirely, depending on the ratio assumed (see SM). These figures cannot say which investments would have worked best, nor capture implementation lags; still, they show that this estimated gap between the resilience investment Jamaica would have needed and what it has actually been able to invest is large and grounded in established benefit-cost-ratio research. The IMF's 2025 Article IV consultation, a health check of a nation's economy, found that Jamaica could spend only 0.2

to 0.4% of GDP per year (US\$40 million to US\$80 million) on adaptation without straining the debt path, which is 4 to 22 times below what offsetting the postdisaster borrowing would require.

This gap narrows considerably once financing structure is considered: Public financing can cover roughly one-third of total adaptation cost before returns become negative, with private capital expected to fund the remainder (7). If we apply that share to our \$360 million to \$900 million range, it implies a government-financed portion of roughly US\$120 million to \$300 million annually. This is still 1.5 to 7.5 times above what the IMF's Article IV consultation treats as fiscally sustainable, but it is a substantially smaller shortfall than the 4 to 22 times gap mentioned earlier. What Jamaica can sustainably afford under current rules falls short of what would have changed its post-Melissa trajectory, because those rules presently leave too little fiscal room for resilience spending to begin with (see SM).

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The architecture perpetuates the cycle

The loop persists because each actor responds rationally to the incentives it faces, yet the combined effect leaves both borrowing countries and their lenders worse off than a coordinated approach would. Governments prioritize debt service because creditworthiness signals carry real consequences for market access and borrowing costs. Rating agencies have limited incentives to change this unilaterally: Physical resilience metrics are not yet standardized, their links to sovereign default probabilities are underresearched, and incorporating them would require restructuring entire rating frameworks (4, 8). Reforming sovereign risk frameworks is more workable, given that agencies treat them as credible inputs.

Credit rating agencies reward what their frameworks are designed to measure. In Jamaica's case post-Melissa, activating disaster risk financing instruments, using disciplined concessional lending, and temporarily pausing its own budget rules through its fiscal escape clause (triggered once a disaster's fiscal impact exceeds 1.5% of GDP; Melissa's was \~3.9%) (see SM) were all real improvements in financial risk management. But what current frameworks do not capture is any change in the physical exposure that produced the crisis in the first place. IMF programs like the Debt Sustainability Analysis (DSA) are built to address sovereign debt distress. The August 2024 supplemental note introduced climate risks into DSA for some programs, yet implementation is still not part of the core methodology (8, 9).

Disaster risk financing instruments are real innovations beyond traditional aid mechanisms, with CCRIF designed for rapid postdisaster liquidity, but the limitation is that of scale and design fit: Instruments designed for investor liquidity are not necessarily built for national recovery. The current architecture produces a coordination failure, where every institution operates rationally within its own mandate, yet the collective outcome is chronic underinvestment in resilience for the world's most vulnerable nations, and the same conditions recur wherever debt constraints and physical risk coincide. Here, sovereign fiscal efforts alone cannot close the gap, as adaptation pays for itself only when governments cover the reactive share of adaptation spending (i.e., disaster relief and recovery), whereas the private sector funds proactive measures like resilient infrastructure and early warning systems. That government share averages about one-third of total adaptation costs across the countries (7). If governments instead fund adaptation entirely themselves, the costs outweigh the savings, and even this best-case split would not fully restore debt sustainability for a high-exposure, high-debt country like Jamaica (7).

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DISRUPTING THE DOOM LOOP

Multilayered resilience frameworks—combining fiscal buffers (reserves or prearranged credit lines that are set aside before a disaster), parametric insurance, and contingent financing like debt-pause clauses—have worked in comparable Caribbean economies $(10)$ . What is missing, however, is the institutional incentive to build these three layers. The interventions below target that gap, so that fiscal discipline and resilience investment reinforce each other instead of competing, benefiting both borrowers and lenders. All are aimed at multilateral institutions, because the IMF, multilateral development banks (MDBs), and sovereign debt markets are more open to coordinated reform (compared to rating agencies, for example) that could shift market signals at scale. Each reform below strengthens one of these layers: Embedding resilience into IMF DSAs builds the incentive structure that ties them together, scaling the RST builds fiscal buffers, recalibrating parametric triggers strengthens the insurance layer, and CRDCs build contingent financing.

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Embed physical resilience into IMF DSAs

The IMF's existing DSA framework, given its mandate for sovereign stability, relationships with all major borrowing countries, and an analytical capacity, is the most viable path to standardizing how physical resilience is measured and rewarded in sovereign risk assessment. The foundational case for integrating climate risks into stochastic DSA (9) links integrated assessment models with debt dynamics to capture how global warming affects growth, fiscal costs, and sovereign wealth. Jamaica's 2025 Article IV consultation represents a step in this direction, with a climate module projecting debt paths under higher adaptation spending (see SM), yet the analysis asked only how much adaptation the country could afford without straining its debt path. It did not, critically, model the reverse: What happens to debt sustainability when adaptation falls short, and a catastrophe follows? Jamaica's post-Melissa trajectory represents that scenario.

Climate warming may suppress growth, and slower growth erodes debt capacity $(9)$ . In addition to this “slow” channel in a DSA, an “acute” channel could see underinvestment in resilience increase the probability and fiscal severity of a disaster, requiring a complementary approach, in which predisaster investment enters the DSA as a variable that shifts the probability distribution of catastrophic-loss scenarios. As noted earlier, financing reactive adaptation can break even and lower the primary balance needed to stabilize debt $(7)$ . Cutting this spending to make room for debt service does not necessarily save money, but instead gives up a return the government would otherwise capture. This share should be protected from crowding out, and embedding it into the core DSA methodology would do it.

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Scale up RST funds

IMF's Resilience and Sustainability Trust, established in 2022 to provide concessional financing, should be more explicitly used to expand the fiscal horizons of highly indebted and climate vulnerable nations.

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Jamaica's public debt-to-GDP trajectory

The historical path shows debt declining from $\sim 144\%$ in 2013 to $\sim 65\%$ by the end of 2024. Following Hurricane Melissa, the debt ratio is projected to peak at $68.5\%$ , an 8.5 percentage point increase over the no-storm counterfactual ( $\sim 60\%$ ).

Early Caribbean pilots have been promising, like Barbados using RST resources to retire high-cost debt and divert those savings toward essential water and food security (11). The instrument is presently underscaled relative to the magnitude of the fiscal constraints, despite a strong economic case for scaling up: The fiscal cost of climate finance at scale to advanced-country donors is modest as a share of GDP, and backing climate-vulnerable economies is in the collective economic interest of financier countries beyond just development obligations (12). The IMF should scale this approach and clearly link RST disbursements to measurable increases in public capital expenditure. In Jamaica's case, this would directly address the crowding-out mechanism due to debt repayment obligations.

Scaling this approach across the roughly 35 to 40 highly indebted, climate-vulnerable small island developing states (SIDS) with active IMF relationships would require cumulative RST disbursements on the order of US\$20 billion to US\$30 billion, values that fall within current RST capacity if climate-vulnerable SIDS are explicitly prioritized (see SM). This requires targeted deployment for countries where RST's concessional terms and long maturities fit the problem, and not for the IMF to serve as the primary creditor for every climate-exposed sovereign. When combined with the fiscal buffers, parametric instruments, and contingent financing, RST-linked commitments carry less of the burden on IMF resources alone (10).

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CRDCs

CRDCs let a borrower defer principal and interest for up to 2 years after a disaster, which redirects existing capital toward emergency response without new debt. Seventy-three countries and major MDBs like the World Bank and the Inter-American Development Bank have committed to implementation (13). In April 2026, Fitch Ratings revised its Sovereign Rating Criteria to clarify that bounded, rules-based payment deferrals in well-designed pause clauses need not be considered a default, provided triggers and protections are clearly specified (14); Moody's Ratings has engaged but has not issued an equivalent revision. Bondholders, initially resistant, are increasingly viewing well-structured CRDCs as credit enhancing, because payment flexibility lowers the odds of disorderly default.

Contingent debt instruments have been proposed for decades but rarely adopted. GDP-linked bonds, the best-known attempt, had three problems: Triggers were tied to GDP figures that a government could influence, difficult pricing (see SM), and a history of issuance mainly through distressed restructurings. CRDCs address these problems: Storm triggers cannot be manipulated, and standardized development bank templates give markets a common reference that earlier instruments did not. Countries like Barbados have adopted them as a precaution, from a position of fiscal strength rather than in a crisis $13$ . CRDCs complement parametric instruments rather than replacing them: Catastrophe bonds supply liquidity when a storm meets the trigger, and a CRDC defers payments on a declared emergency regardless of storm track.

Coordination remains the main barrier, because the price itself is modest. The World Bank charges a fee of just 0.05% of the disbursed balance for its CRDC option, and the clauses' transparency and disclosure benefits can offset even that $(13)$ . The deeper challenge is how CRDCs have been used, given that most have been added during debt restructurings rather than written into new borrowing upfront, which ties the whole idea to distress and puts off the very countries that would benefit most. Had Jamaica's debt included standard CRDC provisions before Melissa, its debt service payments would have paused automatically, but the benefit only holds if the pause applies across all of a country's debt at once, which means standardizing the clause language across every source, including bilateral lenders, development banks, and private bond markets.

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Recalibrate parametric trigger design and coverage limits

Parametric instruments need recalibration on two fronts. First, trigger design should move toward multiparameter indices, making it a hazard-modeling problem as much as an insurance one: incorporating rainfall accumulation, storm surge, and wind speed, and defining triggers over smaller, more localized grid cells rather than large regional ones. This will help reduce the basis risk that left Jamaica with zero payout despite Beryl's billion-dollar damages (5). Hybrid parametric-indemnity structures, where a parametric trigger initiates immediate liquidity while a claims adjustment process determines a supplementary indemnity component (i.e., a payout based on actual verified losses), can be a direct path to closing the gap between contractual performance and actual recovery. This is important because traditional loss-verified insurance is not really available to sovereigns on its own, because insuring a whole country's losses this way requires assessors on the ground and takes months (which is exactly why parametric instruments were built in the first place). A hybrid structure would provide both speed from the parametric trigger and accuracy from the verification.

Second, coverage limits should be expanded by having MDBs back these instruments with additional risk capital or guarantees, so the risk pool itself can safely support larger payouts. This works by growing how large a loss the pool can cover, and not by changing how any individual country's premium is set. Premiums can still scale with a country's actual risk profile, even as the pool's total capacity grows. This distinction is important because if premiums stopped reflecting a country's actual exposure, there would be little reason to continue investing in the resilience measures that lower it. MDB capitalization avoids this by expanding the pool's capacity to pay out while leaving each country's premium tied to its own risk.

The cost trade-off remains a crucial point: Whereas multiparameter triggers improve actuarial efficiency, hybrid structures cost more per policy than pure parametric ones, and that added cost needs to be weighed against the borrowing it can help avoid after a disaster. For the most constrained sovereigns, concessional premium financing through climate funds like United Nations' Loss and Damage Fund can absorb it. These reforms would allow disaster risk financing to meet national recovery needs instead of focusing only on supplying market liquidity.

Jamaica's trajectory from over a decade of hard-won fiscal discipline to a sharp reversal of that progress in a matter of weeks is an urgent signal that institutional frameworks are not keeping pace with a changing climate. The institutional conditions that led to Jamaica's outcome are structural and will return wherever creditworthiness measures fiscal discipline without accounting for the physical resilience that helps sustain it. Reforming how sovereign resilience is measured, financed, and rewarded is a prerequisite for making fiscal discipline meaningful as physical risk intensifies. $\square$

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REFERENCES AND NOTES

1. S. Arslanalp, B. Eichengreen, P. B. Henry, Brookings Pap. Econ. Act. 55, 133 (2024).

2. Planning Institute of Jamaica, Assessment of the socioeconomic and environmental impact of Hurricane Melissa (damage and loss assessment prepared with UN ECLAC and the Government of Jamaica, Planning Institute of Jamaica, 2026); https://jis.gov.jm/total-loss-and-damage-from-hurricane-melissa-estimated-at-1-952-trillion/.

3. S.A. Zenios, Curr. Opin. Environ. Sustain. 67, 101414 (2024).

4. P. Klusak, M. Agarwala, M. Burke, M. Kraemer, K. Mohaddes, Manage. Sci. 69, 7468 (2023).

5. Financial Stability Institute, International Association of Insurance Supervisors, "Uncertain waters: Can parametric insurance help bridge NatCat protection gaps?" (FSI Insights on Policy Implementation No. 62, Bank for International Settlements, 2024); https://www.iais.org/uploads/2024/12/FSI-IAIS-Insights-on-parametric-insurance.pdf.

6. D. J. Clarke, S. Dercon, Dull Disasters? How Planning Ahead Will Make a Difference (Oxford Univ. Press, 2016).

7. M. Calcaterra, A. Consiglio, V. Martorana, M. Tavoni, S. A. Zenios, "Sovereigns on thinning ice: Debt sustainability, climate impacts and adaptation," Working paper 06/2025, Bruegel, 2025; https://www.bruegel.org/working-paper/sovereigns-thinning-ice-debt-sustainability-climate-impacts-and-adaptation.

8. International Monetary Fund, "Staff guidance note on the debt sustainability framework for low-income countries: Supplemental guidance on climate change" (IMF, 2024); https://www.imf.org/en/publications/policy-papers/issues/2024/08/05/supplement-to-2018-guidance-note-on-the-bank-fund-debt-sustainability-framework-for-low-553151.

9. S.A. Zenios, Clim. Change 172, 30 (2022).

10. S. Chen, S. Siegel, C. Tovar Mora, "Fiscal sustainability and natural disaster risks in the ECCU" (Selected Issues Paper 2025/068, International Monetary Fund, 2025); https://doi.org/10.5089/9798229011778.018.

11. J. Rambarran, S. J. Ahmed, “Strengthening the International Monetary Fund’s Resilience and Sustainability Trust to promote a just, global climate transition: Early evidence from Barbados and Jamaica” (Task Force Working Paper 015, Boston University Global Development Policy Center, 2025); https://www.bu.edu/gdp/files/2025/04/TF-WP-015-FIN.pdf.

12. P. Bolton, A. M. Kleinnijenhuis, J. Zettelmeyer, "The economic case for climate finance at scale" (Policy Brief 09/2024, Bruegel, 2024); https://www.bruegel.org/policy-brief/economic-case-climate-finance-scale.

13. Sustainability-linked Sovereign Debt Hub, "Climate resilient debt clauses: State of play" (SSDH, 2025); https://www.ssdh.net/climate-resilient-debt-clauses.

14. Fitch Ratings, "Sovereign Rating Criteria" (Fitch Ratings, 27 April 2026).

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ACKNOWLEDGMENTS

The authors thank K. Mackenzie and S. Evans for their expert review and feedback on the manuscript. Funding was provided by the Lizzy Warner Fellowship, Northeastern University (A.M.), and the US Department of Defense's Strategic Environmental Research and Development Program (RC20-1183 to A.R.G.). E.K. is also employed by Intercontinental Exchange Data Services but contributes here solely in his capacity as adjunct faculty at Northeastern University. The views expressed here are those of the authors alone and do not reflect the views of Intercontinental Exchange Data Services.

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.aeh3608

10.1126/science.aeh3608

$^{1}$ Sustainability and Data Sciences Laboratory, Northeastern University, Boston, MA, USA. $^{2}$ Center for Public Enterprise, Washington, DC, USA. $^{3}$ Artificial Intelligence for Climate & Sustainability, The Institute for Experiential Artificial Intelligence, Northeastern University, Boston, MA, USA. Email: mishra.aay@northeastern.edu; a.ganguly@northeastern.edu

RESEARCH

IN SCIENCE JOURNALS

Edited by

Michael Funk

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NEUROSCIENCE An epigenetic brake for motor control

Cross-talk between blood vessels and neurons supports central nervous system function. Lu et al. identified a vascular-specific mechanism that was critical for developing neurocircuitry in the motor coordination center of the brain (see also the Focus by Bonanomi). The methyltransferase PRMT5 epigenetically repressed the expression of the gene encoding the vascular remodeling factor ANGPTL4. Mice deficient in brain endothelial cell PRMT5 had high amounts of secreted ANGPTL4, which increased the inhibitory synaptic input to the cerebellum and caused progressive motor deficits. These findings broaden the role of neurovascular coupling in development. —Leslie Ferrarelli Sci. Signal. (2026) 10.1126/scisignal.aed6605; 10.1126/scisignal.aek9091

Blood vessels in the brain visualized in a magnetic resonance imaging-based reconstruction

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MOLECULAR BIOLOGY

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ncRNAs tune gene expression dynamics

Most of the genome does not encode proteins but instead produces noncoding RNAs (ncRNAs), the functions of which remain largely mysterious. Using live imaging in developing fly embryos, Batut and Levine found that these ncRNAs help to control when and how strongly protein-coding genes are turned on. For the Hox gene Scr, ncRNAs produced by a distant enhancer delay activation, whereas ncRNAs from a “tethering” element boost expression. Disrupting the enhancer RNA strengthened long-range DNA contacts, leading to premature

activation of Scr. These findings suggest that ncRNAs help to shape genome organization and long-range communication across the genome, ensuring precise timing and levels of gene expression during development.

—Di Jiang

Science p. 402, 10.1126/science.aek5696

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MACHINE LEARNING Stepwise diagnosis with AI

AI applications for clinical medicine continue to advance but often rely on written vignettes. Unfortunately, these are not a realistic representation of clinical medicine, where patients do not come in with a tidy write-up of key symptoms and pertinent laboratory findings. To address this issue, Nori et al. made their AI system start from the patient's chief complaint and decide what follow-up questions to ask and what testing to order to collect the information needed for a diagnosis. In multiple test settings, this system achieved higher accuracy than human responders and at a lower total cost, demonstrating its potential as a tool to assist physicians.—Yevgeniya Nusinovich

Science p. 423, 10.1126/science.aeh7930

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SOLID-STATE PHYSICS Elucidating the phonon

The thermal Hall effect (THE), the appearance of a transverse temperature gradient in response to a longitudinal heat current and in the presence of a perpendicular magnetic field, has been observed in many materials. Depending on whether the material is a metal or an insulator and if it exhibits magnetic ordering, THE has been variously ascribed to electrons, magnons, and, more recently, phonons. But just how phonons cause THE remains controversial. Meng et al. studied this effect in the honeycomb antiferromagnet NiPS $_{3}$ . By measuring five different samples, the researchers found that the amplitude of THE was correlated with the degree of magnetic anisotropy. Along with calculations, which indicated the presence of magnon-phonon band crossings in this material, these results are consistent with an intrinsic phonon THE that may be driven by magnon-phonon hybridization. —Jelena Stajic

Science p. 419, 10.1126/science.adt1992

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MEMBRANES

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Spinning gates to accelerate flow

Ionic species in the channels of porous membranes can be used to enhance the selectivity of a membrane, but this often comes at the expense of flow rate because of a narrowing of the channels. Zhang et al. incorporated ammonium ions into layered MXene membranes. The self-rotating ammonium functional groups endowed the otherwise-static subnanometer channels with dynamic responsiveness, which enabled rapid and selective transport.

—Marc S. Lavine

Science p. 434, 10.1126/science.aed8319

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2D MATERIALS Visualizing strongly correlated phases

Moiré superlattices in stacked van der Waals materials host a variety of phases featuring strong electronic correlations. Two groups used scanning tunneling microscopy to visualize such phases and tuned experimental conditions to induce their melting. Berger et al. focused on twisted bilayers of molybdenum diselenide, the triangular moiré superlattice of which hosts crystalline electronic states. As they varied the carrier density, the researchers observed the electronic crystal melt, which became either a uniform liquid-like state when electrons were added or a disordered state when the system was doped with holes. He et al. worked with Bernal-stacked bilayer graphene fully aligned with hexagonal boron nitride. Placing the sample in an external magnetic field reshaped the electronic energy levels, leading to the formation of strongly correlated topological

states. Direct imaging of these states revealed their intricate structure and elucidated the process of their quantum melting. —Jelena Stajic

Science p. 450, 10.1126/science.aef0940,

p. 440, 10.1126/science.aee6967

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CONSERVATION BIOLOGY Water is coming

Global warming is causing sea level to rise, inundating and shifting coastal ecosystems. Sea-level rise has already led to population declines of coastal species and even an extinction. Jiang et al. estimated the extent of projected future sea-level rise's effects on terrestrial vertebrate diversity at the global scale. They found that one-fifth to two-thirds of species will be exposed to sea-level rise in some part of their habitats, depending on the taxonomic group and projection, with especially high diversity threatened by sea-level rise in Southeast Asia. Considering refugia from sea-level rise in conservation priorities may be important for protecting species in the future. —Bianca Lopez

Science p. 408, 10.1126/science.aed5772

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NATURAL PRODUCTS Constructing nitrogen-rich compounds

The guanidine moiety is found in many plant- and microbe-derived bioactive small molecules, but installing this functional group is chemically challenging. Kolling et al. identified a group of prenyl transferases involved in the production of guanidine-containing natural products and found that they bind and activate free guanidine as a nucleophile to attack prenyl diphosphates. Crystal structures and biochemical experiments established the mechanism of this transformation. The researchers tested a number of enzymes from plant and bacteria that had similar activity, thus establishing a genetic basis for the production of an important group of natural products. —Michael A. Funk

Science p. 413, 10.1126/science.aeg1821

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IN OTHER JOURNALS

Edited by Corinne Simonti and Jesse Smith

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PLANT SENSORS

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A fitness sensor for plants

Guttation is the release of fluid through small pores on leaf margins called hydathodes, and it occurs when root pressure exceeds transpiration. Guttation provides an accessible readout of a plant's nutritional, metabolic, and stress status, but its small volume and rapid evaporation make continuous sampling difficult. Drawing on noninvasive sweat sensors for humans, Xue et al. designed a microfluidic electrochemical monitoring platform called Plantlonics. Its wedge-shaped microchannel, inspired by the pitcher plant's rim, provides a self-driven, unidirectional flow. A multichannel sensing array measures sodium, potassium, and glucose alongside on-leaf temperature and humidity. This allows noninvasive monitoring of stress-induced changes in these biomarkers over several days across multiple plant species, representing a step toward precision agriculture. —Unnati Sonawala

Nat. Commun. (2026)

10.1038/s41467-026-77955-6

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CELL BIOLOGY Understanding implantation failure

Female fertility declines sharply after 35 years of age. Cavanaugh et al. investigated age-related infertility in aged mouse models compared with in vitro fertilization (IVF) clinical datasets. Overly strong contractility in mouse embryos from older females impaired embryonic cell-fate specification and implantation. Mouse models replicated age-related defects seen in humans in relation to

pregnancy outcomes and in vitro implantation assays. A peri-implantation age-related defect involved increased surface tension, substrate adhesion, and viscosity of the embryo, which restricted spreading during implantation. Noninvasive imaging signatures predicted implantation success for mouse embryos from young and aged females. Thus, embryo mechanics can regulate reproductive longevity, providing a potential route for screening embryos to improve IVF outcomes.

—Stella M. Hurtley

Nat. Cell Biol. (2026)

10.1038/s41556-026-02052-1

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2D MATERIALS Cling to the surface

Atomically thin crystals with metallic elements, such as intermetallic compounds and high-entropy metal alloys, can exhibit distinct physical and chemical properties desirable for electronic devices. However, synthesizing two-dimensional (2D) films of these materials has been challenging because of thermodynamic instability and kinetic limitations. Zhang et al. report an adsorption-conversion method that can synthesize a wide range of high-quality intermetallic and high-entropy metal alloy thin films using metal chloride salts. Under a hydrogen environment, adsorbed metal chloride compounds were reduced on the surface, where the released metal atoms lowered the surface energy. Adsorbed chlorine atoms further suppressed vertical 3D growth. The approach produced ultrathin films a few tens of micrometers in size on practical substrates. —Sumin Jin

Nat. Mater. (2026)

10.1038/s41563-026-02752-x

PUBLIC HEALTH

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Cooled by close, curvy green spaces

Urban green space is associated with cooling and reduced heat-related illness. How that space is organized seems to matter, too, although this has not been well resolved at standard spatial resolutions. Wang et al. overlaid statewide health records for 2016 to 2023 onto 1-meter aerial imagery of more 2000 neighborhoods in Arizona. As expected, more green space was linked to reduced heat-related illness. As important, however, were green space complexity and connectedness. Their findings suggest that urban green-cooling initiatives should consider the shape and linkages of spaces as well as their extent. —Angela Hessler

GeoHealth (2026) 10.1029/2026GH001978

The benefits of urban green space, like Rymill Park in Adelaide, Australia, are correlated with its shape and connectivity.

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ACTINIDE CHEMISTRY Carbon and uranium triple up

In a Fischer carbyne, a carbon atom forms a triple bond to a metal and a single bond to an oxygen or nitrogen substituent, with some potential for electron delocalization along the axis. A variety of examples have been characterized with transition metals, and Seed et al. now extend the bonding paradigm to uranium. Specifically, reaction of a triamide uranium complex with a diazophosphorus ylide produced a dinuclear complex with the

uranium centers linked by a CNN bridge. Crystallography and spectroscopy as well as theory support a triple-bond character between the carbon and uranium. —Jake S. Yeston

Nat. Chem. (2026)

10.1038/s41557-026-02260-0

TOXICOLOGY

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Formaldehyde's impact on the brain

Formaldehyde is one of the simplest toxicants, and, if inhaled at high levels, it can cause both acute irritation and serious long-term consequences such as cancer. Associations with depression have also been claimed, but the molecular mechanism of such effects remain poorly studied. Xu and Shen tackled this question by analyzing brain activity of mice exposed to formaldehyde using cyclic voltammetry. They found that this treatment reduced stimulated release of dopamine in the nucleus accumbens. The authors propose a potential association with changes in the gut microbiome, but further mechanistic experiments will be necessary to fully understand and validate these effects. —Michael Funk

ACS Chem. Neurosci. (2026) 10.1021/acschemneuro.6c00121

PLANT BIOLOGY

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Trees straighten themselves by feel

Trees keep their trunks upright by responding to gravity and light, but it is unclear whether they can also sense and correct their own curvature. Caulus et al. investigated whether poplar trees actively straighten bent stems using a sense of their own shape, called proprioception, rather than springing back passively. By tilting young poplars and then spinning them to cancel out gravity sensing, the authors found that the trees still straightened themselves, growing a muscle-like “tension wood” that shifted from one side of the stem to the other to pull it back into shape. This may mean that trees actively monitor and correct their posture, which could help to improve wood quality and the breeding of crops more resistant to storms. —Di Jiang

New Phytol. (2026) 10.1111/nph.71238

CANCER

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STAT2 intron retention and immunotherapy

Alternative RNA splicing is a regulatory process that allows a gene to encode multiple messenger RNA (mRNA) isoforms that can produce proteins with different functions. Using long-read RNA sequencing, Englander et al. mapped alternatively spliced mRNA variants in lung adenocarcinoma, a cancer type that is only partially responsive to current therapies. Thousands of mRNA isoforms were identified in immune-related genes, and intron retention events in the Signal Transducer and Activator of Transcription 2 (STAT2) gene led to the production of altered protein isoforms that regulated immune signaling and interferon response. The molecular changes correlated with the response of lung cancer patients to anti-PD-L1 immunotherapy, suggesting that regulated intron retention in the STAT2 gene may contribute to treatment outcome. —Priscilla N. Kelly

—Priscilla N. Kelly

Science p. 397, 10.1126/science.aea7156

SOLAR CELLS

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Anchors for flexible perovskite modules

Decoupling the deposition of self-assembled monolayers (SAMs) and perovskites enables the fabrication of flexible perovskite modules (PSMs) with high power conversion efficiency (PCE). The stability and PCE of flexible devices fall short of those of their rigid devices because surface hydroxyls desorbing on flexible substrates disrupts SAM assembly. Wu et al. accelerated SAM anchoring with a passivator and reduced their interference with perovskite film formation. A 25-square-centimeter flexible device retained 92.5% of its

Edited by Michael Funk

initial PCE of 22% after 1044 hours of maximum power point tracking at 85°C and 65% relative humidity. —Phil Szuromi

Science p. 398, 10.1126/science.aef9745

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ARTIFICIAL INTELLIGENCE Tag-teaming AI agents

Conventional drug discovery is a labor-intensive and expensive process, requiring separate teams of people for different steps. The Virtual Biotech approach was designed by Zhang et al. to streamline early drug discovery, with an integrated workflow made up of teams of specialized AI agents, all directed by an agent acting as a chief scientific officer. As with any AI-driven biological research, the agents' recommendations will need to be translated into the real world by synthesizing the candidate drugs and testing them. This approach can only work for diseases for which there are enough background data for the AI to interpret, but it may help to identify therapeutic opportunities that would otherwise be missed.

—Yevgeniya Nusinovich

Science p. 399, 10.1126/science.aeg6779

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METABOLISM Goodbye to excess glucose

Diabetes and obesity are becoming increasingly common around the world, and they frequently coexist and reinforce each other. A variety of pharmacological and biological interventions are already available, but each has its advantages and disadvantages and many patients are still in need of better tolerated, more effective, and/or more affordable treatment options. An implantable device developed by Maity et al. helps to fill this gap by providing a controllable way to adjust blood glucose concentration

without medications or insulin (see the Perspective by Bentley and Payne). The wirelessly powered device can be linked to a clinically available continuous glucose monitor to catalyze the conversion of glucose to gluconate, which is then renally excreted. This normalized blood glucose and simultaneously removed some of the excess caloric load when tested in mice.

—Yevgeniya Nusinovich

Science p. 400, 10.1126/science.ady8560; see also p.382, 10.1126/science.aem0762

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CELL BIOLOGY Mitochondria dictate death mechanism

Control of programmed cell death is central to diverse processes from development to cancer therapies. A key event leading to apoptotic cell death is permeabilization of the mitochondrial outer membrane. This normally leads to release of cytochrome c and activation of caspases and the apoptosome. If this apoptotic death process is not completed, then mitochondrial DNA can leak out as well, causing caspase-independent cell death and inflammation. Yang et al. showed that release of cytochrome c and release of mitochondrial DNA are separate biochemical processes (see the Perspective by Muñoz-Pinedo and Martin). They are mediated, respectively, by complexes formed of the proteins BAK and BAX alone or by the incorporation of BAK and BAX in a larger complex with other proteins. The latter form of cell death, referred to as baciptosis by the authors, may be of particular importance in apoptosome-deficient human cancers. —L. Bryan Ray

Science p. 401, 10.1126/science.aea2181; see also p. 383, 10.1126/science.aem1247

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COMPARATIVE COGNITION Fast thinking on the wing

Bird brains were once maligned, but it is increasingly clear that, although structurally different from mammals, they provide high-level analogous cognitive functions. In terms of being able to make rapid decisions based on visual inputs, birds are under some of the strongest selection pressure given their dependence on rapid movement during flight. Schmidbauer and Neider tested decision speed in carrion crows and found that it was roughly twice as fast as that in primates (see the Perspective by Colombo and Poutrain-Sorel). Furthermore, recordings from neurons in the nidopallium caudolaterale, the functional analog of the primate prefrontal cortex, exhibited ramping choice signals similar to those seen within this region during decision-making in primates.

—Sacha Vignieri

Science p. 445, 10.1126/science.aed6459; see also p. 385, 10.1126/science.aem0341

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GLACIAL INCEPTION Anthropogenic reversal of glaciation

Has anthropogenic warming prevented the next glacial cycle? Young et al. showed that it may have done just that (see the Perspective by Marcott). They looked at the evolution of the Barnes Ice Cap on Baffin Island, Canada, the last remaining piece of the Laurentide Ice Sheet (LIS), which once covered much of North America and was the largest of the Pleistocene ice sheets. After shrinking throughout much of the early- and mid-Holocene, the LIS began to grow again around 2000 years ago but then began shrinking once more around 1960. The authors attribute

this reversal to anthropogenic greenhouse forcing, evidence that humans caused the termination of the next glaciation.

—Jesse Smith

Science p. 455, 10.1126/science.aed3379; see also p. 381, 10.1126/science.aem3295

PHYSICS

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Stranded in a metallic sea

Bound states in the continuum (BIC), localized states with energies lying within the continuous spectrum of spatially extended states, appear in systems described by a wave equation. They have been observed largely in photonic and acoustic systems because visualizing electronic BIC in metals is trickier. Thinel et al. used scanning tunneling spectroscopy to measure the local density of states of $Pd_{5}AlI_{2}$ , a van der Waals metal with a decorated checkerboard lattice. On the sites identified as palladium defects, the authors observed sharp, isolated peaks at energies inside the metallic continuum but electronically decoupled from the continuum states. Calculations suggest that these electronic BIC states stem from flat bands associated with frustrated hopping, a mechanism that is generalizable to several types of crystal lattices. —Jelena Stajic

Science p. 429, 10.1126/science.adt9825

T CELLS

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Sugarcoating the fate of γδ T cells

γδ T cells play an important role in maintaining tissue homeostasis but become dysregulated in inflammatory conditions. Santos-Pereira et al. revealed that the γδ T cell glycome plays an important role in γδ T17 cell-fate commitment, promoting a hyperactivated proinflammatory state that exacerbates immune-mediated inflammatory diseases. Analysis of human transcriptomic data and murine models revealed that the absence of β1,6 N-acetylglucosamine–branched N-glycans promoted type-3 interleukin-17A–producing γδ T cells and loss of tolerance. Loss of N-glycan branching in glycoengineered mouse models increased susceptibility to psoriasis, lupus, and inflammatory bowel disease. Supplementing γδ T cells with N-acetylglucosamine reduced disease pathology and γδ T17 cell activation, revealing the importance of glycobiology in γδ T cell behavior and strategies for disease intervention.

—Leoma Bere

Sci. Immunol. (2026)

10.1126/sciimmunol.aec9553

Intron retention regulates STAT2 function and associates with immunotherapy response in lung cancer

Full article and list of author affiliations: https://doi.org/10.1126/science.aea7156

Ryan P. Englander, Mattia Brugiolo, Maëva Devoucoux, Te-Chia Wu, Mitch Kostich, Nathan K. Leclair, Isha Walawalkar, Hyeon Gu Kang, SungHee Park, Florentina Marches, Mark E. Peeples, Phylip Chen, Jacques Banchereau, Peter Yu, Andrew Salner, Romain Banchereau, Karolina Palucka†, Olga Anczuków†\*

INTRODUCTION: Immune checkpoint blockade has transformed the treatment of lung cancer, yet most patients still fail to respond and the molecular determinants of therapy response remain incompletely understood. Alternative RNA splicing, the process by which cells generate multiple messenger RNA (mRNA) isoforms from a single gene by selectively including exons or introns, is frequently dysregulated in cancers, including lung cancer. However, its contribution to antitumor immunity and immunotherapy responses has not been well characterized.

RATIONALE: Splicing alterations in tumors often generate isoforms with altered or disrupted function relative to their canonical counterparts, potentially influencing tumor growth and therapeutic response, and yet a large fraction of these isoforms remains functionally uncharacterized. Long-read RNA sequencing, which captures full-length transcripts rather than short fragments, has substantially improved the ability to identify and functionally interpret these isoforms in health and disease. This approach has previously been applied to catalog isoforms in lung cancer cell lines, but not in primary human lung tumors.

RESULTS: We applied long-read RNA sequencing to primary human lung adenocarcinoma samples to map the alternative splicing landscape of the most common subtype of lung cancer. We identified more than 149,000 full-length mRNA isoforms, more than half of which were unannotated, with many occurring in immune-related genes. Isoforms with immune relevance were enriched for genes involved in interferon responses, a pathway central to both immune activation and suppression in tumors. Among these, we identified two retained introns in STAT2, which encodes a transcription factor required for type I interferon signaling; each of these introns was up-regulated in tumors and predicted to disrupt normal protein function. We functionally characterized both isoforms: Retention of either intron depleted full-length STAT2 protein, but retention of intron 12 specifically produced a truncated isoform that actively suppressed interferon signaling rather than merely failing to support it. This dominant-negative isoform is expressed in lung adenocarcinoma cell lines upon suppression of nonsense-mediated decay, a pathway often attenuated in tumors. Finally, we analyzed pretreatment RNA sequencing data from clinical trials in lung and urothelial cancer and found that the relative abundance of these two STAT2 intron-retention isoforms was associated with checkpoint blockade response, showing stronger retrospective association than existing biomarkers.

CONCLUSION: Alternative RNA splicing is a pervasive and functionally important layer of gene regulation, and yet its role in cancer biology remains incompletely defined. Here, we show that alternative splicing regulates the function of genes implicated in immune response in lung cancer, including in STAT2. Intron retention in STAT2 disrupts type I interferon signaling through

STAT2 intron retention disrupts interferon signaling and correlates with checkpoint blockade response. Long-read RNA sequencing of primary lung adenocarcinomas identified 149,673 full-length isoforms, more than half unannotated. Retained intron 6 depletes full-length STAT2, lowering interferon-stimulated gene (ISG) transcription, whereas retained intron 12 generates a dominant-negative isoform that actively inhibits signaling. The difference between intron 6 and intron 12 retention is associated with anti-programmed death-ligand 1 (PD-L1) response across patient cohorts. FL, full length; ISRE, interferon-stimulated response element; ri12, retained intron 12.

two distinct mechanisms: depletion of functional protein and generation of a dominant-negative isoform under conditions of nonsense-mediated decay suppression in tumors. The relative levels of these intron-retained isoforms represent a candidate biomarker associated with checkpoint blockade response, which warrants prospective validation. More broadly, the scale of unannotated isoform diversity uncovered by this approach suggests that long-read RNA sequencing of primary tumors may reveal additional functionally relevant isoforms of clinical utility beyond STAT2. These findings identify a previously unrecognized splicing-based mechanism of immunotherapy response, with potential implications for future patient stratification strategies pending further clinical evaluation.

CANCER

Intron retention regulates STAT2 function and associates with immunotherapy response in lung cancer

Ryan P. Englander $^{1,2}$ , Mattia Brugiolo $^{1}$ , Maëva Devoucoux $^{1}$ , Te-Chia Wu $^{1}$ , Mitch Kostich $^{1}$ , Nathan K. Leclair $^{1}$ , Isha Walawalkar $^{1}$ , Hyeon Gu Kang $^{1}$ , SungHee Park $^{1}$ , Florentina Marches $^{1}$ , Mark E. Peeples $^{3,4,5}$ , Phylip Chen $^{3}$ , Jacques Banchereau $^{1,6}$ , Peter Yu $^{7}$ , Andrew Salner $^{7}$ , Romain Banchereau $^{8}$ , Karolina Palucka $^{1,9\dagger}$ , Olga Anczuków $^{1,9,10\dagger*}$

Immunotherapy with checkpoint inhibitors has revolutionized cancer therapy and enabled considerable therapeutic advances for treating various diseases, including lung cancer. However, the molecular determinants of variable patient outcomes remain unclear. Using long-read RNA sequencing, we mapped the landscape of alternative RNA splicing in human primary lung adenocarcinomas. We identified more than 149,000 full-length messenger RNA (mRNA) isoforms, more than half of which were unannotated and many that occurred in immune-related genes, particularly within the type I interferon response pathway. We functionally characterized retained introns in the STAT2 gene that produced altered protein isoforms that regulated immune signaling and interferon responses and correlated with patient survival after anti-programmed death-ligand 1 (PD-L1) immunotherapy. These findings position alternative splicing as a regulator of tumor immune responses and reveal intron retention in STAT2 as an interferon regulatory axis that correlates with PD-L1 checkpoint inhibitor response.

Lung cancer is a leading cause of death globally, with lung adenocarcinoma (LUAD) being the most prevalent subtype $(1)$ . Checkpoint inhibitor immunotherapies such as anti-programmed cell death protein 1 (PD-1) antibodies have substantially improved overall survival of patients with LUAD $(2, 3)$ . These therapies promote antitumor immune responses by blocking immunosuppressive pathways that reduce the effector functions of endogenous tumor-reactive CD8 $^{+}$ T cells; however, many patients do not respond to this treatment, and existing biomarkers fail to predict responses adequately $(4)$ . A better understanding of the molecular pathways that regulate immune function in LUAD is vital for improving immunotherapy.

Alternative RNA splicing, a ubiquitous posttranscriptional process that generates multiple mRNAs from a single gene (5), may be key to a more precise understanding of immune responses in tumors. Although almost all multiexonic genes are alternatively spliced in humans, most isoforms remain uncharacterized (6, 7). Splicing is often altered in cancer to favor oncogenic and immune-evasive isoforms (8–11), but the mechanisms underlying these changes in LUAD are poorly understood.

Long-read RNA sequencing (RNA-seq) allows sequencing of full-length transcripts and thus enables deeper functional analyses than would be possible using conventional short-read RNA-seq technology $12-14$ . However, to date, long-read RNA-seq has only been applied to studies of alternative splicing in LUAD cell lines and not primary tumors $15-17$ . In primary tumors from other cancer types, long-read RNA-seq has revealed thousands of previously uncharacterized isoforms $18-21$ , highlighting its potential to uncover biologically and clinically relevant isoforms in LUAD.

Using long-read RNA-seq and a multilevel analytical platform, we mapped full-length mRNA isoforms in LUAD tumors. Many long-read-derived isoforms affected genes in immune pathways, notably interferon (IFN) signaling. IFNs, including type I (IFN-I) and type III (IFN-III), play dual roles in antitumor immunity and immune evasion $22–27$ . We identified and characterized two retained introns using long-read RNA-seq in the STAT2 gene, an essential transcription factor necessary for transducing IFN-I and IFN-III responses. These events impair IFN responsiveness, are tumor-enriched, are targetable by RNA-based methods, and retrospectively associate with patient survival after programmed death-ligand 1 (PD-L1) inhibition. Our findings underscore the utility of long-read RNA-seq to discover immune-regulatory mechanisms in cancer.

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Long-read RNA-seq reveals thousands of unannotated alternatively spliced isoforms in human lung tumors

To interrogate the alternative splicing landscape of human lung cancer, we performed paired long-read and short-read RNA-seq on RNA from 12 LUAD tumors (table S1, A to C) using PacBio single-molecule real-time (SMRT) circular consensus sequencing and Illumina sequencing, respectively (Fig. 1A). Full-length isoforms were assembled using the isoform sequencing (Iso-seq) pipeline, aligned, refined, and merged into a unified transcriptome (28, 29). Unannotated splice junctions detected by long reads were validated using paired short-read RNA-seq from the same RNA sample. We further validated transcript 5' and 3' boundaries using orthogonal datasets, including existing reference transcriptome annotations and previously mapped polyadenylation and transcription start sites (30–34). We determined empirically optimized cutoffs by varying the stringency of these parameters systematically (fig. S1A and table S1, D to H). To assess which filtering parameters were most important for isoform classification, we trained gradient-boosted machine-learning classifiers on our dataset to assess the importance of each parameter for differentiating true isoforms from artifacts (fig. S1, D to I). High-quality isoforms were further filtered for ≥5 long reads in ≥1 sample or ≥3 long reads in ≥2 samples, and isoforms were annotated using SQANTI3 structural categories (35). After stringent filtering, we identified 149,673 full-length mRNA isoforms from 18,300 loci (Fig. 1B and fig. S1B), with 51% of isoforms unannotated compared with the reference transcriptome (Fig. 1B and table S2A). Isoform quantification across tumors showed consistent structural category proportions between patients (fig. S1C and table S2B). Notably, 56% of isoforms (n = 33,267) with unannotated splice junctions [novel-in-catalog (NIC) and novel-not-in-catalog (NNC) categories] were found in ≥50% of patients, suggesting that some unannotated long-read-derived isoforms are recurrent components of LUAD transcriptomes (Fig. 1C and table S2B). Additionally, isoforms across structural categories exhibited shorter 3' untranslated regions (UTRs) than the closest matching reference (fig. S1, J to K, and table S3A). This result is consistent with 3' UTR shortening previously described in cancer (36) but may also reflect a contribution from 3' truncated artifacts arising from degraded mRNA. Of the isoforms, 2% (2940) arose from intergenic regions, with 39% of these being multiexonic (fig. S1M), potentially representing unannotated or reexpressed genes.

We predicted isoform protein-coding sequences for long-read-derived isoforms and compared them with human reference proteins from UniProtKB/Swiss-Prot (37). Most reference-matching isoforms

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Fig. 1. Long-read RNA-seq detects unannotated alternatively spliced isoforms in LUAD primary tumors that are enriched in genes associated with IFN response. (A) Pipeline for the discovery of full-length spliced mRNA isoforms in human primary LUAD tumors ( $n = 12$ patients). RNA from each tumor was sequenced with long-read (LR) RNA-seq to identify unannotated isoforms, which underwent extensive quality control and filtering, including short-read (SR) RNA-seq data from the same sample to validate unannotated spliced junctions, known polyA sites, and known transcription start sites. Isoforms with $\geq 5$ reads in $\geq 1$ sample or $\geq 3$ reads in $\geq 2$ samples were retained. See Materials and methods for filtering details. Full-length isoforms were annotated using SQANTI3 isoform structural categories: FSM, RM, ISM, NIC, and NNC. ORFs were predicted and annotated per isoform. (B) Long-read-derived full-length mRNA isoforms detected in LUAD were classified using SQANTI3 isoform structural categories. (C) Number of patient samples positive for each isoform as quantified by FLAIR, shown by SQANTI3 isoform structural category. (D) The impact of long-read-derived full-length mRNA isoforms on protein-coding potential was predicted by comparing the in silico translated mRNA sequence to the reference protein sequence from UniProt and is shown for "Known" and "Unannotated" isoforms. See Materials and methods for more details. (E) Pathway enrichment analysis of genes with more unannotated than known isoforms using immune-related Hallmark gene sets from MSigDB. See table S4A for gene names and isoform numbers (significance was assessed using a one-sided hypergeometric test; $^{*}P < 0.05$ , and ns is not significant). (F) The impact of long-read-derived mRNA isoforms on protein-coding potential was predicted for unannotated long-read-derived

isoforms affecting genes associated with IFN- $\alpha$ and IFN- $\gamma$ response pathways (n = 1079) versus all unannotated long-read-derived isoforms (n = 52,010) (significance was assessed using the hypergeometric test; $*P < 0.05$ , $P < 0.01$ , $*P < 0.001$ , and ns is not significant). (G) Intron retention events are quantified as PSI using short-read RNA-seq data from TCGA-LUAD tumor (n = 437 patients) and normal lung (n = 46 patients) samples. Intron retention events are filtered for those supported by long-read RNA-seq and skipped in the canonical reference isoform, ranked by FDR and the difference in median PSI between tumor and normal lung samples (median PSI is indicated by a bar, and FDR-corrected values are from rMATS; $***P < 0.001$ ). (H) Full-length spliced mRNA isoforms of STAT2 detected by long-read RNA-seq in LUAD tumor samples, grouped by intron retained (middle) and intron skipped (bottom) isoforms. The full gene structure is shown on top, with the retained introns 6 and 12 highlighted. SQANTI3 structural categories are listed next to each isoform. (I and J) Intron 6 (I) and 12 (J) retention was assessed by RT-PCR with primers located in flanking exons in LUAD tumors (n = 10 patients) used for long-read RNA-seq (left) and normal bronchial epithelial cells (NLE; n = 9 patients) from healthy donors (middle) and quantified as PSI (right; boxplots show median and interquartile range with whiskers extending to 1.5× interquartile; significance was assessed using Student's t test).

had exact protein matches [79% reference match (RM), 75% full-splice match (FSM)], whereas novel structural categories [incomplete-splice match (ISM), NIC, and NNC] frequently encoded divergent proteins (fig. S1L and table S3B). Thus, a substantial proportion of the protein-coding transcriptome in LUAD remains uncharacterized.

To determine how unannotated long-read-derived isoforms might contribute to the LUAD proteome, we classified the predicted open reading frames (ORFs) of isoforms from known genes as either known, unannotated, or truncated relative to the reference (table S3C). We further classified isoforms predicted to encode truncated ORFs into those with or without intron retention events, which often lead to ORF truncation by shifting the reading frame or introducing in-frame premature termination codons (PTCs) $(38)$ . Introns in long-read-derived isoforms were enriched in the terminal 10% of isoforms and were otherwise evenly distributed across gene bodies (fig. S1N). Notably, out of the 52,010 unannotated long-read-derived isoforms with ORF predictions, 35% were predicted to encode truncated proteins, 34% unannotated proteins, and 31% known ORFs (Fig. 1D and table S3C). These data show that unannotated long-read-derived isoforms that may encode uncharacterized and truncated proteins are frequently detected in LUAD.

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Unannotated isoforms are enriched in IFN-related genes

Despite their ubiquity, most alternatively spliced isoforms are functionally uncharacterized $(39)$ . We chose to focus on the role of unannotated long-read-derived isoforms in immune-related pathways, which are critical for tumor immunity and the target of immunemodulating therapies $(40-42)$ . Intriguingly, pathway analysis of genes enriched in unannotated isoforms revealed significant enrichment in IFN- $\alpha$ and IFN- $\gamma$ responses (Fig. 1E). We found unannotated long-read-derived isoforms in 169 of 217 IFN-related genes, including STAT1, STAT2, and HLA-A (table S4B), with 27% $(n = 288)$ of unannotated long-read-derived isoforms in IFN-related genes predicted to encode truncated ORFs owing to intron retention, which is higher than the overall unannotated long-read-derived isoform average (Fig. 1F). Using short-read RNA-seq data from the same tumor samples $(n = 12)$ , we found that $\geq 90\%$ of unannotated long-read-derived isoforms were detected by short-read-based expression quantification of full-length isoforms, providing orthogonal cross-platform validation of these IFN-related unannotated isoforms across all coding categories (fig. S2A). Because intron retention can reduce protein expression by PTC introduction or inhibition of mRNA export, these results suggest that unannotated isoforms containing retained introns may disrupt IFN signaling in LUAD.

To further explore tumor-up-regulated retained introns in IFN-related genes in a larger patient cohort, we quantified splicing using short-read RNA-seq from tumor $n = 437$ and normal lung $n = 46$ samples from The Cancer Genome Altas Lung Adenocarcinoma (TCGA-LUAD) database (fig. S2B). We found 3038 differentially spliced events where the percent spliced-in (PSI) values significantly differed between tumor and normal samples $\left|\left|\Delta\mathrm{PSI}\right| > 5\%\right|$ , false discovery rate (FDR) < 0.05] across 1656 genes, including 69 events in 32 IFN-related genes (fig. S2, C and D, and table S4C). Differential splicing events included comparable overall proportions of intron retention across all genes and IFN-related genes (fig. S2, C and D), suggesting that intron retention is not specific to IFN genes in LUAD. Filtering for intron retention identified 10 long-read–validated events in seven IFN-related genes (table S4D). These intron retention events include (i) two events in STAT2, the essential IFN-I and IFN-III transcription factor (43, 44); (ii) three events in UBA7, an enzyme that covalently modifies other proteins with the polypeptide ISG15 to promote IFN responses and tumor immunity (45); and (iii) events in DHX58, OAS1, and MOV10, all of which encode antiviral effectors with complex roles in tumor immunity (46–48) (Fig. 1G and table S4, C and D). To further validate that these events are not being detected because of differential group sizes, we confirmed that all events except for retained intron 5 of OAS1 were robust to repeat subsampling of our LUAD samples (table S4E).

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STAT2 isoforms with retained introns are expressed in tumor cells

We focused on unraveling the function and regulation of intron retention in STAT2, as retained introns 6 (ri6) and 12 (ri12) were among the most up-regulated IFN-related events in TCGA, and STAT2 is an essential, nonredundant mediator of IFN-I and IFN-III signaling (27, 43). Long-read RNA-seq identified 22 STAT2 isoforms, of which 15 were unannotated, including 12 retaining ri6, ri12, or both (Fig. 1H). All long-read-derived ri6 and/or ri12 isoforms in LUAD tumors were structurally distinct from reference transcriptome annotations (fig. S2E and table S4F).

As an orthogonal validation, we quantified STAT2 intron 6 and intron 12 retention by reverse transcription polymerase chain reaction (RT-PCR) with primers that amplify both intron-containing and fully spliced transcripts in the primary LUAD tumors analyzed by long-read RNA-seq. As a normal reference, we used primary bronchial epithelial cells from healthy donors cultured at the air-liquid interface, a system that recapitulates bronchoalveolar epithelia, including alveolar cells thought to give rise to LUAD (49–51) (Fig. 1, I and J). Consistent with the TCGA data, both introns were retained at significantly higher levels in tumors compared with normal bronchial epithelial cells (medianPSI $_{ri6}$ = 32% tumors versus 15% normal; medianPSI $_{ri12}$ = 25% tumors versus 15% normal) (Fig. 1, I and J). RNA fluorescence in situ hybridization (FISH) on LUAD tumor sections confirmed STAT2 ri6 and STAT2 ri12 signals in KRT8 $^{+}$ tumor cells (fig. S2, F and G), indicating that tumor cells themselves express retained-intron STAT2 isoforms. Consistently, both introns were detectable by RT-PCR in six LUAD cancer cell lines (fig. S2, H and I), although at lower levels (medianPSI $_{ri6}$ = 15%; medianPSI $_{ri12}$ = 12%) than in primary tumors, possibly reflecting differences in baseline intron retention levels between cells in culture and primary tumors. These data indicate that STAT2 ri6 and ri12 are up-regulated in tumors compared with normal lung and are expressed within tumor cells, while not excluding their expression in other cell types.

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STAT2 intron retention regulates STAT2 protein expression and IFN signaling

To assess how STAT2 intron retention affects IFN signaling, we designed splice-switching antisense oligonucleotides (ASOs) targeting the splice sites of STAT2 ri6 (ri6-ASO1) or ri12 (ri12-ASO1 and ri12-ASO2) as molecular tools to promote intron retention (Fig. 2, A and B). In A549 lung cancer cells, these ASOs increased retention of either ri6, ri12, or both, with largely consistent effects at baseline and after IFN-I stimulation (Fig. 2, C to H). The ri6-targeting ASO increased intron 12 retention without a significant effect on intron 6 retention, leading to a >10-fold decrease in STAT2 protein expression (Fig. 2, C, E, and G). Both ri12-targeting

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Fig. 2. ASOs targeting STAT2 retained introns permit dynamic modulation of STAT2 protein expression and IFN response. (A and B) Schematic representation of the position of ASOs targeting the STAT2 splice sites of introns 6 (A) and 12 (B). (C to F) Endogenous STAT2 intron 6 [(C) and (D)] or intron 12 [(E) and (F)] retention in A549 cells transfected with ASOs targeting intron 6 [(C) and (E)] or intron 12 [(D) and (F)], or nontargeting control (NTC), and treated with 100 U/ml IFN-I for 0, 6, or 24 hours before collection, was assessed by semiquantitative RT-PCR with primers that amplify both the skipped and retained-intron isoforms. Representative images along with PSI quantification are shown ( $n = 3$ independent biological replicates; data are mean ± SD; significance was assessed using Student's t test; \*P < 0.05, \*\*P < 0.01, \*\*\*P < 0.001, and ns is not significant; all tests are relative to NTC-ASO for the same IFN-I time point). (G and H) Endogenous STAT2 protein expression in A549 cells transfected with ASOs targeting intron 6 (G) or intron 12 (H), or nontargeting control (NTC), and treated with 100 U/ml IFN-I for 0, 6, or 24 hours before collection was quantified with Western blot with an anti-STAT2 antibody and GAPDH as loading control. Representative images along with quantification normalized to NTC-ASO for the same IFN-I time point are shown ( $n = 3$ independent biological replicates; data are mean ± SD; significance was assessed using Student's t test; \*\*P < 0.01, and \*\*\*P < 0.001). (I and J) Expression of ISGs in A549 cells transfected with ASOs targeting intron 6 (I) or intron 12 (J), or nontargeting control (NTC), and treated with 100 U/ml IFN-I for 6 or 24 hours was quantified by quantitative real-time PCR. Expression is normalized to NTC-ASO for the same IFN-I time point ( $n = 3$ independent biological replicates). FC, fold change.

ASOs increased intron 6 retention under all conditions and increased intron 12 retention with IFN-I, depleting full-length STAT2 by up to \~100-fold (Fig. 2, D, F, and H). Extended RT-PCR with primers flanking introns 6 and 12 confirmed that these effects reflect bona fide intron retention changes rather than exon skipping (fig. S3, A to E) and additionally revealed an isoform retaining both introns 12 and 13, which was also detected in LUAD primary tumors by long reads (Fig. 1H and fig. S3, D and E). ASO effects on intron retention and protein expression were largely consistent across three additional LUAD cell lines (fig. S4, A to C). Computational mapping of known RNA-binding protein (RBP) binding motifs from in vitro and in cellulose binding studies (52) revealed overlaps between ASO target sequences and predicted binding sites for heterogeneous nuclear ribonucleoprotein (hnRNP), serine/arginine-rich (SR), and RNA-binding motif (RBM) protein families (fig. S3, F and G), suggesting that ASO-mediated steric inhibition of regulatory RBP binding contributes to the increase in intron retention. We note, however, that the RBP binding patterns observed at ASO-targeted splice sites are not fully recapitulated by existing computational prediction models, underscoring the known limitations of such tools in capturing the complexity of cotranscriptional RBP dynamics. Finally, we investigated how ASO treatment affects IFN-I signaling using the expression of known IFN-stimulated genes (ISGs) MX1 and RSAD2 as a readout of IFN-I activity. All ASOs promoting intron retention suppressed ISG induction after IFN-I stimulation (Fig. 2, I and J). Together, these results demonstrate that STAT2 splice-switching ASOs can increase intron retention, thereby reducing full-length STAT2 expression and IFN-I activity.

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STAT2 retained-intron isoforms can produce truncated proteins when nonsense-mediated decay is inefficient

Although intron retention frequently introduces PTCs that trigger nonsense-mediated decay (NMD), some PTC-containing mRNAs evade degradation and generate truncated proteins $53, 54$ . Because NMD is often less efficient in tumors than in normal tissues, including in LUAD $55–57$ , we reasoned that tumors with reduced NMD efficiency may express higher levels of truncated STAT2-ri6 or STAT2-ri12 proteins.

To test this, we first scored NMD efficiency in 437 TCGA-LUAD samples by quantifying the inclusion of 12 well-established and experimentally validated NMD-sensitive exons (58–60), where a lower score indicates lower NMD efficiency (fig. S5A). This approach was validated against published RNA-seq data from short interfering RNA-mediated silencing of the essential NMD factor UPF1 (61), in which NMD-deficient cells showed significantly reduced NMD scores (fig. S5B). Tumors with lower NMD scores displayed higher STAT2 ri6 and ri12 retention (fig. S5, C and D, and table S5F), suggesting that intertumoral variation in NMD efficiency contributes to differential STAT2 intron retention. Notably, tumors had lower NMD scores than A549 cells, suggesting higher NMD efficiency in cell lines than in LUAD tumors in vivo. This difference was not attributable to tumor purity, as NMD score did not correlate with purity in TCGA-LUAD (62) (fig. S5, E and F).

To directly test whether truncated STAT2 proteins are expressed endogenously, we inserted a 3xFLAG tag into the 5' region of the endogenous STAT2 locus in A549 and H1975 cells by CRISPR (Fig. 3A), which we confirmed by detection of full-length FLAG-STAT2 with both FLAG and C-terminal STAT2 antibodies (fig. S5G). In both cell lines, endogenous truncated FLAG-STAT2 proteins were detected at molecular weights matching those of cDNA-expressed STAT2-ri6 (\~30 kDa) and STAT2-ri12 (\~50 kDa) controls (Fig. 3, B and C). Treatment with SMGIi, a selective inhibitor of the NMD-essential kinase SMG1 (63), increased STAT2-ri12 protein \~2- to 3-fold alongside elevated ri12- and ri6-containing transcripts (Fig. 3, B and C, and fig. S5, H and I), confirming that NMD actively limits truncated STAT2 protein accumulation.

Finally, we examined truncated-protein isoform expression upon forced intron retention using STAT2 splice-switching ASOs under conditions of NMD inhibition. We treated endogenously tagged cells with the intron retention—boosting ri6-ASO1 or ri12-ASO1 combined with

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Fig. 3. STAT2 retained intron 6– and intron 12–containing isoforms can produce truncated proteins regulated by NMD. (A) Strategy for CRISPR-mediated FLAG epitope tagging of endogenous STAT2. Cells were nucleofected with STAT2 start codon–targeting sgRNA, Cas9 ribonucleoproteins, and donor oligonucleotide encoding the FLAG tag. Single-cell clones were expanded and genotyped, and FLAG-STAT2 protein was characterized by Western blot. (B and C) FLAG-tagged STAT2 protein isoforms in endogenous FLAG-STAT2 A549 (B) or H1975 (C) cells treated with SMG1i (500 ng/ml for 24 hours) or DMSO as negative control were detected by Western blot with anti-FLAG antibody. Transiently transfected FLAG-STAT2-cDNA with ri6 or ri12 were used as molecular weight controls. Representative images are shown along with quantification of STAT2-ri6 and STAT2-ri12 with GAPDH as loading control, normalized to DMSO for each clone (n = 3 independent biological replicates; data are mean ± SD; significance was assessed using Student's t test; \*P < 0.05 and, ns is not significant). (D and E) FLAG-tagged STAT2 protein isoforms in endogenously tagged FLAG-STAT2 A549 (D) and H1975 (E) clones transfected with STAT2 intron 6– or intron 12–targeting ASOs (ri6-ASO1 and ri12-ASO1) or nontargeting control (NTC) and treated with SMG1i (500 ng/ml for 24 hours) or DMSO as negative control were detected by Western blot with anti-FLAG antibody. Representative images are shown along with quantification of STAT2-ri6 and STAT2-ri12 with GAPDH as loading control, normalized to DMSO for each ASO (n = 3 independent biological replicates; data are mean ± SD; significance was assessed using Student's t test; \*P < 0.05, \*\*P < 0.01, and ns is not significant; all tests are relative to DMSO for the same ASO transfection).

NMD inhibition. ri6-ASO1 with SMG1i increased FLAG-STAT2-ri6 protein levels by \~3- to 5-fold, consistent with its increased ri6 retention at the RNA level (PSI $_{ri6}$ = 50 to 80% versus \~20% in control) (Fig. 3, D and E, and fig. S5, J and K). ri12-ASO1 with SMG1i increased FLAG-STAT2-ri12 protein levels by \~5- to 6-fold and FLAG-STAT2-ri6 by \~3-fold (Fig. 3, D and E). Cell line-specific differences in ri6 retention upon ri12-ASO1 treatment and NMD inhibition likely reflect competition among multiple NMD-sensitive STAT2 isoforms, with STAT2-ri12–encoding isoforms increasing preferentially under these conditions. Notably, whereas full-length STAT2 (STAT2-FL) remained the most abundant isoform across conditions, combined ri12-ASO1 and SMG1i brought STAT2-ri6 and STAT2-ri12 to approximately equal abundance as STAT2-FL in A549 cells (fig. S5L), demonstrating that high intron retention alongside inefficient NMD can substantially shift the balance of STAT2 protein isoforms. Taken together, these results demonstrate that truncated STAT2-ri6 and STAT2-ri12 proteins are produced from the endogenous locus, are actively suppressed by NMD, and accumulate when NMD is inhibited or intron retention is elevated.

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STAT2-ri12 inhibits the IFN-I response

Having established that STAT2 intron retention produces truncated STAT2 proteins, we investigated their functional consequences. AlphaFold 3 structural predictions revealed that the STAT2-ri6 coiled-coil domain (CCD) is disrupted by a PTC that replaces the native C-terminal CCD sequence with 20 amino acids encoded by intron 6, predicted to extend outward as a naked $\alpha$ helix that may impair protein-protein interactions (Fig. 4A and fig. S6A). By contrast, STAT2-ri12 undergoes a clean truncation at glycine-372 with no distinctive amino acids, leaving its N-terminal domain (NTD) and CCD structurally intact and potentially preserving canonical interaction surfaces (Fig. 4A and fig. S6A). Both truncated isoforms lack the Src homology 2 (SH2) and transcriptional activation (TAD) domains required for transcriptional up-regulation of STAT2 targets in response to IFN (Fig. 4A). To confirm that neither isoform can transduce IFN responses, we reexpressed FLAG-tagged STAT2-FL, STAT2-ri6, STAT2-ri12, or empty vector (EV) in two independent $\mathrm{STAT2}^{\mathrm{KO}}$ A549 clones in which endogenous STAT2 has been inactivated with CRISPR (fig. S6, B to F). Only STAT2-FL rescued IFN-I-stimulated MX1 and RSAD2 expression, confirming that neither truncated isoform can transduce IFN-I responses (fig. S6G).

We next asked whether truncated isoforms affect IFN-I signaling in cells also expressing full-length STAT2 using doxycycline (DOX)-inducible A549 lines expressing FLAG-tagged STAT2-ri6, STAT2-ri12, or STAT2-FL cDNAs that are truncated after their respective stop codons (Fig. 4, B and C). Upon IFN-I stimulation, STAT2-ri12 expression reduced ISG expression at all IFN-I doses tested, whereas STAT2-ri6 had no effect and STAT2-FL increased ISG expression as expected (Fig. 4D). To define the mechanism, we performed coimmunoprecipitation assays assessing interactions with IRF9 and STAT1, the partners that together with STAT2 form the ISGF3

transcription factor–mediating IFN-I responses (64). STAT2-ri12 retained IRF9 binding but failed to associate with STAT1, consistent with loss of the SH2 domain required for STAT1:STAT2 interaction (64). STAT2-ri6 interacted with neither partner, consistent with its disrupted CCD, which is required for IRF9 binding (65). STAT2-FL interacted with both partners as expected (Fig. 4, A and E). Both truncated isoforms localized predominantly to the cytoplasm regardless of IFN-I stimulation (fig. S7A), suggesting that these interactions occur in the cytosol. Because IRF9 binding and nuclear translocation are required for productive STAT2 signaling (66), STAT2-ri12 likely acts as a dominant-negative inhibitor by sequestering IRF9 and preventing ISGF3 assembly.

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Fig. 4. STAT2 retained intron 6– and intron 12–containing isoforms encode proteins that fail to respond to IFN-I and differ in their inhibitory capacity. (A) Protein structures of STAT2-FL, STAT2-ri6, and STAT2-ri12 protein isoforms predicted by AlphaFold 3. Amino acid residues are colored by protein domain. DBD, DNA binding domain. (B) Strategy for generating DOX-inducible truncated STAT2 protein isoform–expressing A549 lines. Parental A549 cells expressing wild-type STAT2 were infected with lentivirus constructs encoding STAT2-FL, STAT2-ri6.TR, or STAT2-ri12.TR. DOX binding activates the reverse tetracycline-controlled transactivator (rtTA) leading to activation of the tetracycline-responsive element (TRE) synthetic promoter that drives STAT2 isoform expression. iSTAT2-ri6.TR and iSTAT2-ri12.TR are truncated after their respective PTC. (C) Expression of FLAG-STAT2 protein isoforms in A549 cells harboring DOX-inducible STAT2-FL, STAT2-ri6.TR, or STAT2-ri12.TR treated with DOX or DMSO for 48 hours was assessed by Western blot with anti-FLAG antibody, with GAPDH as loading control. Representative images are shown, and the expected positions of STAT2-FL, STAT2-ri6, and STAT2-ri12 are indicated. FL, full length. (D) Expression of ISGs at 6 hours after IFN-I stimulation was assessed by quantitative real-time PCR in A549 cells expressing DOX-inducible empty vector, STAT2-FL, STAT2-ri6.TR, or STAT2-ri12.TR treated with DOX or DMSO for 48 hours, expressed as fold change to the respective DMSO control (n = 3 independent biological replicates; data are mean ± SD; significance was assessed using Student's t test; \*P < 0.05, \*\*P < 0.01, \*\*\*P < 0.001, and ns is not significant). (E) Interaction between STAT2 and STAT1 or IRF9 is assessed in A549 cells harboring DOX-inducible FLAG-tagged STAT2-FL, STAT2-ri12, or STAT2-ri6 treated with DOX for 48 hours to induce expression, followed by 1000 U/ml IFN-I stimulation for 1.5 hours before lysis. FLAG-tagged proteins were immunoprecipitated (IP) using anti-FLAG antibody, eluted with FLAG peptide, and analyzed by Western blot with the indicated antibodies.

These data reveal a functionally important asymmetry between the two isoforms. STAT2-ri12 actively suppresses IFN-I signaling, whereas STAT2-ri6 is functionally inert, neither transducing nor inhibiting the response. This asymmetry has an important implication: Because ri6 lies upstream of ri12, isoforms retaining both introns will encode the STAT2-ri6 protein rather than STAT2-ri12, as the ri6 PTC terminates translation before the ri12-encoded sequence is reached.

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STAT2 retained introns associate with response to PD-L1 inhibition

IFN signaling plays a complex role in cancer immunotherapy: Although essential for leukocyte activation, differentiation, and tumor rejection (27, 67), chronic IFN signaling can drive immunosuppression and contribute to treatment failure (23, 25, 26). To assess how STAT2 intron retention interacts with this dual function, we examined STAT2 intron retention in nonsquamous non-small cell lung cancer patients from the OAK clinical trial, which compared the PD-L1 inhibitor atezolizumab to docetaxel chemotherapy (2, 68). We mapped OAK short-read RNA-seq data to our long-read-enriched LUAD transcriptome and quantified splicing events using rMATS (Fig. 5A and table S5A). We performed multivariate Cox proportional hazards analysis on atezolizumab-treated patients with complete metadata to assess the association of overall survival with STAT2 ri6 and ri12 retention, overall STAT2 expression, intratumoral PD-L1 expression by immunohistochemistry (IHC), and tumor mutational burden (TMB). Cox proportional hazards models estimate the independent effect on survival of each variable measured while controlling for the other variables included in the model. For continuous variables, the hazard ratio (HR) indicates the independent effect of increasing each variable by one increment on the risk of death. For discrete variables, the HR indicates the independent effect of that variable on the risk of death compared with baseline. STAT2 ri12 retention predicted improved survival in atezolizumab-treated patients (HR for death: 0.5, P = 0.005), whereas STAT2 ri6 predicted worsened survival (HR for death: 2.02, P = 0.002), independently of TMB, PD-L1 IHC, and STAT2 expression (fig. S8A). High TMB predicted improved survival (HR for death: 0.47, P = 0.035), which was expected, as TMB is a US Food and Drug Administration (FDA)-approved immunotherapy biomarker. By contrast, PD-L1 staining did not predict overall survival (P = 0.811), consistent with published OAK data (2) (fig. S8A). These associations persisted after adjusting for age, sex, smoking, and transcriptomic markers of IFN signaling IFNG.GS and ISG.RS (69) (fig. S8B).

The opposing effects of ri6 and ri12 prompted us to examine their difference as a composite biomarker. We found that $PSI_{ri12-ri6}$ —the difference between ri12 and ri6 retention—strongly predicted improved survival after PD-L1 blockade (HR for death: 0.48, P = 0.0008) (fig. S8C), an effect that was absent in docetaxel-treated patients, indicating an immune-specific association. We dichotomized patients at a cutoff optimized in biomarker-negative patients ( $PSI_{ri12-ri6} \geq 5\%$ ; see Materials and methods) and found that High- $PSI_{ri12-ri6}$ patients had markedly improved survival compared with Low- $PSI_{ri12-ri6}$ patients, with a stronger effect than High-TMB (Fig. 5, B and C). Notably, only High- $PSI_{ri12-ri6}$ patients derived a survival benefit from atezolizumab over docetaxel (HR for death: 0.49, P = 0.001), with no such benefit observed in Low- $PSI_{ri12-ri6}$ patients (Fig. 5D). Patients with High- $PSI_{ri12-ri6}$ had minimal overlap with High-TMB and PD-L1 positivity (Fig. 5E and fig. S8E). Incorporating $PSI_{ri12-ri6}$ alongside TMB nearly doubled the number of biomarker-positive responders from 9 to 16 (Fig. 5F), positioning $PSI_{ri12-ri6}$ as a possible independent and complementary immunotherapy biomarker pending prospective confirmation.

In total, 304 genes were differentially expressed between High-PSI $_{ri12-ri6}$ and Low-PSI $_{ri12-ri6}$ patients in OAK (table S5B). Gene set enrichment analysis revealed depletion of IFN- $\alpha$ and IFN- $\gamma$ signaling in High-PSI $_{ri12-ri6}$ tumors (Fig. 5G, fig. S8, G and I, and table S5C), suggesting that High-PSI $_{ri12-ri6}$ tumors may have reduced chronic interferon signaling that facilitates responses to PD-L1 inhibition. This result was reproduced in TCGA (fig. S8, H, J, and K and table S5, D and E), showing that the inverse association between PSI $_{ri12-ri6}$ and IFN signaling is reproducible across cohorts. Consistent with a possible role for STAT2-ri12 protein in suppressing IFN-I, High-PSI $_{ri12-ri6}$ patients had a lower NMD score than Low-PSI $_{ri12-ri6}$ patients in both OAK and TCGA (Fig. 5H, fig. S8F, and table S5, F and G), which suggests that their tumors may more efficiently produce STAT2-ri12 protein. Notably, NMD score did not independently predict survival (fig. S8D), indicating that $PSI_{ri12-ri6}$ captures biology beyond NMD efficiency.

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Fig. 5. STAT2 retained introns associate with response to atezolizumab in a phase 3 clinical trial. (A) RNA-seq data from pretreatment nonsquamous non-small cell lung cancer tumors ( $n = 503$ patients) from the OAK open label phase 3 clinical trial were used to quantify alternative splicing events using rMATS, focusing on STAT2 retained- intron events and their relationship to overall survival in patients treated with PD-L1 inhibitor atezolizumab or chemotherapy docetaxel. CA, cassette exon; IR, intron retention; A5SS, alternative $5'$ splice site; A3SS, alternative $3'$ splice site; MXE, mutually exclusive exon. (B and C) Kaplan-Meier plots of overall survival against patients with High-PSI $_{ri12-ri6}$ ( $\geq 5\%$ ; $n = 43$ patients) versus Low-PSI $_{ri12-ri6}$ ( $< 5\%$ ; $n = 212$ patients) (B) or High-TMB ( $\geq 16$ mutations/Mb; $n = 37$ patients) versus Low-TMB ( $< 16$ mutations/Mb; $n = 113$ patients) (C) in OAK patients from the atezolizumab treatment arm. Significance was assessed using the log-rank test. An optimal dichotomized cutoff for PSI $_{ri12-ri6}$ was derived using the function surv\_cutpoint from the R package survminer (see Materials and methods). (D) Cox proportional hazards analysis of overall survival among nonsquamous non-small cell lung cancer patients from OAK in the atezolizumab treatment arm who are High-PSI $_{ri12-ri6}$ ( $n = 43$ patients) or Low-PSI $_{ri12-ri6}$ ( $n = 212$ patients) compared with patients treated with docetaxel ( $n = 248$ patients). Data indicate HR $\pm 95\%$ confidence interval (CI), reflecting the relative rate of death in each group compared with docetaxel-treated patients. Significance was assessed using the Wald test. (E) Overlap of High-PSI $_{ri12-ri6}$ ( $\geq 5\%$ ) and High-TMB ( $\geq 16$ mutations/Mb) patients in the atezolizumab treatment arm of OAK. (F) Atezolizumab responders who achieved a complete or partial response per

Finally, to assess cross-tumor applicability, we computed STAT2 intron retention and $PSI_{ri12-ri6}$ from pretreatment short-read RNA-seq data from IMvigor210, a single-arm phase 2 trial of atezolizumab in metastatic urothelial carcinoma (70). $PSI_{ri12-ri6}$ again correlated with improved survival after atezolizumab treatment, both as a singular variable and as a covariate, with High- $PSI_{ri12-ri6}$ patients showing significantly better outcomes at an independently optimized cutoff (fig. S8, L and M, and table S5, H and I).

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Discussion

Here, we used long-read RNA-seq, which is capable of resolving full-length isoform structures that short-read sequencing cannot distinguish, to comprehensively profile alternatively spliced isoforms in LUAD, revealing more than 149,000 mRNA isoforms, including in genes implicated in IFN responses. Focusing on STAT2, we show that retained introns 6 and 12 impair full-length STAT2 expression, can encode dominant-negative truncated proteins, and may predict patient responses to immunotherapy. These findings may open new avenues for therapeutic targeting of RNA splicing in LUAD.

Existing immunotherapy biomarkers are imperfect (4, 71, 72), and there is a pressing need for more and better tools to guide treatment decisions. We show that patients with higher STAT2 ri12 inclusion relative to ri6 (High-PSI $_{ri12-ri6}$ ) have significantly improved survival after atezolizumab treatment, an association observed in two independent clinical cohorts across distinct tumor types. Although splicing signatures have prognostic value in LUAD (73), to our knowledge, this is the first study to link specific alternative splicing events directly to immunotherapy outcomes. PSI $_{ri12-ri6}$ identifies a patient subset with minimal overlap with TMB or PD-L1 IHC, and incorporating it alongside TMB nearly doubles the number of biomarker-positive responders. This positions PSI $_{ri12-ri6}$ as a potentially clinically actionable transcriptomic biomarker capable of capturing immunotherapy benefits that existing tools miss, warranting prospective validation in future studies. The mechanistic basis for this association may relate to the ability of STAT2-ri12, but not STAT2-ri6, to act as a dominant-negative inhibitor of IFN-I signaling: Given that chronic IFN-I impairs immunotherapy efficacy (25, 26, 69), tumors expressing STAT2-ri12 may be better primed to respond to anti-PD-L1 immunotherapy. Because ri6 is upstream of ri12, ri6 retention can block STAT2-ri12 expression, potentially explaining the association between ri6 and poorer survival. Alternatively, High-PSI $_{ri12-ri6}$ tumors may harbor reduced NMD efficiency, leading to higher levels of PTC-encoding neoantigens that enhance immune recognition. Additional research to investigate whether STAT2 intron retention plays a direct mechanistic role in driving antitumor immune responses in vivo represents a clear next step for future research.

If STAT2 intron retention directly influences therapy response, manipulating it may represent an innovative therapeutic strategy. Using an FDA-approved ASO chemistry, we demonstrate that STAT2 splicing

trial criteria stratified by biomarker positivity. (G) Significantly enriched pathways in High-PSI $_{ri12-ri6}$ or Low-PSI $_{ri12-ri6}$ patients from OAK (FDR < 0.05) using MSigDB Hallmark 2020 Gene Sets (94, 95). Genes were ranked by their Wald test statistic from differential gene expression analysis comparing High-PSI $_{ri12-ri6}$ to Low-PSI $_{ri12-ri6}$ patients with DESeq2, and gene set enrichment analysis was conducted on the ranked gene list using gseapy. A positive normalized enrichment score (NES) indicates pathway enrichment in High-PSI $_{ri12-ri6}$ patients, whereas a negative NES indicates pathway enrichment in Low-PSI $_{ri12-ri6}$ patients. Immune-related pathways are highlighted in purple. (H) NMD score in OAK patients who are High-PSI $_{ri12-ri6}$ ( $\geq 5\%$ ; n = 70 patients) versus Low-PSI $_{ri12-ri6}$ (<5%; n = 433 patients) (boxplots show median and interquartile range, with whiskers extending to 1.5× interquartile; significance was assessed using Student's t test). A lower NMD score reflects less efficient NMD (see Materials and methods).

can be pharmacologically modulated to regulate STAT2 protein expression and IFN-I signaling strength. ASOs targeting STAT2 splicing could enable clinicians to precisely inhibit STAT2 activity as well as IFN-I and IFN-III signaling in cancer as necessary, providing a more refined degree of control over inflammation than is presently possible. Additional studies to assess the impact of ASO-mediated STAT2 splicing manipulation alongside immunotherapy in vivo are therefore warranted.

Though differences in STAT2 ri6 and ri12 retention between tumor and normal tissue appear modest, small splicing changes can have outsized functional consequences: NMD can mask increases in the production of NMD-sensitive isoforms, as described for other targets (74, 75), and simultaneous shifts across multiple isoforms produce nonlinear changes in isoform ratios that are often amplified by complex interactions between transcription, mRNA stability, translation efficiency, and protein turnover (76). Notably, LUAD tumors with reduced NMD efficiency display substantially higher STAT2 intron retention, and pharmacological NMD inhibition elevates truncated STAT2 protein 2- to 3-fold in cell lines, which, taken together, suggests that tumors with low NMD activity plausibly express truncated STAT2 proteins at functionally relevant levels. Key limitations of our study include the inability to directly measure STAT2 protein isoforms in primary tumors owing to the absence of isoform-specific antibodies and the fact that isoforms identified by long-read RNA-seq are not necessarily cancer specific or cancer enriched, as they have not been compared with long-read data from normal lung tissue.

Although RNA splicing has been studied for decades, the full diversity of spliced isoforms, especially in immune-related genes, has only recently begun to be fully appreciated $12, 13, 15, 18, 21, 77$ . The extensive catalog of previously unannotated isoforms uncovered here in well-studied cancer genes underscores how much of the tumor transcriptome, and its functional consequences, remains invisible to short-read approaches alone. Some of these isoforms, including those of STAT2, may be expressed across multiple cell types within the tumor microenvironment, and single-cell and spatial long-read sequencing will be essential to resolve their cell-type specificity in future studies.

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Materials and methods

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Clinical samples

Studies involving human tumor samples were conducted according to the protocol approved by the Institutional Review Board of The Jackson Laboratory for Genomic Medicine (IRB number 2019-RELY-002-HHC and 2019-RELY-002). Postsurgical tumor samples from patients with invasive LUAD were collected with appropriate informed consent at Hartford Hospital. Human bronchial epithelial cells and derived cultures used in this study were obtained from deceased donors through the National Disease Research Interchange (NDRI) and from deidentified deceased donors procured through (Ohio) donor recovery programs. The research was reviewed by The Jackson Laboratory Institutional Review Board (2019-NHSR-048; 2022-NHSR-004) and determined to qualify as non-human subjects research because all specimens were obtained from deceased donors and provided without direct identifiers. All research activities were conducted in accordance with institutional policies and ethical standards.

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Human cell lines

Cell lines were obtained from the American Type Culture Collection (ATCC). A549 lines were cultured in Ham's F-12 Nutrient Mixture (ThermoFisher Scientific no. 11765-054) supplemented with $10\%$ fetal bovine serum (FBS) (GeminiBio no. 100-500), 25 mM HEPES (ThermoFisher no. 15630-080), 2 mM L-glutamine (ThermoFisher no. 25030-081), and 1% penicillin/streptomycin mixture (ThermoFisher no. 15140-122). NCI-H1373, NCI-H1573, NCI-H1693, NCI-H1755, and NCI-H1975 lines were cultured in RPMI-1640 medium (ThermoFisher no. 11875-093) supplemented with 10% FBS (Denville Scientific no. C788U23) and 1% diluted penicillin/streptomycin mixture (ThermoFisher no. 15140-122). All cell lines were grown at 37°C with 5% CO₂. For routine subculturing, cells were lifted by incubating cell cultures with 0.05% trypsin-EDTA (ThermoFisher no. 25300-054) at 37°C until cells were detached. Cells were routinely tested negative for mycoplasma using the MycoAlert Mycoplasma Detection Kit (Lonza no. LT07-318).

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Human primary bronchial epithelial cells

To generate air-liquid-interface (ALI) cultures from lung epithelial progenitors, primary lung epithelial cells were plated on inserts with a pore size of 0.4 $\mu$ m (Corning no. 3470) coated with 0.03 mg/ml Collagen I Rat Tail Protein (Gibco no. A1048301). After seeding, wells were maintained for 8 to 10 days in Pneumacult-Ex Plus Medium (STEMCELL no. 05040) supplemented with 10 $\mu$ M ROCK inhibitor Y-27632 (Abmole no. Y-27632) until cells reached 100% confluence, with media changes every 2 to 3 days. Cells were then differentiated for 5 to 7 days in Pneumacult-ALI Medium (STEMCELL no. 05001) supplemented with 10 $\mu$ M ROCK inhibitor Y-27632 (Abmole no. Y-27632) with media changes every 2 to 3 days, alongside measurement of Trans-Epithelial/Endothelial Electrical Resistance (TEER) every 2 to 3 days until cells were fully differentiated, as described previously (78, 79). Finally, cells were differentiated in Pneumacult-ALI Medium (STEMCELL no. 05001) without ROCK inhibitor for \~28 days with media changes on the basal side of the insert every 2 to 3 days. Once TEER values reached >500 ohms/cm $^{2}$ , media was removed from the apical layer and checked under the microscope every 2 to 3 days for cilia beating and mucus production. After differentiation, the air-liquid interface membrane was harvested and lysed directly in RLT for subsequent RNA extraction.

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Plasmids

All plasmids were sequence-confirmed using whole-plasmid Nanopore sequencing or standard Sanger sequencing (Quintara Biosciences). All primer sequences used for cloning are listed in table S6H.

pVAX1 transient transfection plasmids: Full-length STAT2 isoform sequences were derived via fusion PCR from A549 cDNA using Phusion Hot Start II DNA Polymerase (ThermoFisher Scientific no. F-549L). All constructs were obtained by sequential fusion PCRs of partial elements of STAT2 obtained from A549 cDNA or gDNA, finally NheI and EcoRI sites were added. All cloning oligos used are listed in table S6H. The resulting amplicons were digested using NheI-HF (New England Biolabs no. R3131) and EcoRI-HF (NEB no. R3101) and ligated into the linearized pVAX1 (Addgene no. 196624) backbone using T4 DNA Ligase (NEB no. M0202). Empty vector pVAX1 (pVAX1-EV) was generated by restriction digest using NheI-HF (NEB no. R3131) and XbaI (NEB no. R0145) and ligation of the backbone to itself using T4 DNA Ligase (NEB no. M0202).

pLJM1 lentiviral insert plasmids: Third-generation lentivirus encoding 3xFLAG-tagged STAT2 isoforms were generated by subcloning each isoform from pVAX1 into pLJM1-Polylinker (Addgene no. 164143) using T7\_F and BGH\_R to amplify the insert followed by restriction digest by NheI-HF and EcoRI-HF.

pINDUCER20 inducible insert plasmids: All inserts were amplified from pVAX1 using primers AgeI\_T7 and PacI\_BGH and subcloned into pCR8-ccdb-u1 (gift from A. Cheng) using AgeI-HF (NEB no. R3552) and PacI (NEB no. R0547) sites. Inserts were transferred into pINDUCER20 (Addgene no. 44012) using Gateway cloning (Invitrogen no. 11791020).

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Generation of STAT2 knockout cell lines

STAT2-targeting gRNA was designed using the CRISPR Design Tool (https://design.synthego.com/#/, Synthego) using the Ensembl GRCh38. p10 human genome build targeting STAT2 (table S6D). Single guide RNA (sgRNA) with standard chemical modifications (2'-O-methylated nucleotides and phosphorothiorate linkages in the first and last three bases) targeting the relevant sequences were synthesized (Synthego). Then, 16 $\mu$ g of sgRNA was incubated with 20 $\mu$ g of Alt-R HiFi Cas9 Nuclease V3 (IDT no. 1081060) for 30 min at room temperature. A549 cells were harvested and nucleofected with the sgRNA:Cas9 ribonucleoprotein mixture using the 4D-Nucleofector X Unit (Lonza) with nucleofection solutions and programs as listed in table S6E. Cells were incubated in complete growth media supplemented with 5 $\mu$ M Alt-R HDR Enhancer V2 (IDT no. 10007921). Twenty-four hours after nucleofection, media was removed and replaced with complete growth media without HDR Enhancer. Nucleofected cells were harvested and serially diluted to a concentration of 5 cells/ml and plated into each well of a 96-well plate. Single cell clones were expanded and gDNA was extracted using the QIAamp DNA Mini Kit (Qiagen no. 51306). The edited region was amplified using primers listed in table S6F, and PCR products were confirmed by Sanger sequencing. Chromatogram files from single cell clones were deconvoluted into constituent alleles with DECODR (https://decodr.org/) using parental A549 cells as control. STAT2 knockout (deletion) was confirmed via Western blot and IFN stimulation followed by RT-qPCR for known STAT2-dependent ISGs MX1 and RSAD2 (80).

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CRISPR-mediated endogenous STAT2 FLAG epitope tagging

A sequence encoding a 3xFLAG epitope tag was inserted immediately downstream of the STAT2 start codon in A549 and H1975 cells by CRISPR-Cas9-mediated homology-directed repair (HDR). An sgRNA targeting the STAT2 start codon region (table S6D) was synthesized and complexed with Cas9 as described above. Then, 200 pmol of a single-stranded HDR donor oligonucleotide encoding the 3xFLAG tag flanked by STAT2 homology arms (IDT; sequence listed in table S6G) was added to the nucleofection reaction. Cells were nucleofected with the sgRNA:Cas9 ribonucleoprotein and donor oligonucleotide using the 4D-Nucleofector X Unit with nucleofection solutions and programs as listed in table S6E. Immediately after nucleofection, cells were resuspended in complete growth media supplemented with Alt-R HDR Enhancer V2 (IDT no. 10007921) at 5 $\mu$ M (A549) or 3 $\mu$ M (H1975). After 24 hours, media was replaced with complete growth media without HDR Enhancer. After 3 days, cells were harvested and serially diluted to 5 cells/ml and plated into 96-well plates for single-cell cloning. The edited region was amplified using primers listed in table S6F, and PCR products were confirmed by Sanger sequencing. Successful in-frame FLAG tag insertion was confirmed by Western blot using an anti-FLAG antibody.

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Generating stable cell line expressing STAT2 isoforms

Ten micrograms of lentiviral plasmids were transfected alongside 5 $\mu$ g psPAX2 (Addgene no. 12260) and 2.5 $\mu$ g pMD2.G (Addgene no. 12259) into HEK293T cells using Lipofectamine 3000 (Invitrogen no. L3000015) according to manufacturer instructions. Lentiviral supernatants were collected at 48 and 72 hours and concentrated as previously described (81). Concentrated lentivirus was then resuspended in Opti-MEM (Invitrogen no. 31985) and stored at $-80^{\circ}$ C until further use.

Cells were plated at $4 \times 10^{4}$ cells/cm $^{2}$ and transduced after 2 hours by supplementing media with polybrene (Sigma no. TR-1003-G) to a final concentration of 8 $\mu$ g/ml and adding the desired volume of concentrated lentivirus dropwise. Cells were selected in either 1 $\mu$ g/ml puromycin (Gibco no. A1113803) for lines generated with pLJM1-derived virus or 4 mg/ml G418 (Gibco no. 10131035) for lines generated with pINDUCER20-derived virus.

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IFN stimulation

Cells were stimulated with Universal Type I Human Interferon (PBL Assay Science no. 11200) at indicated doses and durations using complete growth medium as the diluent.

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ASO transfections

LUAD cell lines were reverse transfected in a 24-well plate with 2'-O-methoxyethyl-phosphorothioated ASO (IDT) at a final concentration of 100 nM using Lipofectamine RNAiMAX (Invitrogen no. 13778150) according to manufacturer instructions. Target ASO sequences are listed in table S6C. Seventy-two hours after transfection, cell lysate for RNA or Western blot was collected by direct lysis in the plate.

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NMD inhibition

To inhibit NMD, cells were treated with complete growth media supplemented with 500 ng/ml SMG1i (Sigma-Aldrich no. SML3864) or dimethyl sulfoxide (DMSO) as negative control for 24 hours before collection for RNA or Western blot. For combined ASO transfection and NMD inhibition, cells were transfected with ASO as described above for 72 hours and treated with SMG1i for the last 24 hours before sample collection.

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RNA extraction from tumors and cell lines

High-quality RNA was extracted from samples using the RNeasy Mini Kit (Qiagen no. 74106). For primary tumor samples, three 30- $\mu$ m tissue sections were cut using a Cryostat from each OCT-embedded tumor and placed directly into 350 $\mu$ l of RLT Lysis Buffer supplemented with 1% $\beta$ -mercaptoethanol. For cell lines, cells were lysed by direct addition of 350 $\mu$ l of RLT Lysis Buffer supplemented with 1% $\beta$ -mercaptoethanol to the wells directly. Samples were treated with DNase I (Qiagen no. 79256) for 1 hour at room temperature following manufacturer instructions. For RNA extracted from primary tumor samples, RNA quality was assessed with the RNA 6000 Pico Kit (Agilent no. 5067-1513) on a 2100 Bioanalyzer (Agilent). Only samples with an RNA integrity number above 7.0 were selected for sequencing.

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cDNA synthesis and RT-PCR

RNA was extracted as described above, and 200 to 1000 ng of RNA was reverse-transcribed using SuperScript III Reverse Transcriptase (Invitrogen no. 18080093). Semiquantitative RT-PCR was used to amplify 20 ng of cDNA with optimized melting temperatures and cycle numbers using Q5 High-Fidelity Polymerase with High-GC Buffer (NEB no. M0491S). Primer sequences are listed in table S6A. PCR products were separated on a 2% agarose gel with SYBR Safe (Invitrogen no. S33102) and imaged on a ChemiDoc MP Imaging System (Bio-Rad). Band intensities were quantified with ImageLab 6.1.0 (Bio-Rad). The PSI was calculated as the intensity of the included band of the target event divided by the sum of the included and skipped bands of the target event. For each target event, bands of interest were extracted with a Gel Extraction Kit (Qiagen no. 28704) and Sanger sequenced (Quintara Biosciences) to confirm their identity. Only verified bands were included in the calculation of PSI.

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Quantitative RT-PCR

cDNA was synthesized as described above. Quantitative PCR (qPCR) was used to amplify 10 ng of cDNA with iTaq Universal SYBR Green Supermix (Bio-Rad no. 1725120) in 384-well plates (Applied Biosystems no. 4309849) using a QuantStudio 7 Flex machine (Applied Biosystems). Primers are listed in table S6B. Data were analyzed using QuantStudio Real-Time PCR software. All gene expression was normalized to the housekeeping gene GAPDH (glyceraldehyde 3-phosphate dehydrogenase).

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Western blot analysis

Cells were harvested by direct lysis in the cell-culture dish in 2x Laemmli buffer (Bio-Rad no. 1610737) with 5% (v/v) β-mercaptoethanol preheated to 95°C. Samples were boiled at 95°C for 20 min, with brief vortexing during incubation. Samples were allowed to cool and either frozen at -80°C or run on a 4 to 15% gradient TGX Stain-Free gel (Bio-Rad no. 4568086). Gels were transferred onto 0.2-μm nitrocellulose membranes (Bio-Rad no. 1620168) and blocked in 5% (w/v) milk in Tween 20-TBST (50 mM Tris pH 7.5, 150 mM NaCl, 0.05% (v/v) Tween 20). Blots were incubated with primary antibody overnight at 4°C and with secondary antibody for 1 hour at room temperature. A ChemiDoc MP Imaging System (Bio-Rad) was used for infrared or chemiluminescent detection. Blots probed with an horseradish peroxidase (HRP)-conjugated secondary were incubated in Clarity Western ECL Substrate (Bio-Rad no. 1705060) for 1 min before image acquisition. Protein expression was quantified using ImageLab 6.1.0 software (Bio-Rad) and normalized first to GAPDH as a loading control and then expressed as fold change to experimental controls. All antibodies used and their respective dilutions are listed in table S6I.

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Immunofluorescence

Cells were cultured in black 96-well imaging plates (Revvity no. 6055300) for 48 hours and fixed by incubating wells with 4% (w/v) paraformaldehyde in phosphate-buffered saline (PBS). Cells were permeabilized with 0.2% (v/v) Triton X-100 in PBS and blocked with 10% (v/v) goat serum (Sigma-Aldrich no. G6767 in 0.2% (v/v) Triton X-100 in PBS. Wells were incubated in primary antibody diluted in blocking solution overnight at 4°C and detected using Alexa-fluor-488 anti-rabbit or Alexa-fluor-568 anti-mouse conjugated secondary antibodies (Invitrogen) used at 1:500 in blocking solution. Cells were costained with Hoechst 33342 (ThermoFisher no. H3570, 1:2000) and phalloidin-AlexaFluor 647 conjugate (ThermoFisher no. A22287, 1:1000) in PBS for 15 min at room temperature. Wells were imaged on an Opera Phenix High-Content Screening machine (Revvity). All antibodies used and their respective dilutions are listed in table S6J.

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ViewRNA FISH

RNA transcripts were visualized in optimal cutting temperature (OCT)-embedded lung tumor sections using the ViewRNA Tissue Assay Fluorescence Kits (ThermoFisher no. QVT0700). Human STAT2 ViewRNA type 4 probes, human KRT8 ViewRNA type 6 probes, and human STAT2\_ri6 or \_ri12 ViewRNA type 1 probes were obtained from ThermoFisher (table S6K). The assay was performed according to the tissue-based ViewRNA assay protocol with formaldehyde fixation and a 20-min protease treatment. ViewRNA probes were detected with Leica TCS SP8 confocal microscope at $40\times$ magnification.

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Whole-cell extraction and FLAG immunoprecipitation

Doxycycline-inducible A549 cell lines expressing 3×FLAG-tagged STAT2-FL, STAT2-ri12, or STAT2-ri6 were induced with DOX (100 ng/ml) for 48 hours and subsequently stimulated with IFN-I (1000 U/ml) for 1.5 hours before harvest. Whole-cell extracts (WCEs) were prepared using a high-salt lysis protocol. Briefly, cells were washed with ice-cold PBS and lysed in buffer containing 50 mM Tris-HCl (pH 8.0), 450 mM NaCl, 1% Triton X-100, 2 mM MgCl₂, 0.1 mM ZnCl₂, 2 mM EDTA, 10% glycerol, 1 mM DTT, protease inhibitor cocktail, 1 mM Na₃VO₄, and 50 mM NaF for 30 min at 4°C. An equal volume of NaCl-free buffer was added to adjust the final NaCl concentration to 225 mM. Lysates were incubated on ice for 5 min, clarified by centrifugation (14,000 rpm, 30 min, 4°C), and the supernatant collected as WCE.

For FLAG immunoprecipitation, anti-FLAG M2 agarose beads (Sigma no. A2220) preequilibrated in WCE buffer (225 mM NaCl) were incubated with extracts overnight at 4°C with rotation. Beads were washed four times with WCE buffer and FLAG-tagged proteins were eluted sequentially using 3×FLAG peptide (200 μg/ml) in elution buffer (20 mM HEPES pH 7.5, 100 mM KCl, 0.1% Triton X-100, 20% glycerol, 100 $\mu$ M ZnCl $_{2}$ , 1 mM DTT). Eluates were collected after two successive incubations at 4°C before downstream analyses.

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Long-read RNA-seq of tumor samples

Iso-seq libraries were prepared according to Iso-seq Express Template Preparation (Pacific Biosciences) using 300 ng of RNA. Full length cDNAs were generated using NEBNext Single Cell/Low Input cDNA synthesis and Amplification Module (NEB) in combination with Iso-Seq Express Oligo Kit (Pacific Biosciences), with 12 cycles of PCR amplification. Amplified cDNAs were purified using ProNex beads. All samples yielded more than 160 ng of cDNA and were used for library preparation. SMRTbell library preparation including DNA damage repair, end repair and A-tailing and ligation with SMRTbell Adaptors (Pacific Biosciences) were performed following manufacturer recommendations. Loading protocols for each sample were made using PacBio SMRTLink software following manufacturer recommendations. Libraries were sequenced on either a PacBio Sequel II or PacBio Sequel IIe instrument (Pacific Biosciences). Each sample was individually sequenced on a single SMRT cell.

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Short-read RNA-seq of tumor samples and cell lines

Short-read RNA-seq libraries were prepared with a KAPA mRNA Hyperprep Kit (Roche) according to manufacturer instructions. First, polyA RNA was isolated from 300 ng total RNA using oligo-dT magnetic beads. Purified RNA was then fragmented at 85°C for 6 min, targeting 250–to 300-base pair (bp) fragments. Fragmented RNA was reverse transcribed with random primers with an incubation of 25°C for 10 min, 42°C for 15 min, and an inactivation step at 70°C for 15 min. This was followed by second strand synthesis and A-tailing at 16°C for 30 min and 62°C for 10 min. A-tailed, double stranded cDNA fragments were ligated with Illumina unique adaptors (Illumina). Adaptor-ligated DNA was purified using KAPA Pure beads. This was followed by 10 cycles of PCR amplification. The final library was cleaned up using KAPA Pure Beads (Roche). Quantification of libraries was performed using real-time qPCR (ThermoFisher). Sequencing was performed on an Illumina NovaSeq 6000 instrument generating paired end reads of 150 bp, targeting 100 million to 200 million reads for each sample.

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Long-read RNA data processing

Long-read RNA-seq files were processed according to the Iso-Seq pipeline provided by Pacific Biosciences at https://github.com/PacificBiosciences/pbbioconda. Briefly, HiFi CCS BAM files from sequencing runs were trimmed and demultiplexed using lima (v2.7.1) with the-ccs and-peak-guess parameters. The resultant reads were quality controlled to remove polyA tails and artifactual concatemers using isoseq refine (v4.0.0) with the-require-polya parameter. Reads were assembled into distinctive isoform clusters using isoseq cluster2 (v4.0.0) and mapped to the hg38 genome with pbmm2 (v1.13.0). Finally, mapped isoform clusters were collapsed into nonredundant full-length isoforms using isoseq collapse (v4.0.0).

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Long-read isoform filtering and quality control

Isoforms identified by long-read RNA-seq were filtered to remove low-quality isoforms and artifacts with the SQANTI3 (v5.2) pipeline $(35)$ , found at https://github.com/ConesaLab/SQANTI3. To validate unannotated splicing junctions with SQANTI3, samples selected for long-read RNA-seq were also sequenced with short-read RNA-seq. Briefly, short-read RNA-seq FASTQ files were trimmed using fastp (v0.20.0) and aligned to the hg38 genome using STAR $(82)$ (v2.7.10b) using multi-sample two-pass mapping to maximize sensitivity for detection of unannotated splice junctions. Long-read isoforms were classified using the sqanti3\_qc.py script from the SQANTI3 distribution using the GENCODE v44 comprehensive gene annotation on reference chromosomes $(30)$ as the reference transcriptome, CAGE peaks from the refTSS database (31) (v3.1), the human polyA motif list from SQANTI3, and splice junction output files obtained from STAR. Isoforms were filtered using the rules mode of sqanti3\_filter.py from the SQANTI3 distribution to remove artifacts; for a complete description of filtering parameters used, please refer to the rulesFilter.json file (Data S1). We used per-sample isoform counts from FLAIR (see section "Characterizing long-read isoforms" below) to further filter our isoforms; only isoforms with $\geq5$ long-read counts in $\geq1$ sample or $\geq3$ long-read counts in $\geq2$ samples were retained. The resultant filtered GTF was annotated and merged with well-supported isoforms from the reference GTF GENCODE v44 using a custom Python script.

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Characterizing long-read isoforms

Per-sample isoform quantification from long-read RNA-seq: We used FLAIR (83) (v3.0.0) to quantify isoform counts in long-read RNA-seq samples. Briefly, our long-read GTF was converted to BED12 format using the gtfToGenePred and genePredToBed utilities from the UCSC Genome Browser (84) (https://hgdownload.soe.ucsc.edu/admin/exe/) with default options. We converted HiFi CCS FASTQ files from sequencing runs into FASTA format from the command line and ran flair quantify using the long-read BED12 file using the options -tpm, -stringent, and -check\_splice. We queried the raw counts file across each patient sample and considered an isoform detected in a sample if the raw count was $\geq 1$ using a custom Python script.

Calculating UTR length differences of full-splice match isoforms detected in LUAD: Isoforms were filtered to include only isoforms categorized as full-splice match or reference match by SQANTI3. The diff\_to\_TSS and diff\_to\_TTS parameters from the SQANTI3 classification step were multiplied by -1 to obtain values for the difference in isoform 5' and 3' UTR lengths relative to the closest matching reference isoform, such that a positive number indicates a longer UTR in that isoform relative to the closest matching reference isoform and a negative number indicates a shorter UTR in that isoform relative to the closest matching reference isoform.

Isoform ORF prediction and comparison to reference sequences: We ran the isoform open reading frame prediction tool CPAT (85) (v3.0.2) on our long-read transcriptome FASTA file using options -top-orf=10 and -min-orf=25. The highest scoring predicted ORF for each isoform was collected and filtered to keep all ORFs with a coding probability score $\geq0.364$ (the optimal value for human ORFs). These putative ORFs were compared to human reference protein sequences from the UniProtKB/Swiss-Prot database (37) using blastp (86) (v2.14.0+). We calculated ORF identity to the UniProt reference as follows: $(2\times\text{matching residues})/(\text{query length}+\text{reference length})\times100\%$ . For each ORF, we took the best ORF identity value and rounded with the floor function. Results were grouped by isoform structural category from SQANTI3 and binned as indicated.

Prediction of isoform coding potential: To identify isoforms with likely frameshifts or in-frame premature termination codons, we used a custom Python script and human reference protein sequences from the UniProtKB/Swiss-Prot database $(37)$ as the reference. For each isoform corresponding to a gene present in the reference, the script translated the transcript in all three reading frames and compared the resulting peptide sequences with the annotated reference protein. We first identified isoforms whose translated products contained N- and C-terminal regions matching those of the reference protein. Isoforms in which these termini were split across different reading frames or were separated by a stop codon within the same frame and whose N-terminal ORFs had a stop codon more than 55 nucleotides upstream of the last splice junction $(87)$ were classified as containing a frameshift or an in-frame PTC, respectively. If the stop codon was no more than 55 nucleotides upstream of the last splice junction, the isoform was classified as encoding a previously uncharacterized C terminus. Isoforms whose translations matched the reference protein's N- and C-termini within a single uninterrupted ORF were instead grouped as (i) exact matches (identical to the reference) or (ii) inexact matches (containing internal mismatches or gaps relative to the reference). Isoforms lacking either the N- or C-terminal match were flagged accordingly. Isoforms that were not able to be classified using these definitions were classified as unknown and not considered in further analysis.

Identification of isoforms with retained introns: To identify isoforms with retained introns, we used a custom Python script to collect all possible retained introns from our long-read GTF and remove those introns that are retained in the canonical reference isoform from the GENCODE v44 comprehensive gene annotation $(30)$ .

Classification of isoforms: Isoforms were grouped into the following categories based on their coding potential and intron retention status: "Exact match to reference protein" if the isoform contained an ORF that exactly matched a reference protein; "Novel protein sequence" if the closest matching ORF contained a novel amino acid sequence either internally or at the C terminus; "Intron retention leading to protein truncation" if the isoform contained a frameshift or PTC-containing ORF and contained a retained intron; or "Protein truncation without intron retention" if the isoform contained a frameshift or PTC-containing ORF and did not contain a retained intron.

Machine-learning-based feature importance analysis: Each isoform in the SQANTI3 classification table was labeled “Isoform” or “Artifact” according to its filter\_result. Per isoform structural category, a gradient-boosted classifier (XGBoost v3.2.0; 300 trees, max\_depth = 5, learning rate = 0.05) was trained to recover the Isoform/Artifact decision from the SQANTI3 feature set, with mean area under the ROC curve (AUC) estimated by stratified five-fold cross-validation (scikit-learn v1.7.2, sklearn.model\_selection.StratifiedKFold, sklearn.metrics.roc\_curve and auc). Per-feature importance was then quantified as the mean reduction in AUC across 30 independent random permutations of that feature's values across isoforms, using sklearn.inspection.permutation\_importance with scoring="roc\_auc."

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Differential splicing and gene expression analysis

We used a custom in-house pipeline to conduct differential splicing analysis, available at https://github.com/TheJacksonLaboratory/splicing-pipelines-nf. Briefly, the pipeline was used to trim FASTQ files with trimmomatic (88) (v0.39) and align them to the human reference genome with the merged long-read and reference GTF using STAR (82) (v2.7.9a). A PSI for each splicing event in each sample was calculated using rMATS (89) (v4.1.2) using both splice junction read counts as well as exon and intron body read counts to infer PSI. When applicable, a $\Delta$ PSI was calculated wherein $\Delta$ PSI = (mean PSI) $_{case}$ – (mean PSI) $_{control}$ . Gene and isoform count estimates were made using StringTie (90) (v2.1.7), with STAR-aligned BAM files as input and compiled into a counts matrix using a custom Python script. Differential gene analysis was conducted using DESeq2 (91) (v1.44.0) using a Wald test to calculate P values and the Benjamini-Hochberg method to derive FDR-corrected P values.

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TCGA splicing analysis, gene expression, and tumor purity estimates

BAM files corresponding to genome-mapped RNA-seq files from LUAD patients (TCGA-LUAD) were downloaded from the Genomic Data Commons (accession no. phs000178.v11.p8) using the gdc-client executable (https://github.com/NCI-GDC/gdc-client) with a manifest derived by checking options for Data Type:Aligned Reads, Experimental Strategy:RNA-Seq, Workflow:STAR 2-Pass Transcriptome, and Data Format:bam. BAM files were converted back to raw FASTQ format using samtools (92) (v1.4.1) to sort BAM files by name (option -n) and the bamtofastq utility from bedtools (93) to convert the sorted BAM file into paired-end FASTQ files. FASTQC (https://www.bioinformatics.babraham.ac.uk/projects/fastqc/, v0.11.9) was used to calculate quality metrics for the resultant FASTQ files. Only samples for which both FASTQ files passed default metrics were considered for further analysis. Splicing analysis and gene expression analysis were conducted using the in-house pipeline described above with a read length of 50 bp and strandedness set to “false” to indicate that libraries were unstranded. Tumor purity estimates from TCGA-LUAD (62) were downloaded from https://raw.githubusercontent.com/BioinformaticsFMRP/TCGAbiolinks/master/data/Tumor.purity.rda.

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Splicing analysis and gene expression from OAK and IMvigor210

FASTQ files from pretreatment tumor samples from nonsquamous non-small cell lung cancer patients from OAK, metastatic urothelial carcinoma patients from IMvigor210, and associated metadata were downloaded from the European Genome-phenome Archive (accession numbers EGAD00001008549, EGAD00001008550, EGAD00001007703, EGAD00001006630, and EGAD00001006631). Splicing analysis and gene expression analysis were conducted using the in-house pipeline described above with a read length of 51 bp and strandedness set to "first-strand" to indicate that libraries were reverse stranded.

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NMD score

To score NMD efficiency, we used PSI values from our rMATS-based pipeline for 12 NMD-sensitive poison exons in SR family splicing factors (58–60). Splicing event PSI values were Z-scored and individual event Z-scores were summed in each sample, then multiplied by -1 to derive the NMD score. Splicing event IDs for the included events are listed in table S5, F and G. FASTQ files from siRNA-mediated UPF1 silencing experiments were downloaded from the Gene Expression Omnibus (accession number GSE176197), and splicing analysis and gene expression analysis were conducted using the in-house pipeline described above with a read length of 150 bp and strandedness set to “first-strand” to indicate libraries were reverse stranded.

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IFN signaling scores

IFNG.GS and ISG.RS scores were calculated using gene lists as previously described $(69)$ . Briefly, VST-normalized counts from DESeq2 of genes from each list (excluding STAT2) were summed within each sample and Z-scored across each group.

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Gene set enrichment analysis

To conduct gene set enrichment analysis on differentially expressed genes, genes were ranked by their Wald test statistics as calculated by DESeq2 (91) (v1.44.0). GSEApy (94) (v1.1.3) was used to conduct enrichment analysis on the ranked gene list using the "Prerank" module with the Molecular Signatures Database (MSigDB) Hallmark 2020 Gene Set (95).

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Prediction of RBP motifs

We used the tool RBPmap at http://rbpmap.technion.ac.il/ (52) to identify predicted RNA-binding protein motifs that overlapped the target sites of STAT2 ri6- and ri12-targeting ASOs. Overlapping motifs were visualized using the UCSC genome browser.

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AlphaFold 3 protein structure predictions

To predict protein structures, polypeptide sequences were processed by AlphaFold 3 (96) using the online server at: https://alphafoldserver.com. Resultant protein structure files were visualized using ChimeraX-1.9 (97).

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Statistical analysis

For the proportion of novel isoforms stratified by coding sequence impact, significance was assessed with a hypergeometric test taking the P value for over- or underenrichment as appropriate. For splicing from short-read RNA-seq, significance was assessed using the rMATS statistical model $(89)$ using the FDR-corrected P value. For subsampling analysis, an equal number of tumor and normal samples were selected using the function random.choice from numpy (v1.26.4), and significance was assessed using a two-sided Mann-Whitney U test and was repeated 100 times. All gene, pathway, and cell-type enrichment analysis results were filtered for FDR-adjusted P < 0.05. For RT-PCR, Western blots, and quantitative RT-PCR, data are shown as mean ± SD, and significance was assessed using an unpaired two-tailed Student's t test unless otherwise specified. Survival analysis was conducted using right-censored survival data from OAK and IMvigor210, and significance was assessed using the Wald test without multiple comparisons adjustments for Cox proportional hazards models using the R package survivalAnalysis (v0.3.0) or the log-rank test for Kaplan-Meier curves using the R package survival (v3.8.3) (98). We used the function surv\_cutpoint from the R package survminer (v0.5.0) on biomarker-negative (TMB < 16 mutations/Mb or TMB not specified) patients from OAK and IMvigor210 to identify optimal PSI $_{ri12-ri6}$ cutoffs for Kaplan-Meier survival analysis.

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Generative AI for writing code

We used Claude Code (Claude Sonnet 4.6; Anthropic, PBC) for assistance with writing code and as an editorial aide during the editing process. All artificial intelligence (AI)-generated code was produced in specific subdirectories without access to parent data or the ability to write outside of those folders. Prompts for script generation included strict instructions to not modify any data in parent directories, and all AI-generated or AI-edited scripts were manually checked before use.

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Graphs and figures

Data were processed using Python or R, and plots were generated with R using the ggplot2 library or Microsoft Excel. Figures were made with Adobe Illustrator 2023 for Mac in compliance with Science/AAAS guidelines concerning image integrity.

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ACKNOWLEDGMENTS

We thank all members of the Anczuków and Palucka labs for helpful discussions and comments on the manuscript and A. Patel from ThermoFisher for assistance with ViewRNA probe design. We acknowledge assistance from the Microscopy, Genome Editing, and Genome Technologies Sequencing Services at The Jackson Laboratory, which are supported in part by National Cancer Institute (NCI) grant P30CA034196. We used Claude Code (Claude Sonnet 4.6; Anthropic, PBC) as an assistive editing tool to optimize code design and condense language during the editing process. We performed molecular graphics and analyses with UCSF ChimeraX, developed by the Resource for Biocomputing, Visualization, and Informatics at the University of California, San Francisco, with support from National Institutes of Health grant R01-GM129325 and the Office of Cyber Infrastructure and Computational Biology, National Institute of Allergy and Infectious Diseases. This research makes use of data generated by Genentech. Funding: We acknowledge funding from National Institutes of Health grants U19AI142733 (K.P., O.A.), R01CA248317 (O.A.), R01GM138541 (O.A.), F30CA278494 (R.P.E.), and P30CA034196 (K.P., O.A., R.P.E.) and funding from Sanofi S.A. SANOFI-SRA-FY19-JFB (J.B.). Author contributions: Conceptualization: R.P.E., O.A., J.B., K.P.; Methodology: R.P.E., O.A., K.P., M.K., N.K.L., M.B., T.-C.W., S.P., I.W., F.M., M.E.P., P.C.; Investigation: R.P.E., M.B., A.S., P.Y., R.B., M.D., H.G.K., I.W.; Visualization: R.P.E., O.A., M.B.; Funding acquisition: O.A., K.P., J.B., R.P.E.; Project administration: R.P.E., O.A., K.P.; Supervision: O.A., K.P., J.B.; Writing – original draft: R.P.E., O.A., M.B.; Writing – review & editing: R.P.E., O.A., K.P., R.B., J.B., N.K.L., M.B., S.P. Competing interests: R.P.E., O.A., N.K.L., J.B., and K.P. are listed on a patent application (D25-008-USPROV1, US provisional application no. 63/852,095) submitted by The Jackson Laboratory that covers the use of splice-modulating ASOs targeting STAT2 as well as STAT2 intron retention events as immunotherapy biomarkers. In the early stage of the study, J.B. was a member of the board of directors and scientific advisory board of Neovacs and Ascend Biopharma and a scientific advisory board member of Cue Biopharma. Now, J.B. is the founder of Immunoledge LLC, an entity designed to advise biotech start-ups. In this role, J.B. serves as chief information officer of Georgiamune, scientific advisory board member of Metis Therapeutics, and adviser to The Jackson Laboratory. During the course of this study, K.P. was a member of the advisory board for Cue BioPharma and a founding member of Guardian Bio. OA is a member of the scientific advisory board of NeoSplice, Akari Scientific, and EnteloBio. The authors declare no other competing interests. Data, code, and materials availability: Our splicing analysis pipeline v2.0 has previously been described (99) and is freely available on Github (https://github.com/The.JacksonLaboratory/splicing-pipelines-nf). All other data are available in the paper and supplementary materials or are available from the corresponding author upon request. Tables S1 to S6 may also be accessed at https://github.com/ryanpe13002/Supplementary-Tables-2/. Sequencing data generated as part of this study are available on dbGaP (the Database of Genotypes and Phenotypes) under accession no. phs004211.v1.p1 and ImmPort under study accession no. SDY3373. License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.aea7156

Figs. S1 to S8; Tables S1 to S6; MDAR Reproducibility Checklist; Data S1

Submitted 24 July 2025; resubmitted 1 April 2026; accepted 26 August 2026

10.1126/science.aea7156

Decoupled self-assembled monolayer and perovskite deposition for efficient flexible solar modules

Yeyong Wu, Xikun Zhang, Tiankai Zhang, Guiying Xu\*, Yunxiu Shen, Chengxin Guo, Qing Miao, Junyuan Ding, Yue Yin, Qinrong Cheng, Wen Liu, Xiaoxiao Wu, Kaiqiang Chen, Wenwen Kou, Zhiyun Cao, Haiyang Chen, Weijie Chen, Yujin Chen, Feng Gao, Yaowen Li\*, Yongfang Li

Full article and list of author affiliations: https://doi.org/10.1126/science.aef9745

INTRODUCTION: Flexible perovskite solar cells (PSCs) enable efficient solar energy harvesting in curved and mobile scenarios such as buildings, transportation, wearables, and portable devices, substantially expanding the clean energy supply boundary. Although small-area flexible PSCs have reached a power conversion efficiency (PCE) of 26.22%, approaching that of rigid PSCs, device upscaling triggers pronounced declines in both PCE and operational stability, creating a notable performance gap between large-area flexible perovskite solar modules (PSMs) and their rigid counterparts. This considerable efficiency and stability deficit remains a critical barrier to the commercialization of both single-junction and tandem flexible perovskite photovoltaics.

RATIONALE: The inferior performance of large-area flexible PSMs is closely associated with the distinct surface properties of flexible substrates. Their ITO surfaces typically have a lower density and less uniform distribution of hydroxyl groups, compromising self-assembled monolayer (SAM) anchoring and wetting of polar perovskite precursors. Surface treatment can temporarily increase hydroxyl density, whereas SAM-perovskite precursor codeposition can overcome the wetting limitation. However, these hydroxyl groups are rapidly lost in the polar precursor solution, creating a kinetic mismatch between hydroxyl loss and SAM anchoring. Specifically, interactions between perovskite colloids and the phosphonic acid groups of SAM molecules retard SAM adsorption, causing hydroxyl groups to be depleted before efficient SAM anchoring and ultimately compromising SAM coverage and perovskite crystallization. Accordingly, we introduced 3,5-bis(methylsulfonyl)phenylammonium iodide (BSAI) as a decoupling agent into the codeposition precursor. We hypothesized that BSAI preferentially interacts with perovskite precursor species, weakening their interaction with Me-4PACz and accelerating SAM anchoring.

RESULTS: Systematic investigations reveal BSAI exerted a dual function through its ammonium and dual sulfonyl groups bound strongly to perovskite colloids. First, it disrupted coordination between Pb-I colloids and the phosphonate groups of Me-4PACz to facilitate the quick adsorption to the substrate before surface hydroxyl groups desorption, enabling uniform SAM anchoring on large-area substrates. Meanwhile, it also retarded perovskite nucleation to promote oriented crystal growth, yielding optimized film morphology over large areas. The compact Me-4PACz anchoring and high perovskite crystallinity in decoupled codeposition strategy contributed to a certified PCE of 26.9% for small-area flexible PSCs, while certified PCEs of 22.3, 20.6, and 20.2% are achieved on flexible PSMs with substrate areas of 25, 100, and 1050 cm $^{2}$ (device areas of 14.55, 80, and 750 cm $^{2}$ ), respectively. The modules retained more than 92% of their PCE after \~1000 hours of maximum power point tracking under the ISOS-L-3 protocol (85°C, 65% relative humidity) and passed all IEC TS 63163:2021 test sequences, as certified by TÜV SÜD. The strategy also shows broad applicability to rigid substrates and different SAM molecules.

CONCLUSION: We identified the key factors by which substrate surface properties constrain the performance of flexible PSMs, and developed decoupled codeposition strategy to address the long-standing bottleneck of performance loss during flexible PSMs upscaling. The decoupling agent BSAI reduced perovskite-SAM strong interactions to facilitate compact SAM anchoring and high perovskite crystallinity, which enables high-efficiency, stable large-area flexible photovoltaic devices. This work advanced the commercial viability of flexible perovskite photovoltaics and demonstrated their practical potential in portable and mobile power supply scenarios. □

Compact and uniform Me-4PACz and perovskite film on flexible substrate through Decoupled SAM-perovskite codeposition strategy. The decoupling agent BSAI preferentially binds to the Pb-I framework, thereby reducing the Me-4PACz-perovskite interaction. This effect facilitates the quick anchoring of Me-4PACz to surface hydroxyl groups on PET/ITO substrates and ameliorates perovskite crystallization kinetics, ultimately yielding stable tridentate-anchored SAMs and uniform perovskite films.

Me-4PACz:BSAI:perovskite solution

Decoupled self-assembled monolayer and perovskite deposition for efficient flexible solar modules

Yeyong Wu $^{1\dagger}$ , Xikun Zhang $^{1\dagger}$ , Tiankai Zhang $^{2\dagger}$ , Guiying Xu $^{1*}$ , Yunxiu Shen $^{1}$ , Chengxin Guo $^{3}$ , Qing Miao $^{1}$ , Junyuan Ding $^{1}$ , Yue Yin $^{1}$ , Qinrong Cheng $^{1,3}$ , Wen Liu $^{1}$ , Xiaoxiao Wu $^{1}$ , Kaiqiang Chen $^{1}$ , Wenwen Kou $^{1}$ , Zhiyun Cao $^{1}$ , Haiyang Chen $^{1}$ , Weijie Chen $^{1}$ , Yujin Chen $^{3}$ , Feng Gao $^{4}$ , Yaowen Li $^{1,5*}$ , Yongfang Li $^{1,3,6}$

The power conversion efficiency (PCE) and stability of flexible perovskite solar modules (PSMs) are less than those of their rigid devices because surface hydroxyls desorption on flexible substrates, which disrupts self-assembled monolayer (SAM) anchoring and perovskite crystallization. We developed a decoupled SAM-perovskite codeposition strategy that accelerates SAM anchoring by reducing the SAM-perovskite interaction and ameliorates perovskite crystallization. The certified PCE with phenethylammonium iodide as the passivation molecule was 20.2% on PSMs with device areas of 750 cm $^{2}$ . With 1,3-diaminopropane dihydroiodide as the passivator, the PCE of 22.0% for a device area of 14.55 cm $^{2}$ decreased by 8% after 1044 hours under maximum power point tracking at 85°C and 65% relative humidity. The devices pass all sequences of an international commercialization assessment standard for flexible portable PSMs.

Cost-effective, highly efficient flexible perovskite solar cells (PSCs) could expand the application of solar energy to curved buildings, vehicles, airplanes and wearable electronics (1-3). Although small-area flexible PSCs have already achieved power conversion efficiencies (PCE) of $26.22\%$ (4-6), appreciable PCE and stability drops occur upon device upscaling (fig. S1 and tables S1 and S2), which results in a performance gap between large-area flexible perovskite solar modules (PSMs) and their rigid counterparts (7-13). The substantial efficiency and stability deficit poses challenges for the commercial viability of both single junction and tandem flexible PSMs.

The substantial differences in substrate properties are the primary cause of the inferior performance of large-area PSMs (14–16). Flexible plastic substrates only permit low-temperature indium tin oxide (ITO) deposition, which forms ITO layers with low crystallinity that have surface hydroxyl groups that readily desorb in polar solvents. These properties increased the difficulty of uniformly depositing large-area self-assembled monolayers (SAMs) and perovskite films compared with rigid glass substrates (17–19). Even the SAM-perovskite precursor codeposition method, which circumvents the issue of poor large-area wettability of perovskite on the SAM layer and realizes state-of-the-art efficiency on rigid perovskite modules, still fails when being applied on flexible substrates (20, 21).

The key reason for the ineffectiveness of the codeposition method on the flexible substrate lies in the dynamic competition between rapid surface hydroxyl groups desorption and delayed SAM anchoring. The surface hydroxyl groups on the flexible substrate quickly desorb, whereas the strong interaction between perovskite and phosphonic acid groups in the SAM molecules impedes the SAM anchoring process (22, 23), yielding nonuniform SAM deposition and compromised perovskite crystallinity (24–27). To address this dynamic competition, we developed a decoupled codeposition strategy by incorporating a decoupling agent, 3,5-bis(methylsulfonyl) phenylammonium iodide (BSAI), into the perovskite-SAM ([4-(3,6-dimethyl-9H-carbazol-9-yl) butyl] phosphonic acid, Me-4PACz) codeposition process. The ammonium group and two sulfonyl groups of BSAI cause it to bind strongly to perovskite colloids and disrupt the coordination between Pb ions and the phosphonic acid groups in Me-4PACz.

This dual function not only enabled effective and uniform SAM layer deposition on large-area flexible substrates with minimal interference, but also retarded nucleation to promote oriented perovskite growth, which realized optimized morphologies over areas up to $1050 \, cm^2$ . This decoupled codeposition strategy enables a record PCE of 26.9% (26.9% certified) on small-area ( $0.0628 \, cm^2$ ) flexible PSCs. Moreover, it delivered scalable flexible PSMs with record PCE of 23.1% (22.3% certified), 21.0% (20.6% certified), and 20.6% (20.2% certified) on 25, 100, and $1050 \, cm^2$ substrates (device areas of 14.55, 80, and $750 \, cm^2$ , respectively), mitigating the constraint of PCE loss as the module device size increased. Moreover, the flexible PSMs retained >92% of their initial PCEs after \~1000 hours of continuous operation under maximum power point tracking (MPPT) under ISOS-L-3 protocol [ $85^\circ C$ , 65% relative humidity (RH)] and successfully passed all test sequences defined by IEC TS 63163:2021, an international commercialization assessment standard for flexible portable photovoltaic modules, as certified by TÜV SÜD. We also applied this decoupled codeposition strategy to rigid modules, delivering rigid PSMs ( $5 \, cm \times 5 \, cm$ ) with a certified PCE of 23.8% and $T_{97} >2500$ hours aging under the same protocol. The decoupled codeposition strategy deployed high-efficiency flexible PSMs, allowing stable power supply while being integrated into portable chargers and radio-controlled unmanned aerial vehicles (RC-UAVs), validating their practical applicability and commercial viability.

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Desorption-prone nature of surface hydroxyl oxygen on flexible substrates

Initially, we compared the performance of rigid and flexible PSMs (with a size of $5 \, cm \times 5 \, cm$ ) by applying two different common fabrication methods: sequential deposition and conventional codeposition method (detailed fabrication procedures are provided in the Experimental section). On glass/ITO substrates, PSMs fabricated with the codeposition method achieved a slightly higher average PCE than those prepared by Me-4PACz-perovskite sequential deposition (22.0% versus 21.7%), highlighting its superiority in the fabrication of large-area modules. However, on polyethylene terephthalate (PET)/ITO substrates (the electrical and optical properties are similar to the glass/ITO substrates, fig. S2), the PSMs fabricated by the conventional codeposition method and sequential deposition method both delivered a much lower average PCE (14.6 and 15.8%, respectively) compared with rigid devices fabricated with the same deposition method (22.0 and 21.7%), which highlights the intrinsic limitations of the previously reported fabrication methods for high-performance flexible PSMs (Fig. 1A, fig. S3, and table S3).

Altered surface chemical properties, especially the stability of surface hydroxyl groups, have presented a major obstacle for applying common fabrication methods on flexible substrates. X-ray photoelectron spectroscopy (XPS) revealed that the ratio of hydroxyl oxygen to lattice oxygen on PET/ITO (15%) was only half of that on glass/ITO (29%) (Fig. 1, B and C, fig. S4, and table S4) (28–30). Low-density surface hydroxyl coverage results in poor wettability (fig. S5) (31, 32). Specific surface treatment, such as plasma treatments, can temporarily increase hydroxyl group density on the surface of PET/ITO and improve the wettability at the initial stage (fig. S5). However, these surface hydroxyl groups generated by plasma treatment still quickly desorb, especially under external perturbations (28, 33).

Fig. 1. Desorption-prone nature of surface hydroxyl oxygen on flexible substrates. (A) The distribution of PCEs for PSMs on rigid (glass/ITO) and flexible (PET/ITO) substrates using sequential deposition and codeposition. (B and C) XPS O 1s spectra of glass/ITO (B) and PET/ITO (C) substrates at the initial state, after plasma treatment, after EtOH washing, and after DMF washing. (D) XPS P 2p spectra of glass/ITO and PET/ITO surfaces through sequential deposition and codeposition. (E) Schematics of hydroxyl group density, SAM anchoring, and perovskite film quality on PET/ITO through sequential deposition and codeposition.

After exposure to polar solvents, including ethanol (EtOH) and dimethylformamide (DMF)—which are commonly used in processing SAM and perovskite layers, respectively—the hydroxyl-to-lattice oxygen ratio on glass/ITO decreased only slightly (from 58 to 48% after EtOH washing and from 58 to 49% after DMF washing). By contrast, the corresponding hydroxyl-to-lattice oxygen ratio on PET/ITO decreased sharply (from 53 to 19% after EtOH washing and from 53 to 21% after DMF washing) (Fig. 1, B and C, fig. S4, and table S4) (28, 34), implying the rapid desorption of surface hydroxyl groups. We attributed the desorption-prone nature of hydroxyl groups on PET/ITO to the lower crystallinity of the ITO layer, which resulted in a higher concentration of oxygen vacancies and more electron-deficient In/Sn sites (fig. S6 and supplementary text section 1) (35). These electron-deficient In/Sn sites readily interacted with Lewis basic solvents, such as DMF and EtOH, through Lewis acid-base interactions, thereby perturbing surface hydroxyl binding and promoting hydroxyl loss (fig. S7 and supplementary text section 2) (36–38).

The desorption-prone nature of surface hydroxyl groups on PET/ITO largely affected SAM deposition in the sequential process. The P 2p signal intensity in XPS from Me-4PACz on PET/ITO was approximately half of that on glass/ITO (\~6800 versus \~3300) (Fig. 1D), indicating less efficient anchoring of Me-4PACz on the flexible substrate. In addition, the subsequent perovskite crystallization was adversely affected by the intrinsically nonpolar Me-4PACz terminal group (figs. S8 to S11), which led to a broad distribution of PCEs and reduced reproducibility of flexible PSMs fabricated by sequential deposition (Fig. 1A and fig. S3). These findings indicated that sequential deposition was not well-suited for large-area flexible PSMs (schematically illustrated in Fig. 1E).

The codeposition method mitigated the large-area wettability limitations of perovskite precursors on SAM-covered surfaces (fig. S12). However, the easy removal of surface hydroxyl groups by DMF also severely disrupted the Me-4PACz anchoring process in the codeposition method on flexible substrates. After rinsing codeposited Me-4PACz-perovskite layers with DMF (fig. S13), the P 2p signal intensity on PET/ITO was again approximately half of that on glass/ITO (\~2800 versus \~4500) (Fig. 1D), confirming reduced anchoring efficiency on flexible substrates even with codeposition. Given the strong interactions between Me-4PACz and the perovskite precursors in solution (figs. S14 to S17 and supplementary text section 3), the limited Me-4PACz anchoring would impair hole extraction and the residual Me-4PACz in precursors would perturb perovskite film growth, as evidenced by the poor film morphology observed on flexible substrates (figs. S18 to S21 and supplementary text section 4; schematically illustrated in Fig. 1E).

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Decoupled codeposition strategy and the selection of decoupling agent

Given that surface hydroxyl groups on the PET/ITO substrates are prone to desorption, merely increasing their population cannot achieve effective SAM anchoring. Ideal SAM-perovskite codeposition requires accelerating the anchoring kinetics between SAM molecules and hydroxyl groups. We introduced a decoupling agent with a much stronger affinity to Pb-I framework in conventional codeposition method to develop a “decoupled codeposition” strategy that avoided the poor wettability issue of depositing perovskite film on SAM, especially over a large-scale. The decoupling agent preferentially bound to Pb-I framework, thereby reducing the Me-4PACz-perovskite interaction and enabling Me-4PACz quick anchoring onto PET/ITO. Once anchored, Me-4PACz could be stabilized on the ITO surface.

We designed three molecules containing Lewis base or ammonium groups that could interact with Pb-I framework through coordination and ionic bonding: 3,5-bis(methylsulfonyl)phenylamine (BSA, two -S=O groups), phenylammonium iodide (PAI, ammonium group), and 3,5-bis(methylsulfonyl)phenylammonium iodide (BSAI, integrating both functionalities) [fig. S22; detailed synthesis procedures of BSAI are in the materials and methods in the supplementary materials (SM), as candidates for decoupling agents] (39). To evaluate the decoupling efficacy of these additives, we systematically tracked the interactions of Me-4PACz in the full precursor solution upon the introduction of BSA, PAI, and BSAI, respectively. Fourier-transform infrared (FTIR) and nuclear magnetic resonance (NMR) spectroscopies (Fig. 2, A and B, fig. S23, and supplementary text section 5) jointly revealed that the bifunctional BSAI triggered the greatest release of Me-4PACz from the Pb-I framework colloids, surpassing those of BSA and PAI, and led to the most effective decoupling of Me-4PACz and perovskite precursors. Density functional theory (DFT) calculations also showed that BSAI exhibited strong binding to the precursor Pb-I framework (-1.43 eV), substantially exceeding that of Me-4PACz (-0.60 eV), through cooperative S=O…Pb coordination and N-H…I ionic interactions (fig. S24). Interaction region indicator analysis further confirmed strong attractive interactions for both binding motifs (fig. S25). Such synergistic dual strong interactions enabled BSAI to outcompete Me-4PACz for binding to the Pb-I colloids, thereby effectively producing the strongest decoupling effect.

We incorporated BSAI as the decoupling agent in the codeposition method to reduce the interaction between Me-4PACz-perovskite and promote Me-4PACz release to anchor to ITO. The adsorption and anchoring kinetics of Me-4PACz with and without the BSAI were tracked from the in situ FTIR spectra (Fig. 2, C to E, and figs. S26 and S27). At the pre stage (0 min), the as-deposited film without BSAI showed only slight shifts of the P=O and P-O-(H) peaks (1260.17 and 1107.05 cm $^{-1}$ , respectively), relative to the precursor solution (1260.74 and 1106.46 cm $^{-1}$ respectively), indicating that most Me-4PACz was associated with Pb-I framework colloids, thereby suppressing its initial adsorption onto PET/ITO (fig. S26). By contrast, the film with BSAI exhibited pronounced peak shifts from 1266.04 and 1103.08 cm $^{-1}$ to 1259.50 and 1105.60 cm $^{-1}$ , respectively, implying substantial coordination of Me-4PACz onto PET/ITO with electron-deficient In/Sn sites.

During subsequent processing, both samples exhibited three progressive stages (stages I through III). For the sample without BSAI, we observed a negligible P–O–(H) peak shift (from 1107.05 to 1106.66 cm $^{-1}$ ) within the first 9 min (stage I), which then shifted to 1104.83 cm $^{-1}$ (at a rate of $\sim0.17~cm^{-1}~min^{-1}$ ) in the next 11 min, which indicated that only a limited number of P–O–In/Sn bonds formed during this period (stage II). The peak position stabilized at 1104.64 cm $^{-1}$ after 20 min, implying that the anchoring process was nearly complete (stage III). By contrast, the sample with BSAI exhibited distinctly accelerated anchoring kinetics. The rapid shift occurred much sooner (after 5 min) and proceeded at a higher rate of $\sim0.64~cm^{-1}~min^{-1}$ , indicating more pronounced formation of P–O–In/Sn bonds (stage II). The P–O–(H) vibration signal stabilized at 1097.98 cm $^{-1}$ after 16 min, indicating that anchoring was near saturation (stage III). This greater peak shift rate revealed that the incorporation of BSAI effectively disrupted the interaction between Me-4PACz and the Pb-I framework and facilitated the rapid release and more effective anchoring of Me-4PACz on the PET/ITO surface. In addition, DFT calculations revealed a tridentate anchoring configuration, characterized by one P=O $\cdots$ In/Sn coordination interaction and two covalent P–O–In/Sn bonds, with a high binding energy ( $E_{b}$ ) of -4.650 eV (fig. S28). Overall, the combined in situ FTIR and DFT results indicated that Me-4PACz adopted a tridentate anchoring configuration on PET/ITO.

We further checked the effectiveness of Me-4PACz anchoring with the BSAI incorporation through time-resolved ex situ measurements, including XPS (Fig. 2, F to H, fig. S29, and table S5), atomic force microscopy-infrared spectroscopy (AFM-IR, fig. S30), and scanning electrochemical cell microscopy-thin-layer cyclic voltammetry (SECCM-TLCV, fig. S31) (40). All of the measurement results showed evidence of a three-stage Me-4PACz anchoring process (supplementary text section 6).

Based on these results, the anchoring process of Me-4PACz on PET/ITO during conventional and decoupled codeposition can be summarized as follows (Figs. 2, I to P): During the pre stage, the conventional codeposition process (without BSAI) exhibited strong interactions between Me-4PACz and Pb-I framework colloids and retained most Me-4PACz in the precursor solution and suppressed its adsorption onto PET/ITO, resulting in limited $\mathrm{P = O\dots In / Sn}$ coordination. The facile coordination of DMF with electron-deficient In/Sn sites perturbed the local electronic environment, weakening hydroxyl-In/Sn interactions, and promoting interactions between neighboring hydroxyl groups (Fig. 2I). By contrast, with BSAI, Me-4PACz was effectively released from the Pb-I framework colloids and rapidly adsorbed onto PET/ITO through stronger coordination interactions. Surface hydroxyl groups then interacted with the phosphonic acid moieties of adsorbed Me-4PACz, stabilizing hydroxyl-rich interfacial sites against DMF-induced perturbation (Fig. 2M).

During stage I, at relatively low temperatures, dehydration-condensation slowly occurred between P-OH groups of adsorbed Me-4PACz and surface hydroxyl groups, gradually forming In/Sn-O-P bonds in both systems. In the conventional process, a competing DMF-induced dehydration-condensation simultaneously consumed surface hydroxyl species and reformed metal-oxygen-metal bonds (Fig. 2, J and N). During stage II, at elevated temperatures, anchoring reactions become more favorable. However, in the conventional process, hydroxyl depletion suppressed efficient anchoring despite partial migration of Me-4PACz toward the ITO interface induced by perovskite crystallization (Fig. 2K). By contrast, the BSAI-containing system showed accelerated anchoring caused by effective initial adsorption (Fig. 2O). During stage III, as anchoring sites approach saturation and surface hydroxyl density decreases, the anchoring rate slows markedly in both systems (Fig. 2, L and P).

Fig. 2. Decoupled codeposition strategy and anchoring kinetics of Me-4PACz. (A) FTIR spectra of pure Me-4PACz, Me-4PACz:DMF:FAI:PbI $_{2}$ solution, Me-4PACz:DMF:FAI:PbI $_{2}$ :BSA solution, Me-4PACz:DMF:FAI:PbI $_{2}$ :PAI solution, and Me-4PACz:DMF:FAI:PbI $_{2}$ :BSAI solution. (B) ${}^{1}$ H NMR spectra of pure Me-4PACz, Me-4PACz:FAI:PbI $_{2}$ , Me-4PACz:FAI:PbI $_{2}$ :BSA, Me-4PACz:FAI:PbI $_{2}$ :PAI, and Me-4PACz:FAI:PbI $_{2}$ :BSAI samples in DMF-d $_{7}$ . (C to E) In situ FTIR spectra of samples without BSAI (C) and with BSAI (D), together with the corresponding evolution of the P–O–(H) vibrational peak position (E) on PET/ITO substrates during the annealing process. (F to H) Time-resolved ex situ XPS tracking of the anchoring kinetics. High-resolution P 2p spectra of the samples processed without BSAI (F) and with BSAI (G). Evolution of the P/In signal intensity ratio plotted as a function of annealing time (H). (I to P) Schematic illustration of the anchoring process of Me-4PACz on PET/ITO during both the conventional (I to L) and decoupled (M to P) codeposition processes.

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SAM morphology and perovskite crystallization modulation by the decoupled codeposition

The accelerated anchoring kinetics of Me-4PACz in the decoupled code-position process enabled a uniform SAM morphology on the PET/ITO surface. Time-of-flight secondary ion mass spectrometry (ToF-SIMS) analysis revealed a more compact and vertically concentrated distribution of Me-4PACz, represented by the $\mathrm{PO}_2^-$ signal, near the substrate region in the BSAI incorporated decoupled codeposited (target) film compared with the conventionally codeposited (control) film (Fig. 3, A and B). In addition, we lifted off the perovskite layer from the substrate to directly monitor Me-4PACz signals using different codeposition methods. A more pronounced Me-4PACz signal was observed from the buried interface of perovskite in the control sample, whereas a stronger Me-4PACz signal was tracked from the ITO surface in the target sample, both of which reflect the ideal morphology of SAM in the decoupled codeposition strategy (fig. S32).

The lateral distribution of Me-4PACz was also more compact and homogeneous in the target sample. In the cross-sectional images under high-angle annular dark-field scanning transmission electron microscopy (HAADF-STEM) (Fig. 3, C and D), Me-4PACz appeared as a faint, brighter layer between the darker ITO and molybdenum oxide $(\mathrm{MoO_x})$ layers caused by atomic number contrast. Compared with irregular thickness and sparse coverage (with some regions measuring $< 1\mathrm{nm}$ ) in the control samples, Me-4PACz exhibited a continuous coverage and uniform thickness of 1 to $2\mathrm{nm}$ across the whole monitored region in the target samples (41). The lateral uniform anchoring of Me-4PACz on substrate was further corroborated by AFM-IR, tracking from the uniform distribution of characteristic P–C stretching vibration signal of Me-4PACz at 14:18 cm $^{-1}$ (Fig. 3, E and F). The homogeneous Me-4PACz anchoring enhanced hole extraction and suppressed nonradiative recombination (figs. S33 to S37, table S6, and supplementary text section 7). Moreover, uniform Me-4PACz anchoring was achieved across large-area flexible substrates up to 30 cm × 35 cm, demonstrating the scalability of the decoupled codeposition strategy for large-area flexible modules (figs. S38 to S44, table S7, and supplementary text section 8).

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Fig. 3. Perovskite crystallization and SAM release by decoupled codeposition. (A and B) ToF-SIMS depth profiles of control (A) and target (B) perovskite films. The spatial distribution of $PbI^{-}$ , $In^{-}$ , $PO_{2}^{-}$ , and $SO_{2}^{-}$ ions correspond to the distributions of perovskite, ITO, Me-4PACz, and BSAI, respectively. (C and D) Cross-sectional HAADF-STEM images of control (C) and target (D) SAMs between $MoO_{x}$ and PET/ITO. Scale bars, 10 nm. (E and F) AFM-IR mapping at $1418\ cm^{-1}$ (P–C stretching of Me-4PACz) of control-ITO (E) and target-ITO (F). Scale bars, 2 $\mu$ m. (G and H) In situ PL spectra of control (G) and target (H) perovskite films during $N_{2}$ -knife treatment and subsequent annealing. (I and J) In situ synchrotron GIWAXS of control (I) and target (J) perovskite films during annealing.

In addition to assisting robust and compact anchoring of Me-4PACz, the decoupling agent BSAI could also modulate the crystallization kinetics in the target film compared with the control film. From in situ photoluminescence (PL) spectroscopy during slot-die coating, the perovskite growth underwent three stages: First was the prenucleation stage (stage I) dominated by the $Pb_{3}I_{8}\cdot2DMF\cdot2FA$ solvent complex (42), which had a low PL intensity. Second was the intermediate phase nucleation stage (stage II) which started with a steep PL surge at $\sim780$ nm. Upon annealing, the film entered the crystal growth stage (stage III), accompanied by a rapid PL intensity rise and a slight red shift of the peak. Compared with the conventional codeposition, the PL intensity near 700 nm during stage I in the BSAI incorporated decoupled codeposition was clearly reduced, which was evidence of effective suppression of solvent complex formation, likely resulting from the strong interaction of BSAI with Pb–I frameworks. This strong interaction retarded the formation of intermediate phase, thereby delaying the onset of nucleation from 22.1 s in the control codeposition to 30.5 s (Fig. 3, G and H). In addition, the control film exhibited poorer stability under ambient conditions, undergoing gradual decomposition and a corresponding decline in PL intensity (fig. S45) compared with the target films. The retarded perovskite crystallization in the decoupled codeposition was further confirmed by the slower emergence of the absorption edge in the in situ UV–vis absorption spectra (fig. S46 and supplementary text section 9).

The retarded crystallization kinetics ameliorated the perovskite crystallinity in the decoupled codeposition strategy. From the in situ synchrotron-based grazing incidence wide-angle x-ray scattering (GIWAXS) results, the control films contained not only $\delta$ -phase but also $\alpha$ -phase crystallites with varied (001), (011), and (111) orientations during early growth, resulting from the heterogeneous nucleation. After annealing, the $\delta$ -phase and disordered $\alpha$ -phase perovskite domains remained (Fig. 3I). By contrast, the target film showed effective suppression of both the $\delta$ -phase and the $\alpha$ -phase components with (011) and (111) orientations. Instead, a pronounced and gradual growth of the $\alpha$ -phase (001) signal was observed (Fig. 3J and fig. S47), confirming a facet-oriented crystallization in the decoupled codeposition. The more detailed incident-angle dependent GIWAXS measurements further revealed that the BSAI incorporation in the decoupled codeposition facilitated consistently high crystallinity and eliminated impurities across the whole perovskite film (figs. S48 to S52 and supplementary text section 10).

With the ameliorated perovskite crystallinity, we assessed the large-scale horizontal uniformity of the target films. Perovskite layers with the size of $5 \times 5 \, cm^{2}$ , $10 \times 10 \, cm^{2}$ , and $30 \times 35 \, cm^{2}$ were slot-die coated and nine subregions (labeled I through IX) were examined through optical and morphological characterizations (figs. S8, S40, and S53). The PL intensity and absorbance of different subregions vary considerably across the control $25 \, cm^{2}$ film, and the variation became more pronounced in the larger samples ( $100 \, cm^{2}$ and $1050 \, cm^{2}$ ) (Fig. 4A and figs. S54 to S57). By contrast, the target films displayed negligible variations in PL intensity and absorbance across all areas even for the $1050 \, cm^2$ sample (Fig. 4B and figs. S54 to S57). In addition, substantial voids were observed in scanning electron microscopy (SEM) images (fig. S58) at the bottom interface of the control films caused by local nonwettability, whereas the target films showed only dense, pinhole-free microstructures even across the entire $1050 \, cm^2$ area (fig. S59). We observed similar retarded crystallization process and oriented lattice growth in perovskite with only BSAI addition, which implies that the optimization of the perovskite layer mainly came from strong interactions between the decouple agent BSAI and Pb–I framework colloids (fig. S60 and supplementary text section 11).

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Efficiency and stability improvement with the decoupled codeposition strategy

We fabricated flexible PSCs through the BSAI incorporated decoupled codeposition strategy [with the configuration of PET/ITO/perovskite: Me-4PACz/phenethylammonium iodide (PEAI)/C $_{60}$ /2,9-dimethyl-4,7-diphenyl-1,10-phenanthroline (BCP)/copper (Cu)] that demonstrated fast transient photocurrent decay, a prolonged charge-carrier lifetime, a reduced trap density, and minimized nonradiative recombination (fig. S61 and supplementary text section 12). For a small-area (0.0628 cm $^{2}$ ) flexible device fabricated by spin-coating, a record PCE of 26.9% [26.9% certified by TÜV SÜD, 26.9% by Verband Deutscher Elektrotechniker Testing and Certification Institute (VDE), and 26.8% by China Photovoltaic Product Quality Inspection and Testing Center (CPVT)] was achieved with the decoupled codeposition strategy with 0.5 mg mL $^{-1}$

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Fig. 4. Efficiency of flexible PSMs enabled by decoupled codeposition strategy. (A and B) PL intensity mapping of nine regions from control (A) and target (B) perovskite films $(30 \times 35 \, \text{cm}^{2})$ . (C) J-V curves of $0.0628 \, cm^{2}$ flexible PSCs under AM 1.5G illumination $(100 \, \text{mW cm}^{-2})$ . (D) PCE evolution versus year chart of the reported flexible PSCs. The solid and open symbols represent the certified and in-laboratory-measured values, respectively. (E to G) I-V curves of flexible modules with aperture area of $14.55 \, cm^{2}$ (E), $80 \, cm^{2}$ (F), and active area of $750 \, cm^{2}$ (G); insets show module photographs. (H) PCE of flexible PSCs as a function of device area. (I) Certified record PCE statistics of flexible modules in different device areas.

BSAI (Fig. 4, C and D, figs. S62 to S68, tables S8 to S11, supplementary text sections 13 and 14), which outperformed the PCE of 24.5% using the conventional codeposition method.

The high homogeneity of both SAM anchoring and perovskite crystallization also contributed to efficient flexible PSMs. The detailed fabrication process of the flexible PSMs is presented in figs. S69 and S70. The light beam-induced current (LBIC) mapping demonstrated that the target modules with the decoupled codeposition exhibited more homogeneous and stronger external quantum efficiency response across the whole region (fig. S71). Thus, the target mini-module $(5 \times 5 \, \text{cm}^2, \text{aperture area: } 14.55 \, \text{cm}^2)$ using the decoupled codeposition strategy achieved a PCE of 23.1% and stabilized output of 22.6% (certified PCE under reverse scan was 22.3% and certified steady-state PCE is 22.2%, Fig. 4E, figs. S72 and S73, and table S12), which was substantially higher than that of the control flexible submodules (15.3%). The PCEs of the Target flexible PSMs also exhibited superior reproducibility, as evidenced by the notably narrower device-to-device variation distribution (fig. S74). With further upscaling, we fabricated flexible PSMs with an area of $10 \times 10 \, cm^2$ (aperture area: $80 \, cm^2$ ) and $30 \times 35 \, cm^2$ (active area: $750 \, cm^2$ ) based on the decoupled codeposition strategy, and achieved PCEs of 21.0% (20.6% certified) and 20.6% (20.2% certified), respectively (Fig. 4, F and G, figs. S75 and S79, and table S12), whereas the control modules exhibited lower PCEs of only 11.5 and 7.95%. The decoupled codeposition strategy exhibited negligible PCE “scale-up efficiency loss” (Fig. 4H) and delivered record PCEs of commercial-size flexible PSMs (Fig. 4I and table S13).

We further demonstrated the general applicability of the decoupled codeposition strategy to different substrates and SAM molecules. Rigid PSMs with different areas fabricated by the decoupled codeposition achieved PCEs of 24.2% (23.8% certified, 14.55 cm $^{2}$ ), 22.1% (80 cm $^{2}$ ), and 21.6% (750 cm $^{2}$ ), respectively (figs. S80 and S81 and table S14). In addition, flexible PSMs incorporating different SAM molecules, namely [2-(3,6-Dimethoxy-9H-carbazol-9-yl)ethyl]phosphonic acid (MeO-2PACz), [4-(7H-Dibenzo[c,g]carbazol-7-yl)butyl]phosphonic acid (4PADCB), and (4-(2,7-dibromo-9,9-dimethylacridin-10(9H)-yl)butyl)phosphonic acid (DMAcPA), into the perovskite precursor delivered similar PCEs (22.5, 22.6, and 22.8%), underscoring the broad applicability of this approach with different SAMs (fig. S82 and table S15).

To assess the commercial viability of flexible PSMs, we systematically evaluated their operational stability following the standardized International Summit on Organic Solar Cells Stability (ISOS) protocols, including photothermal aging, damp heat exposure and thermal cycling. To minimize the disturbance from passivation for long-term stability evaluation of decoupled codeposition strategy, we replaced PEAI with a more robust passivation molecule 1,3-diaminopropane dihydroiodide (figs. S83 and S84, table S16). As shown in Fig. 5A and table S17, under ISOS-L-3 testing conditions (1-sun illumination at $85^{\circ}$ C with MPPT), the encapsulated target flexible PSMs (5 cm × 5 cm) retained 92.5% of its initial PCE of 22.0% after 1044 hours, whereas the control device maintains only 42.1%.

The decoupled codeposition strategy first realized stable operation of flexible PSM at $85^{\circ}$ C, yet previous stability test results were limited to $<70^{\circ}$ C. (Fig. 5E and table S18). A similar trend was observed for unencapsulated devices under continuous 1-sun illumination at $85^{\circ}$ C in a $N_{2}$ atmosphere (fig. S85). The target device retained 91.8% of its initial efficiency after 900 hours, compared with only 43.0% for the control device, which confirms that the decoupled codeposition strategy significantly improves the intrinsic operational stability of flexible modules. During the damp heat test ( $85^{\circ}$ C and 85% RH, ISOS-D-3), the target modules maintained 94.6% of their initial PCE after 1050 hours, whereas the control modules degraded to 62.9% (Fig. 5B, fig. S86A, and table S17). In the thermal cycling test between $-40^{\circ}$ C and $+85^{\circ}$ C (ISOST-3), the target modules retained 95.1% of their initial performance after 200 cycles, whereas the control modules substantially degraded, with PCE decreasing to 51.5% of the initial value (Fig. 5C, fig. S86B, and table S17).

We attributed enhanced stability to two main factors. First, the decoupling agent inhibited interaction between perovskite and Me-4PACz and promoted complete anchoring of Me-4PACz to substrate, which suppressed deleterious reactions between phosphonic acid groups and perovskites under high humidity, elevated temperature, and illumination (figs. S87 to S94, supplementary text sections 15 and 16) (43). Second, the presence of electron-deficient In/Sn surface sites on PET/ITO facilitated Me-4PACz anchoring in strong tridentate binding mode, thereby further enhancing the anchoring stability (figs. S95 to S98, table S19, and supplementary text section 17).

The mechanical durability of the flexible modules was also evaluated by cyclic bending at a radius of 10 mm (1% strain, axis $\perp$ current flow) (figs. S99 and S100, table S20, and supplementary text section 18). After 10,000 bending cycles, the target modules retained 92.1% of their initial PCE, whereas the control modules preserved only 75.5%. We attributed this enhanced mechanical durability to the strengthened SAM/perovskite interface that formed from the dense and pinhole-free bottom surface of the perovskite film, which minimized internal free surfaces and thereby suppressing crack initiation and propagation along the buried interface under cyclic shear stress (figs. S101 to S105, table S21, and supplementary text section 19).

To evaluate the operational robustness under combined complex aging conditions, our PSMs were submitted to the Technical Inspection Association TÜV SÜD, where they successfully completed all required tests in accordance with IEC TS 63163:2021 (an international commercialization assessment standard for flexible portable photovoltaic modules, figs. S106 and S107, table S17, and supplementary text section 20). Additionally, the rigid perovskite modules fabricated with the decoupled codeposition strategy retained \~97.4% PCE after 2520 hours of aging according to ISOS-L-3 protocol after encapsulation, whereas the control device PCE decayed to \~63.3% (Fig. 5D and table S17). The operational lifetime of rigid modules further validated the ability to enhance stability of decoupled codeposition strategy (Fig. 5F and table S22).

We demonstrate real-world applications of high-efficiency flexible perovskite modules in two critical scenarios: portable chargers and RC-UAVs, showcasing technology readiness near commercial maturity. The flexible PSMs used in these demonstrations weighed only 20.31 g (equivalent to four sheets of A4 paper; see movie S1). The portable PSMs generated 20.5 W of electricity under clear weather (with irradiance of $1058 \, W m^{-2}$ ) and maintained an output of 12.1 W on cloudy late afternoons (with irradiance of $635 \, W m^{-2}$ ), fully meeting charging demands of personal electronics (Fig. 5G and movie S2). Laminating flexible PSMs onto the aerodynamically designed curved wings of an RC UAV increased the total weight by $\sim8\%$ . However, it extended the flight endurance from 8 to 19 min and expanded the flight range from $\sim4$ to $\sim9.5 \, km$ . This enhancement substantially increased the flying scope of the RC UAV without compromising its flight altitude or balance (Fig. 5H, figs. S108 and S109, movie S3, and supplementary text section 21).

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Discussion

We developed a decoupled codeposition strategy by incorporating BSAI as a tailored modulator in the conventional SAM-perovskite codeposition precursor solution. The strong interaction between BSAI and perovskite precursor impedes interaction between Me-4PACz and perovskite, facilitating rapid and efficient Me-4PACz anchoring on the PET/ITO electrode, as well as high-quality perovskite film growth, which addressed both the challenges of achieving homogeneous and compact SAM/perovskite stack layers over large areas on flexible substrates. This decoupled codeposition strategy contributed to a record PCE of 26.9% (26.9% certified by TÜV SÜD, 26.9% by VDE, and 26.8% by CPVT) for small-area flexible PSCs, while PCEs of 23.1% (22.3% certified), 21.0% (20.6% certified), and 20.6% (20.2% certified) are achieved on flexible PSMs with substrate areas of 25, 100, and 1050 cm $^{2}$ (active areas of 14.55, 80, and 750 cm $^{2}$ ), respectively. The resulting flexible PSMs (device area 14.55 cm $^{2}$ ) retained >92% of their initial efficiencies (22.0%) after \~1000 hours of MPPT at 85°C. Moreover, the commercial-scale flexible PSMs (device area 900 cm $^{2}$ ; PCE 19.9%) successfully passed all sequences of the IEC TS 63163:2021 reliability tests, as certified by TÜV SÜD. The rigid PSMs also remained >97% PCE after \~2500 hours aging under the same conditions, underscoring the universality of the decoupled codeposition strategy. Our work provides a mechanistic understanding at the molecular level of the competitive interplay between SAM anchoring and perovskite crystallization and offers an effective and feasible regulatory strategy for efficient commercial-scale flexible PSMs.

C

B

E

D

G

Fig. 5. Stability and real-world applications of flexible perovskite modules. (A) PCE evolution of encapsulated flexible PSMs (aperture area of $14.55 \, cm^2$ ) when operating under 1-sun full spectrum illumination and MPPT at $85^\circ C$ and $\sim65\%$ RH (ISOS-L-3). (B) PCE evolution of encapsulated flexible PSMs (aperture area of $14.55 \, cm^2$ ) when heated under $85^\circ C$ and $85\%$ RH (ISOS-D-3). (C) Thermal cycling aging from $-40^\circ C$ to $+85^\circ C$ under dark (ISOS-T-3). (D) PCE evolution of encapsulated rigid PSMs (aperture area of $14.55 \, cm^2$ ) when operating under 1-sun full spectrum illumination and MPPT at $85^\circ C$ and $\sim65\%$ RH (ISOS-L-3). (E) MPPT stability ( $T_{90}$ ) versus test temperature chart of the reported flexible PSCs and PSMs. (F) MPPT stability (PCE maintained at $85^\circ C$ ) versus lifetime chart of the reported rigid PSMs. (G) Portable charging performance and real-time power output of flexible PSMs from 18 to 24 November 2025; deep blue dots indicate irradiance. (H) Power output of RC-UAVs integrated with flexible PSMs from 22 to 28 November 2025; dark blue dots indicate irradiance.

The SM presents additional information supporting the conclusions of this work, including materials and methods, 21 sections of supplementary text, 109 supplementary figures, 22 supplementary tables, four dynamic movies, and additional cited references. Collectively, these contents corroborate the experimental observations and validate the mechanistic framework proposed in the main text.

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ACKNOWLEDGMENTS

This work was supported by the Priority Academic Program Development of Jiangsu Higher Education Institutions (PAPD), Collaborative Innovation Center of Suzhou Nano Science and Technology, and the Key Laboratory of Polymeric Materials Design and Synthesis for Biomedical Function, Soochow University, and Laboratory of Flexible Electronics Technology, Tsinghua University. The authors are grateful for the technical support for Nano-X from Suzhou Institute of Nano-Tech and Nano-Bionics, Chinese Academy of Sciences (SINANO). We gratefully acknowledge the support from Shanghai Synchrotron Radiation Facility (SSRF) for use of the BL14B beamline. Funding: This work was supported by the following: National Natural Science Foundation of China (grants 52325307 and 52273188 to Y.W.L.); National Natural Science Foundation of China (grant 52573207 to G.Y.X.); National Key Research and Development Program (2024YFF1401103 to Y.W.L.); Suzhou Key Core Technologies project (SYG2024146 to Y.W.L.); the Key R&D and Achievement Transformation Plan Project of Inner Mongolia Autonomous Region (2025YFHH0021 to Y.W.L.); the Science and Technology Major Project of Jiangsu Province (BG2025024 to Y.W.L.); Natural Science Foundation of the Jiangsu Higher Education Institutions of China (25KJB480012 to G.Y.X.) Author contributions: Conceptualization: Y.W.L. Methodology: Y.W.L., G.Y.X., Y.J.C., C.X.G., W.J.C., H.Y.C., and Q.R.C. Investigation: Y.W.L., G.Y.X., Y.Y.W., X.K.Z., Y.X.S., Q.M., J.Y.D., Y.Y., W.L., X.X.W., Z.Y.C., K.Q.C., and W.W.K. Visualization: Y.W.L., G.Y.X., and Y.Y.W. Funding acquisition: Y.W.L. Project administration: Y.W.L. Supervision: Y.W.L. and G.Y.X. Writing - original draft: Y.W.L., G.Y.X., Y.Y.W., and T.K.Z. Writing - review & editing: Y.W.L., G.Y.X., Y.Y.W., T.K.Z., F.G., and Y.F.L. Competing interests: Y.W.L., G.Y.X., Y.Y.W., and Y.F.L. are inventors on a patent application related to this work filed by Soochow University. The remaining authors declare no competing interests. Data, code, and materials availability: All data needed to evaluate the conclusions in the study are available in the main text or the SM. Source data and key quantitative analyses are available at Zenodo (44). License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/content/page/science-licenses-journal-article-reuse

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.aef9745

Materials and Methods; Supplementary Text; Figs. S1 to S109; Tables S1 to S22; References (45–110); Movies S1 to S4

Submitted 30 January 2026; resubmitted 31 May 2026; accepted 28 August 2026

10.1126/science.aef9745

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The Virtual Biotech: A multi-agent AI framework for therapeutic discovery and development

Harrison G. Zhang\*, Peter Eckmann, Jiacheng Miao, Andrew B. Mahon, James Zou\*

Full article and list of author affiliations: https://doi.org/10.1126/science.aeg6779

INTRODUCTION: Drug discovery requires integrating evidence across biological scales and data modalities to make a sequence of complex decisions, from target prioritization to clinical development. The relevant data, tools, and expertise remain fragmented across organizations and siloed workflows. Overcoming this fragmentation requires not just individual artificial intelligence (AI) models, but holistic systems that can organize specialized expertise, tools, and data into coordinated therapeutic decision-making.

RATIONALE: AI agents are language models equipped with tools and databases that can autonomously perform multistep analyses. We introduce the Virtual Biotech, a multi-agent organization modeled on a drug-development company, with agentic divisions spanning target discovery, safety assessment, modality selection, and clinical development. A virtual chief scientific officer interprets scientific questions, delegates analyses to domain-specialized scientist agents, and synthesizes their findings. The system provides access to more than 100 specialized tools covering 78,726 targets and 39,530 diseases, enabling in-depth and nuanced primary data analysis. A scientific reviewer critiques analyses before evidence synthesis, and analysis artifacts are retained for transparency and reproducibility. We applied the Virtual Biotech to three early-development decision points: target prioritization, modality selection, and analysis of clinical translation failures.

RESULTS: First, the Virtual Biotech autonomously annotated and analyzed clinical trial outcomes to identify transcriptomic features of drug targets associated with trial success. More than 37,000 agents curated structured trial outcomes. Across 55,984 trials, the Virtual Biotech found that drugs targeting cell type-specific genes were $40\%$ more likely to progress from phase 1 to phase 2 and $48\%$ more likely

A multi-agent AI system for therapeutic research. The Virtual Biotech is coordinated by a virtual chief scientific officer (center) that directs domain-specialized AI agents to perform analyses across early drug discovery. In three case studies, the Virtual Biotech conducted multistep investigations spanning target prioritization, target validation and modality selection, and analysis of clinical translation failures.

to reach market, while exhibiting 32% lower adverse event rates. These associations persisted after accounting for genetic evidence, suggesting that single-cell features provide information complementary to genetics for target prioritization. Second, the Virtual Biotech evaluated B7-H3 as a lung cancer target, integrating statistical genetics, single-cell, spatial, and clinicogenomic data. The agents localized B7-H3 overexpression to cancer-associated fibroblasts, linked B7-H3-high regions to immune exclusion and worse survival, and proposed an antibody-drug conjugate strategy. Third, the system analyzed a terminated ulcerative colitis trial targeting oncostatin M receptor (OSMR). Longitudinal single-cell analyses suggested that OSMR was not the dominant driver of the pathway the antibody was intended to block because related receptors converge on the same signaling pathway. Across all case studies, the Virtual Biotech outperformed three state-of-the-art agentic systems, producing more accurate trial annotations and more biologically meaningful conclusions from diverse data modalities. Human experts reimplemented core analyses, confirming the agent conclusions and code correctness.

CONCLUSION: The Virtual Biotech demonstrates that an organized system of AI agents can carry out integrative and multimodal reasoning for early therapeutic development at a scale difficult for human-only teams. By systematically bringing diverse evidence to bear on therapeutic decisions, while keeping human scientists in the loop, it can help identify opportunities and support more informed development choices. □

\*Corresponding author. Email: hgzhang@stanford.edu (H.G.Z.); jamesz@stanford.edu (J.Z.) Cite this article as H. G. Zhang et al., Science 394, eaeg6779 (2026). DOI: 10.1126/science.aeg6779

Target Prioritization

Target Validation & Modality Selection

Clinical Translation

Failure Analysis

ARTIFICIAL INTELLIGENCE

The Virtual Biotech: A multi-agent AI framework for therapeutic discovery and development

Harrison G. Zhang $^{1*}$ , Peter Eckmann $^{2}$ , Jiacheng Miao $^{1,3}$ , Andrew B. Mahon $^{4}$ , James Zou $^{1,2*}$

Drug development requires evidence integration across biological scales and modalities, but relevant tools are fragmented. We introduce the Virtual Biotech, an organization of artificial intelligence (AI) agents modeled on a drug-development company, with agentic divisions spanning target discovery, safety assessment, modality selection, and clinical development. We demonstrate its utility at three drug-development decision points. First, more than 37,000 agents annotated outcomes from 55,984 trials and found that drugs targeting cell type-specific genes were 48% more likely to reach market with 32% fewer adverse events. Second, it integrated multimodal evidence to propose a therapeutic strategy in lung cancer. Third, it analyzed a terminated ulcerative colitis trial and inferred potential mechanisms of failure. These results demonstrate that human-guided multi-agent systems can conduct transparent, multiscale analyses to inform therapeutic-development decisions.

Drug discovery is one of the most consequential and challenging endeavors in biomedicine. Bringing a therapeutic from concept to clinic often requires more than a decade of development and costs on the order of billions of dollars (1-3). Despite these investments, \~90% of drug candidates entering phase 1 trials never reach approval, with failures most often driven by insufficient efficacy and safety liabilities (4-7). To reduce this attrition, modern drug discovery increasingly draws on evidence from diverse sources to validate targets, including but not limited to human genetics, functional genomics, single-cell and spatial profiling, structural biology, medicinal chemistry, and clinical medicine (8).

Organizational and scientific bottlenecks have limited the proper use of this evidence in practice. The expertise to collect and analyze it is fragmented across disciplines, formats, and biological scales, producing siloed workflows (3, 9, 10). Additionally, weighing disparate and sometimes conflicting evidence is difficult, particularly when organizational dynamics or differing prior beliefs shape decisions (3, 9). Fragmented teams also document their workflows differently, making findings hard to audit and decisions hard to reconstruct (3, 11, 12). Further, the recent explosion in the scale of biological data renders manual integration across modalities more difficult (3, 9). Thus, despite advances in data-driven approaches, early-stage drug development remains slow, resource intensive, and prone to failure (1-7).

Artificial intelligence (AI) agents have been proposed to accelerate scientific tasks that involve extensive data analysis, as they are language models equipped with tools and databases that enable them to autonomously carry out complex multistep tasks. Specifying a role and providing domain-specific tools, such as bioinformatics software, specializes an agent for a class of tasks. Recent work also explores multi-agent systems, where multiple specialized agents collaborate to solve complex problems (13).

Here, we introduce the Virtual Biotech, a multi-agent AI research platform that retrieves, analyzes, and integrates multimodal evidence to answer scientific questions in early-stage human therapeutic discovery. A virtual chief scientific officer (CSO) orchestrator breaks down queries into manageable subtasks, directs them to specialized AI scientist agents, and reasons about their results. This structured collaboration encourages deep data-driven analyses of primary evidence and allows for weighing of disparate sources of evidence using a unified reasoning layer to arrive at nuanced conclusions.

Agentic systems have already shown promise in scientific domains such as chemistry and AI research automation (14–17). In biomedicine, agentic methods tailored to specific workflows have emerged, with applications such as gene editing, spatial and single-cell omics, rare disease diagnosis, and nanobody design (18–22). Recent work expanded the domain of agentic reasoning by incorporating a wider range of tools, databases, and code execution workflows for general-purpose data analysis (23–28). Nonetheless, these frameworks largely concentrate on biological data analysis and are typically governed by a single agent. In comparison, the Virtual Biotech is a multi-agent system explicitly designed for translational reasoning across the entire human therapeutic R&D pipeline. By coordinating analysis over the large scale and complexity of drug discovery data, the system can answer scientific questions with holistic, data-driven reasoning.

We first describe the Virtual Biotech tool environment and multi-agent orchestration. We then present three translational case studies that demonstrate how the Virtual Biotech can generate evidence for key decision points in early therapeutic discovery and development. The first case study focuses on large-scale target prioritization by connecting target-level molecular characteristics to clinical-trial outcomes. The second examines drug target B7-H3 in lung cancer from the angle of target validation and modality selection. The third investigates a discontinued oncostatin M receptor (OSMR) ulcerative colitis trial to infer possible reasons for clinical translation failure and to outline biomarker-driven strategies for clinical development.

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Results

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Overview of the Virtual Biotech

The Virtual Biotech emulates a cross-functional therapeutic research organization. It consists of four divisions of scientist agents that address key steps of the drug discovery pipeline (Fig. 1A and table S1). Domain-specialized scientist agents in each division have complementary expertise and domain-specific tools that allow them to query, analyze, and integrate biomedical information across the translational spectrum for evidence-based assessments of drug discovery questions (see Materials and methods for details).

We created domain-specific model context protocol (MCP) servers to provide a unified programmatic interface to major biomedical databases and knowledge sources, abstracting the complexity of heterogeneous data formats and query APIs (application programming interfaces) into standardized tools (Fig. 1B and supplementary text I) (29–31). Each scientist agent accesses curated, expertise-aligned MCP tools to gather evidence from relevant sources, transforming static databases into interactive knowledge layers that agents dynamically analyze in response to user questions.

We developed specialized MCPs that provide Virtual Biotech scientist agents with >100 analytical tools to interrogate large-scale, heterogeneous biomedical data spanning 78,726 targets, 39,530 diseases, 14.5 million protein–protein interactions, >3 million credible genetic sets, and >100 million single-cell profiles (32, 33). The platform further integrates chemoinformatics and pharmacology resources covering 18,119 drugs, 6332 distinct mechanisms of action, 114,270 US Food and Drug Administration (FDA) adverse event reports,

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Fig. 1. Overview of the Virtual Biotech AI agents, tools, and orchestration procedure. (A) The multi-agent AI system organization and scientific divisions. (B) Overview of model context protocol (MCP) servers, grouped by domain area, which provide customized tools to query and analyze diverse biological and clinical data sources. (C) The workflow of the Virtual Biotech. In response to a user query, the virtual CSO first asks any relevant follow-up questions to clarify user intent before doing expensive analyses. In parallel, the chief of staff agent prepares a briefing on the topic with recent developments, data availability, and general field context. The virtual CSO then coordinates divisions of specialized scientist agents to perform analyses to answer the user's query. Next, the scientific reviewer agent evaluates the methodology and claims from scientist agents, and upon reviewing the feedback, the CSO either coordinates revised analyses with scientist agents or synthesizes the evidence into a report.

32,783 pharmacogenomic variants, and drug perturbation expression measurements from Tahoe-100M (34). In addition, ClinicalTrials.gov records are accessible through our MCP (35). Scientist agents can further query biomedical literature through PubMed and retrieve additional targeted datasets via web-based tools. These resources are largely human-focused and thus support target-centered queries in human diseases represented by the data.

We developed a user interface for the Virtual Biotech that displays the agents' reasoning process, indicates which tools are currently in use, and allows users to download the corresponding data, reproducible code, and reports generated during each session (fig. S1).

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Virtual Biotech orchestration

Upon receiving a user's query and before initiating scientist work, the virtual CSO initiates its own strategic orientation (Fig. 1C and supplementary text II). Its chief of staff agent first generates a briefing on general field awareness, data landscape, and recent developments, to help the virtual CSO frame the analysis, set proper feasibility expectations for the user, and identify key questions. In parallel, the virtual CSO interviews the user to clarify the intent of the user and increase the alignment of human-AI collaboration (36, 37). Once briefed, the virtual CSO routes tasks to relevant scientist agents (Fig. 1C).

After the scientist agents complete their analyses, the scientific reviewer agent evaluates their outputs to understand how well they address the user's original question, the strength of the evidence supporting their conclusions, and the overall thoroughness of the analysis (Fig. 1C and supplementary text III). If gaps or unsubstantiated claims are identified by the scientific reviewer agent, the CSO redelegates to relevant scientist agents for iterative refinement.

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Target prioritization: Virtual Biotech connects preclinical biology with clinical outcomes to identify drug target features associated with trial success

Drug discovery programs face substantial attrition, with lack of efficacy and safety concerns accounting for \~79% of clinical trial failures $(38)$ . Prior target prioritization work established that targets supported by human genetic evidence are much more likely to progress through clinical development $(39-41)$ . To expand on these results for better target prioritization, we provided Virtual Biotech with this earlier work and instructed the system to critically evaluate its own infrastructure and recommend directions to expand this analysis $(40)$ . The virtual CSO used its clinical trialist agent to enrich the 55,984-trial Open Targets clinical trial dataset with additional outcome annotations. It also proposed using its single-cell agent to design genomic features for association testing with trial outcomes, following Razuvayevskaya et al. $(33, 40, 42)$ . Agent-based outcome annotation was necessary because the original Open Targets dataset lacked endpoint data and ClinicalTrials.gov records often provide incomplete, inconsistent, or free-text-only outcomes $(43, 44)$ . Agent curation was therefore needed to standardize outcomes and recover missing or conflicting data from sources such as publications and press releases.

Massively parallel, source-tracked extraction of trial outcomes: The clinical trialist agent proposed key outcome variables for large-scale extraction, including trial-phase progression, primary and secondary endpoint results, and adverse event rates. It developed a systematic protocol to obtain trial results from sources such as publications and press releases. The workflow began with a human user instructing the virtual CSO to curate clinical trial outcomes for phase 2 and 3 trials in the Open Targets dataset. The virtual CSO translated this goal into a distributed extraction task and delegated protocol design to a clinical trialist agent, which specified the required outcome fields, evidence hierarchy, and source-tracking requirements. The virtual CSO then dispatched 37,075 clinical trialist agents in parallel, with one agent assigned to each National Clinical Trial identifier (NCT ID) (Fig. 2A). At this scale, comprehensive curation is impractical without parallelization, necessitating a multi-agent architecture capable of executing data curation in a distributed manner.

Each clinical trialist agent followed a three-tier evidence cascade for its assigned NCT ID: It first systematically queried the ClinicalTrials.gov database, then searched PubMed for publications containing trial results when primary data were incomplete, and finally consulted online press releases and regulatory announcements (Fig. 2A and supplementary text IV) (35). Agents recorded the source of information for each annotation. The median per-trial cost was \$0.23 in Anthropic API fees. For phase 1 trials, success was algorithmically defined as progression to phase 2, because phase 1 trials assess safety and dosing rather than efficacy.

To assess annotation quality, manual review of 100 randomly selected clinical trials was performed and agreement with agent annotations was 88.4% for primary endpoints (76 out of 86 applicable trials), 88.4% for secondary endpoints (76 out of 86), and 92.4% for adverse event rates (61 out of 66 reporting exact statistics). Furthermore, agreement was 85.6% for primary endpoints across 7666 trials overlapping with the manually curated Therapeutic Data Commons (TDC) Trial Outcome Prediction dataset (see Materials and methods for more details) $(45)$ . These agreement metrics demonstrated that the agent annotated trials reliably and that the resulting labels were suitable for analyses.

Translational feature engineering with single-cell atlases: To derive single-cell expression features of drug targets, the single-cell agent proposed and implemented a comprehensive feature extraction framework for Tabula Sapiens, a healthy human reference atlas of 27 tissues (46). The agent designed features organized into two categories: cell-type specificity metrics and expression heterogeneity measures. For specificity, the agent proposed the tau cell-type specificity index, where values approaching zero indicate ubiquitous expression whereas values approaching one indicate expression restricted to a single cell type (47). To capture expression heterogeneity within cell populations, the agent proposed a bimodality coefficient calculated from the skewness and kurtosis of expression distributions among expressing cells, where higher values may indicate “on/off” expression patterns within a tissue (48, 49). Various measures of bimodality have been proposed for gene expression analysis, but this specific bimodality coefficient, originally developed in psychology and social sciences, is an underexplored and interpretable metric for gene expression bimodality (50–55). These two features were moderately correlated (Pearson $\rho = 0.54$ ), suggesting that they provide some complementary information.

Virtual Biotech–driven analysis reveals genomic features associated with trial success: The final integrated dataset comprised 55,984 clinical trials spanning phase 1 (n = 14,237), phase 2 (n = 22,164), phase 3 (n = 14,911), and phase 4 (n = 4672) (Fig. 2B). Trial-level outcome annotations were linked to target-level molecular features extracted by the Virtual Biotech and to genetic evidence scores from Open Targets.

The clinical trialist agent first successfully replicated the genetic evidence results reported by Razuvayevskaya et al., finding that genetic support is associated with trial progression and also protective of early trial stoppage (fig. S2A) (40). Using the additional trial outcomes curated by the Virtual Biotech, it also found that trials that achieved primary endpoints and showed lower adverse events were enriched with genetic evidence (fig. S2, A and B). Following the approach from the analogous study on genetic evidence, the clinical trialist agent then evaluated the association between single-cell transcriptomic features of drug targets and trial outcomes (39, 40).

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B

Fig. 2. Large-scale clinical trial data extraction using the Virtual Biotech. (A) Overview of the data extraction and curation process. For each National Clinical Trial (NCT) ID, the clinical trialist agent uses tool calls to ClinicalTrials.gov, PubMed, and the web to gather information about the trial. After reasoning about its findings, the agent enters information into a structured JSON ontology for downstream analysis. (B) Sankey plot of the curated clinical trial dataset (n = 55,984) showing trial phase, trial status, and outcomes.

Both tau cell-type specificity and expression bimodality score were associated with trial progression through clinical development phases (Fig. 3A). Following binarization of targets based on their tau metric into cell type-specific versus broadly expressed classes (see Materials and methods for details), the clinical trialist agent found that drugs acting on cell type-specific targets were 48% more likely to ever reach phase 4.

Targets with higher cell-type specificity were more likely to meet defined primary endpoints [odds ratio (OR) = 1.12; 95% confidence interval (CI): 1.09–1.14], secondary endpoints (OR = 1.12; 95% CI: 1.09–1.14), and successful phase 1 to phase 2 progression (OR = 1.27; 95% CI: 1.22–1.33) (Fig. 3A). Drugs with cell type-specific targets were 40% more likely to progress from phase 1 to phase 2. Similarly, targets with a higher expression bimodality score were more likely to achieve a positive primary endpoint, a positive secondary endpoint, and successful phase 1 to phase 2 progression (Fig. 3A).

The Virtual Biotech further found that trials with targets that have a higher cell-type specificity and expression bimodality score reported lower adverse event rates across many organ systems (Fig. 3B). Trials testing cell type-specific targets had on average $32\%$ lower adverse event rates. This suggested that targets with more heterogeneous and cell type-restricted expression patterns may offer improved safety profiles.

Next, we demonstrated that these findings are robust to confounders. To assess whether the observed associations could arise by chance or through confounding in the complex trial-to-target mapping, we performed permutation testing >1000 iterations, confirming that all findings remained statistically significant (permutation P < 0.05) against the empirical permuted null (fig. S3, A and B). To control for potential confounding between disease indications and between drug modalities, we further estimated ORs using mixed-effects models adjusted for trial phase and enrollment year, with drug modality and disease indication area as random effects. The adjusted odds ratios for cell-type specificity and expression bimodality score remained statistically significant across mixed-effects models (fig. S3, C and D).

Another key question is whether single-cell transcriptomic features of targets provide independent value beyond established human genetic evidence linking targets to disease. Therefore, we replicated our findings adjusting for genetic evidence. After adjustment, the associations between trial outcomes and each of the two single-cell features—cell-type specificity and expression bimodality score—remained statistically significant with negligible reductions in effect sizes (fig. S4, A and B). We further estimated ORs for single-cell features among trials with no genetic evidence (75% of trials) and found that single-cell features had similar or even stronger effect sizes in this subset (fig. S4, C and D). Together, these results indicated that single-cell information captures additional biological signal associated with clinical trial outcomes beyond genetic evidence alone. A recent report by Dann et al. similarly found that cell type-restricted targets were associated with phase progression but did not study association with endpoints or adverse events $(56)$ .

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Target validation and modality selection: Virtual Biotech research builds preclinical rationale for B7-H3 antibody-drug conjugate development in lung cancers

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We next investigated a common drug program-level decision point: whether multimodal evidence can support a coherent therapeutic hypothesis and modality choice for a nominated target in a given disease context. To demonstrate the Virtual Biotech's capacity to rapidly generate rigorous evidence to support this task, we prompted the system to assess the therapeutic potential of B7-H3 (also known as CD276) in lung adenocarcinoma (LUAD) and small cell lung cancer (SCLC). B7-H3 is a transmembrane immune checkpoint protein that is highly expressed in solid tumors, including lung cancers $57$ . Its receptor is unknown, and its role in cancer remains unclear, though it likely has both immunologic and nonimmunologic functions $58$ . The user's initial query was: "Evaluate the therapeutic candidacy of B7-H3 as a target in lung cancer." The virtual CSO interpreted this as a therapeutic target evaluation task and decomposed it into a set of evidence-generation modules spanning human genetics, target biology, single-cell transcriptomics, spatial transcriptomics, biomarker-stratified survival analyses, and prior clinical trial data.

The statistical genetics agent first evaluated germline genetic support for B7-H3 as a lung cancer target. No significant associations or credible sets were identified at the B7-H3 locus for lung cancer, and the agent concluded that germline genetic evidence for B7-H3 as a lung cancer target was weak (Fig. 4A). Despite this, the virtual CSO correctly interpreted the absence of genome-wide association study (GWAS) signal as nondisqualifying, noting that for potential immune checkpoint targets, therapeutic rationale can derive from somatic tumor overexpression rather than germline risk variants. This reasoning distinguished B7-H3 from targets where genetic evidence is essential for

B

Fig. 3. Preclinical single-cell atlas features of drug targets significantly associated with key clinical trial outcomes. (A) Associations between single cell-derived features of the drug target and phase progression, trial stoppage, and efficacy outcomes. Plot shows the standardized odds ratio (all features normalized to have a standard deviation of 1) with 95% CIs. (B) Associations between single cell-derived features and serious adverse event rates grouped by organ system. Forest plot shows beta regression coefficients with 95% CIs.

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"Evaluating B7-H3 (CD276) therapeutic potential in lung cancer...

B

\- No B7-H3 variants or credible sets identified across four population-level lung cancer GWAS.

\- No machine learning locus-to-gene causal predictions identified.

\- Genetic constraint showed predicted LoF observed/expected ratio of 0.67, indicating moderate LoF tolerance.

\- ENCODE E2G identified high-confidence regulatory regions at the B7-H3 locus in normal lung, supporting strong regulatory activity.

\- Limited germline evidence does NOT invalidate therapeutic potential. Rationale may derive from somatic tumor overexpression rather than inherited risk.

Proceeding to expression-based analyses."

C

"Tumor-enriched B7-H3 expression for both LUAD and SCLC is strongest in cancer-associated fibroblasts (CAFs), not malignant cells.

A next step is understanding how cell-cell communication is disrupted and what signals B7-H3+ CAFs send to immune cells. This bridges the gap between knowing which cells express B7-H3 and understanding their function."

E

"Analysis of Visium LUAD spatial transcriptomics suggests that B7-H3 expression contributes to a immune-excluded niche. Mixed-effects modeling showed reduced immune cell abundance around high B7-H3 expression spots relative to low B7-H3 spots. This provides spatial validation for the immunosuppressive ligand-receptor interactions identified.

I want to understand whether this immunosuppressive phenotype translates into clinically meaningful survival differences."

validation, prompting the virtual CSO to instruct its single-cell agent to perform analyses for more clarity.

The single-cell agent queried and downloaded single-cell atlases from CELLxGENE Census, comprising 62,341 cells from 9 donors in the SCLC atlas, 337,002 cells from 69 donors in the LUAD atlas, and 86,478 cells from lung tissue of 26 healthy donors (Fig. 4B) (59). The agent conducted cell type-resolved differential expression analysis with pseudobulk aggregation, revealing that B7-H3 up-regulation was not uniform across all cell types but concentrated in fibroblasts in both SCLC $\left[\log_{2}\text{ fold change (log2FC)} = 2.13, \text{ false discovery rate (FDR) adjusted P value} = 3.5\ 10^{-9}\right)$ and LUAD ( $\log_{2}FC = 1.79, FDR P value = 2.0 \times 10^{-8}$ ) (Fig. 4C).

F

"Querying CELLxGENE Census for LUAD, SCLC, and healthy lung atlases to characterize B7-H3 expression at single cell resolution. Performing QC, correcting for batch effects with Harmony, visualizing atlases with UMAP."

"B7-H3+ fibroblasts show a immunosuppressive program.

Let's analyze spatial transcriptomics next to validate whether these predicted immunosuppressive interactions translate into a physical immune exclusion phenotype."

"B7-H3 seems to be a potential prognostic biomarker in NSCLC. With the spatial evidence of immune exclusion, these results support the hypothesis that B7-H3-mediated immunosuppression contributes to adverse clinical outcomes—providing a mechanistic and clinical rationale for therapeutic targeting of B7-H3 in lung cancer"

Fig. 4. Virtual Biotech evaluates B7-H3 (CD276) as a therapeutic target in lung cancer. (A) Summary from statistical genetics agent of germline genetic findings for B7-H3 in lung cancer. (B) UMAP of lung adenocarcinoma (LUAD) and small cell lung cancer (SCLC) single-cell atlases prepared by the single-cell atlas agent. (C) Differential expression analysis of B7-H3 by cell type identified significantly increased expression in fibroblasts. (D) Ensemble cell-cell communication inference by the single-cell agent revealed distinct signaling pathways found in B7-H3+ cancer-associated fibroblasts in SCLC (shown here) and LUAD (fig. S5). (E) Spatial transcriptomic analyses of LUAD primary-site tissue identifies immune-excluded niches in the top quartile of B7-H3-expressing spots relative to the bottom quartile of B7-H3-expressing spots. Bar plot quantifies the percent change (95% bootstrap CI over 10,000 resamples) in neighbor immune abundance between top and bottom quartile of B7-H3-expressing spots across 12 LUAD tumor samples. Statistical significance was assessed using a linear mixed-effects model adjusted for focal-spot total UMI count, fibroblast abundance, malignant epithelial abundance, and endothelial abundance as fixed effects with nested random effects for patient and sample within patient ( $P < 0.01$ , $*P < 0.001$ ). (F) Survival analysis of the lung adenocarcinoma cohort from The Cancer Genome Atlas project identifies B7-H3 as a potential prognostic biomarker of disease-free survival.

On the basis of these findings, the single-cell agent hypothesized that B7-H3-high fibroblast cells might actively shape an immunosuppressive tumor microenvironment (TME). It then performed a ligand-receptor interaction analysis to identify differences in signaling between fibroblasts whose B7-H3 expression fell within the highest versus lowest quartiles of the cell population (60). This identified 180 significant interactions in SCLC and 226 interactions in LUAD (see Materials and methods for details) that were specific to B7-H3-high fibroblasts communicating with immune cells (Fig. 4D and fig. S5A). The single-cell agent identified five main signaling groups: sheddases that release activating ligands from immune cell surfaces, myeloid-reprogramming mediators that polarize macrophages toward immunosuppressive states, proangiogenic factors that remodel tumor vasculature, immunosuppressive cytokines that engage inhibitory receptors, and chemokine pathways that retain immune cells in the fibroblast niche. These results suggest that B7-H3-high stromal cells may use additional immunomodulatory mechanisms beyond B7-H3's canonical checkpoint function.

The scientific reviewer agent was then dispatched and noted that the ligand-receptor analysis inferred cell-cell communication from dissociated single-cell data that lost spatial tissue context. Thus, the virtual CSO reasoned that spatial profiling was needed to verify whether these predicted immunosuppressive interactions corresponded to a physical immune exclusion phenotype. It then dispatched the single-cell agent to analyze a Visium dataset comprising 12 lung tissue samples from patients diagnosed with LUAD, totaling over 25,000 spatially resolved spots (61). To infer spot-level cell-type abundances, the single-cell agent applied Cell2Location using the prior LUAD single-cell atlas as reference (fig. S5B) (62). It then implemented a mixed-effects regression model to assess whether spots expressing B7-H3 in the top quartile showed altered immune cell compositions within their immediate spatial neighborhood relative to the bottom quartile. B7-H3-high spots exhibited lower abundance of neighboring immune cells such as T cells, macrophages, monocytes, and dendritic cells (Fig. 4E). Notably, these effects showed spatial attenuation as depletion was strongest in the immediate neighborhood (first hexagonal ring around Visium spot) and progressively weakened at the second and third rings, consistent with a local exclusion mechanism. This demonstrated that B7-H3 expression spatially correlated with an immune-excluded TME, supporting the hypothesis of an immunosuppressive phenotype.

Next, the virtual CSO wanted to understand whether this immunosuppressive phenotype corresponded to differences in patient outcomes. The virtual CSO tasked the clinical trialist agent with performing a biomarker-stratified survival analysis on the TCGA PanCancer Atlas LUAD cohort, which included 477 patients with gene expression measurements and detailed survival outcomes (63, 64). To maximize separation between biologically distinct groups, the clinical trialist agent stratified patients by B7-H3 expression quartiles, comparing patients in the top and bottom quartiles on the basis of their B7-H3 expression (Fig. 4F). In a Cox proportional hazard model adjusted for age, cancer stage, and sex, elevated B7-H3 expression was significantly associated with worse overall survival [hazard ratio (HR) = 1.62; 95% CI: 1.05–2.49; P = 0.028] and worse disease-free survival (HR = 2.06; 95% CI: 1.08–3.90; P = 0.027). Together with spatial evidence of immune exclusion, the virtual CSO suggested that B7-H3-mediated immunosuppression could drive poor clinical outcomes, providing mechanistic and clinical rationale for targeting B7-H3 in lung cancer.

Finally, the virtual CSO dispatched the target biologist agent to determine the optimal modality. The agent retrieved Human Protein Atlas data confirming B7-H3 cell surface expression with subcellular vesicle localization (65). Together with the single-cell finding that

B7-H3 is overexpressed predominantly in TME fibroblasts rather than only on malignant cells, this led the virtual CSO to nominate an antibody-drug conjugate (ADC). The CSO reasoned that an ADC could act through three mechanisms consistent with these findings: cytotoxic payload delivery to B7-H3-expressing cancer cells, TME alteration through inhibition of B7-H3-mediated immunosuppressive checkpoint interactions, and bystander killing of adjacent B7-H3-negative cancer cells. Small-molecule and proteolysis targeting chimera (PROTAC) approaches were deprioritized after the pharmacologist agent's tractability analysis identified no existing chemical binders.

This case study was conducted without web search to prevent information leakage, and the underlying language model had a knowledge cutoff of January 2025. Of note, existing literature emphasized B7-H3's expression on cancer cells and canonical checkpoint-associated functions, motivating antibody- and ADC-based programs largely through a cancer cell-centric lens (57, 58). By contrast, the Virtual Biotech integrated evidence to nominate a less explored but mechanistically coherent hypothesis: that B7-H3 is more strongly overexpressed in cancer-associated fibroblasts, spatially associates with immune exclusion, and stratifies poor clinical outcomes, an interpretation that is not directly identified from any single dataset or publication. In August 2025, the FDA granted Breakthrough Therapy Designation to ifinatamab deruxtecan, a first-in-class B7-H3-targeted ADC (66–68). As the Virtual Biotech did not have access to this information, the regulatory announcement provided external support for the system's mechanism-driven therapeutic design.

This systematic and data-driven analysis was completed for a total cost of \$50.00 in Anthropic API credits. It showed how the Virtual Biotech can accelerate target validation and modality selection, a typically manual process performed by cross-functional drug discovery teams. The full conversation transcript is in supplementary text V.

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Clinical translation failure analysis: Virtual Biotech identifies possible failure mechanisms for terminated phase 2 trial testing first-in-class monoclonal antibody (mAb) against OSMR in ulcerative colitis

We subsequently used the Virtual Biotech to analyze cases of late-stage clinical development failure. We focused on the phase 2 MOONGLOW study (NCT06137183), a trial in ulcerative colitis (UC) evaluating the oncostatin M receptor subunit OSMRβ as a therapeutic target (69). OSMRβ is a cytokine receptor subunit that heterodimerizes with gp130 to mediate oncostatin M signaling pathways implicated in inflammation and fibrosis such as JAK-STAT (70, 71). Prior research demonstrated that elevated mucosal OSMR expression appears to mark a treatment-refractory UC inflammatory state, and mucosal OSMR expression has been independently associated with anti-TNF (tumor necrosis factor) nonresponse (71–73).

Vixarelimab is a first-in-class mAb engineered to block OSMRβ-mediated signaling (69). In MOONGLOW, adults with moderate-to-severe UC were randomized to receive vixarelimab or placebo. However, the trial was terminated in June 2025 because an interim futility analysis indicated that the primary endpoint was unlikely to be achieved (69). Accordingly, the initial query to the virtual CSO was: "We want to understand why trial NCT06137183 was terminated. This trial tested a first-in-class monoclonal antibody against OSMR in patients with UC. The results have been posted, and the trial was terminated due to interim futility analysis, which showed lack of efficacy. This termination was not related to safety concerns." The virtual CSO interpreted this as a clinical translation failure analysis and decomposed the query into subtasks focused on trial protocol and eligibility review, mechanistic assessment of OSMRβ signaling, pathway redundancy analysis in treatment-refractory gut tissue, and cross-disease exploration of OSMR-associated stromal activation programs.

The clinical trialist agent first analyzed trial design using the ClinicalTrials.gov record, which included the full study protocol (Protocol GA44839, Version 2 PDF) (69). It focused on the inclusion criteria, noting that the trial selected for a treatment-refractory study population of patients with UC who showed poor response to conventional or advanced therapies (Fig. 5A) (69). Because the drug target OSMRβ signals through the JAK-STAT pathway, the agent reasoned that it was important to understand whether OSMRβ serves as a primary driver of JAK-STAT signaling in treatment-refractory UC biology or if it instead represented a redundant point of entry into the same signaling cascade.

To answer this question, the single-cell agent then independently identified the TAURUS dataset (435,857 cells from 20 patients with UC) to investigate MOONGLOW failure mechanisms because it is a single-cell transcriptomic atlas of UC gut biopsies collected before and after anti-TNF therapy. The agent reasoned that this dataset, rather than a treatment-naïve UC atlas, enabled investigation of OSMR cell states from biologic nonresponders that resembled the specific patient population of MOONGLOW (74).

Accessing supplementary materials of the original study, the agent first confirmed that OSMR expression increased in three fibroblast cell states exclusively in nonresponders after treatment, consistent with the trial's rationale for targeting this receptor and with existing studies $(71, 72)$ . The agent then designed computational experiments not found in the original study. To investigate how this OSMR up-regulation affects downstream signaling, the agent implemented a genome-wide screen of transcription factor (TF) activity using the CollecTRI regulon database and applied mixed-effects modeling to identify differentially active TFs between nonresponders and responders in posttreatment tissue $(75)$ . This screen revealed that STAT1 activity was broadly elevated in nonresponder stroma where OSMR is expressed, reaching significance in 9 of 10 stromal cell types (mixed-effects P < 0.05 after FDR correction). This established that the JAK-STAT signaling axis downstream of OSMRβ is persistently active in the treatment-refractory tissue.

However, the agent noted a key structural aspect of the target biology: OSMRβ forms a heterodimer with gp130 (IL6ST), the common signal-transducing subunit used by the interleukin-6 (IL-6) cytokine family that includes IL-6, LIF, IL-11, CNTF, and CT-1. This observation brought into question the extent to which the prolonged STAT activation was genuinely attributable to OSMRβ itself versus being mediated by other gp130-family receptors that converge on the same pathway. To quantify the contribution of each receptor on inferred STAT1 activity, the agent designed a Shapley-based variance decomposition analysis across gp130-family receptor genes within each stromal cell state of posttreatment tissue from nonresponders. This analysis found that despite being the drug target, OSMR expression accounted for less variation in STAT1 activity than other co-receptors in most stromal cell types where OSMR is expressed (Fig. 5B). These findings raised the possibility that anti-OSMRβ therapy constituted a partial blockade in the context of treatment-refractory UC biology. This concept is consistent with a recent study that reported that treatment-refractory UC can reflect inflammatory pathways persisting through parallel receptor complexes that converge on the same downstream pathways (76).

The agent then hypothesized that, if redundancy within the gp130 axis contributes to treatment-refractory UC biology, a composite score capturing baseline gp130 axis expression could better predict nonresponse to therapy than OSMR alone. Thus, the clinical trialist agent then designed a gp130-axis risk score (see Materials and methods for details) and compared its performance to both OSMR expression alone and a previously reported five-gene nonresponse signature across four infliximab-treated UC cohort datasets (77–80). The gp130-axis score consistently outperformed OSMR alone across all four cohorts (Fig. 5C). The gp130-axis score also performed comparably to the Arijs signature across all cohorts, despite being derived entirely from the agent's prior single-cell mechanistic insight rather than from supervised gene selection. These findings supported the hypothesis that the gp130 signaling axis, rather than OSMR $\beta$ alone, better captures treatment-refractory disease in UC.

Finally, the Virtual Biotech investigated whether OSMR up-regulation is specific to UC or reflects a conserved stromal activation program across diseases. It conducted a systematic cross-disease expression survey by querying OSMR-pathway gene expression across 112 diseases represented in the CELLxGENE Census single-cell atlas, applying linear mixed models to test for disease-specific OSMR up-regulation relative to healthy tissue while accounting for donor and dataset batch effects (Fig. 5D) (59). The survey analysis recovered established OSMR biology in the stromal compartments of UC, colorectal, and gastric cancers, and in cardiomyocytes in myocarditis (74, 81–83). Beyond this, the Virtual Biotech highlighted roles for OSMR in acute kidney injury, pilocytic astrocytoma, periodontitis, and Alzheimer's disease and related dementias, with increased expression compartmentalized predominantly in fibroblast, endothelial, or neuronal cell types. The enrichment of OSMR expression across anatomically and etiologically diverse diseases suggested a conserved disease program associated with chronic inflammation. The cross-disease signals raised the possibility that OSMR-directed therapeutic strategies may have relevance beyond UC.

Taken together, this retrospective assessment demonstrated that the Virtual Biotech can start from a terminated clinical study and generate mechanistic insight. The agents combined trial protocol review, treatment-refractory study population target biology, single-cell signaling interrogation, biomarker performance comparison, and cross-disease expression mining to arrive at a unified rationale for the absence of efficacy: OSMRβ may label a treatment-refractory stromal inflammatory phenotype in UC but may not be the predominant driver of downstream JAK-STAT signaling in relevant OSMR-expressing cell states. Instead, these findings pointed to broader redundancy along the gp130 axis as a more accurate representation of treatment-refractory UC biology, enabling the derivation of a composite biomarker that surpassed OSMR alone in predicting nonresponse in independent cohorts. This case study was completed for a total cost of \$59.00 in Anthropic API credits, and the full conversation transcript is in supplementary text VI.

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Correctness and reproducibility of Virtual Biotech analyses

To evaluate the correctness and reproducibility of the case study analyses performed by the Virtual Biotech, we conducted human expert review. We split each of the two case studies into four stand-alone analyses (eight total). For B7-H3, these analyses correspond to Fig. 4, panels C to F. For OSMR, they correspond to Fig. 5, panels B to D. We recruited four human reviewers, and each was assigned to two analyses conducted by the Virtual Biotech. For each analysis, reviewers were asked to perform analyses following the same instructions from the virtual CSO to AI scientists by writing their own code. They were then asked, "After implementing the analysis yourself, do your conclusions generally match that of the Virtual Biotech? Please add notes describing your findings and thought process."

Experts answered “Yes” for all eight analyses, confirming that their analyses matched the agent’s findings. Then, experts reviewed the corresponding agent-written code for the analysis and were asked “Is the code written by the Virtual Biotech correct and free from mistakes that significantly impact the conclusions of the analysis? Please add notes describing your findings and thought process.” The reviewers answered “Yes” for all eight of the analyses, identifying minor stylistic design choices that the reviewers had made differently in their own analyses. These differences did not affect findings and interpretations. See supplementary text VII for example notes from the experts and figs. S6 and S7 for side-by-side comparisons of the Virtual Biotech and the expert-generated findings. These results demonstrated that the Virtual Biotech’s implementations are accurate.

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Comparison of the Virtual Biotech with other agentic systems

To compare the quality of Virtual Biotech responses to that of similar agentic systems, we queried Biomni, Kosmos, and PantheonOS (23–25), three state-of-the-art general purpose agentic systems, with our case studies: clinical trial annotations, B7-H3, and OSMR. For clinical trial annotation, we found that all three systems produced less accurate

A

"Analyzing NCT06137183 trial protocol and posted results. I'll delegate this task to the clinical trialist agent..."

"Accessing the ClinicalTrials.gov record. I see that this is a terminated Phase II trial testing vixarelimab in participants with moderate to severe ulcerative colitis (UC).

Analyzing study population..."

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Terminated

Based on a fatality analysis, which suggested that the Moonglow study was unlikely to meet its primary endpoint.

A Study to Evaluate the Efficacy, Safety, and Pharmacokinetics of Vixarelimab in Participants With Moderate to Severe Ulcerative Colitis (UC)

ClinicelTrials.gov ID NCT06187183

"I found TAURUS, a single cell atlas of adalimumab treatment in UC. Original study authors found increased OSMR expression in 3 fibroblast cell states exclusively in non-responders (NRs) after adalimumab."

I'm now scoring cell-type resolved TF activity followed by mixed-effects screening...

I see elevated STAT1 activity in NR post-treatment tissue in 9/10 stromal cell types. But, OSMR shares the gp130 signaling chain with 6 other receptors. Performing Shapley dominance decomposition to quantify redundancy...

Fascinating: despite being the drug target, OSMR explains less STAT1 variance than gp130, LIFR, or IL27RA in the vast majority of stromal cell types — JAK-STAT signaling driven through other receptors."

D

"I wonder if OSMR upregulation itself specific to UC? Launching OSMR expression analysis across 112 diseases with single cell data in CELLxGENE Census.

The survey analysis recovered established OSMR biology in UC fibroblasts and cardiac muscle. Interestingly, it suggests previously underexplored roles of OSMR in acute kidney injury, pilocytic astrocytoma, periodontitis, and Alzheimer's — predominantly in fibroblast, endothelial, or neuronal cell compartments.

Significantly increased OSMR expression spans many diseases, suggesting a conserved inflammatory program with potential therapeutic relevance for vixarelimab beyond UC.

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Eligibility Criteria

---

Description

Inclusion Criteria:

\+ Diagnosis of UC for at least 3 months + Moderately to severely active UC, assessed by mMS + Inadequate response, loss of response to, or intolerance to conventional or advanced therapies for UC

---

Exclusion Criteria:

\+ Diagnosis of Crohn's disease or indeterminate colitis

+ Suspicion of ischemic, radiation, microscopic, or infectious colitis

  • Prior colectomy

B

\- Inadequate response or loss of response to previous treatment of UC with tofacitinib, upadacitinib, or other systemic janus kinase (JAK) inhibitor

"NCT06137183 enrolled a treatment-refractory UC cohort: patients showed prior poor response to conventional therapies and/or advanced therapies (biologics and targeted small molecules). They also did not enroll JAK-inhibitor non-responders."

I'd like to better understand the treatment refractory biology in this patient population..."

"If signaling redundancy potentially explains why anti-OSMR mAb failed, I hypothesize that a gp130-axis score should outperform OSMR alone in predicting non-response.

I'm constructing a gp130-axis score by averaging pre-treatment expression of gp130-axis genes. Testing across four infliximab UC trial datasets as validation...

Fig. 5. Retrospective evaluation of terminated phase 2 trial protocol by the Virtual Biotech leads to refined development strategy for an OSMRβ-directed therapy in ulcerative colitis (UC). (A) Agent summary of the phase 2 UC trial (NCT06137183) investigating vixarelimab. (B) Single-cell signaling analysis of the TAURUS UC atlas. Shapley dominance analysis decomposes STAT1 activity across gp130-family α receptors, showing that OSMR is not the leading receptor driving persistent STAT1 activity in the majority of nonresponder stromal cell types. Right panels show OSMR detection fraction among each cell type, STAT1 activity enrichment in nonresponder versus

The gp130-axis score consistently outperforms OSMR alone. Virtual Biotech mechanistic insight from single-cell decomposition validates as a stronger clinical biomarker in bulk tissue."

responder posttreatment tissue, and overall cell-state abundances. (C) External validation in four cohorts of UC patients with bulk RNA-seq data collected of a 10-gene gp130-axis score to predict responders from nonresponders. Performance was compared against OSMR alone and a published five-gene inflammatory signature. AUC annotated per score within each trial. (D) Cross-disease OSMR expression analysis. Per-donor pseudobulk OSMR expression queried across 112 diseases in CELLxGENE Census and tested via linear mixed-effects models (disease versus matched normal tissue). Heatmap shows disease settings and cell types with significantly increased OSMR expression; black dots indicate FDR P < 0.05.

annotations on both the manual review set and the TDC labels as compared to the Virtual Biotech (table S2). For B7-H3 and OSMR, we queried each system with the same initial prompt used for the Virtual Biotech and had them perform open-ended analysis (tables S3 and S4). For a fair comparison, we provided similar levels of human steering to each system as was done for the Virtual Biotech in our case studies: Ask the system for a number of possible next steps after each analysis and manually select the most promising. We selected the choice that most closely aligned with analyses that were done in the case studies for comparability. Overall, these other agentic systems used fewer data modalities, performed less rigorous analyses, and produced fewer biologically meaningful results compared to the Virtual Biotech for both case studies (see supplementary text VIII for more details).

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Discussion

The Virtual Biotech is a multi-agent platform for early-stage drug discovery. At its core, a virtual CSO plans and coordinates multiple domain-specific scientist agents that analyze and reason over primary data sources. The domain-specialized scientist agents mirror core R&D functions and have access to a wide variety of tools and data sources. This collaborative setup allows for unified decision-making based on a collective and nuanced understanding of many primary data sources.

Our experiments showed that the Virtual Biotech is capable of performing large-scale analysis of clinical trials and identified several transcriptomic features of drug targets associated with clinical trial success. Additionally, two case studies on real-world drug development scenarios showed that the Virtual Biotech can yield insightful hypotheses that complement the evidence and conclusions reached by modern biopharmaceutical companies. This work contributes to a broader emergence of agentic AI systems organized around expert biomedical workflows $(21)$ . Beyond these scientific findings, the Virtual Biotech enables integrated cross-domain reasoning, more auditable evidence-based decision-making, and scalable analyses (see supplementary text IX for extended discussion).

The single-cell transcriptomic features of drug targets identified by the Virtual Biotech are themselves of independent interest as predictors of clinical trial success. Genetic evidence is recognized as one of the strongest predictors of clinical success and plays a central role in modern target prioritization $(39)$ . Prior work has also suggested that single cell-derived signals contain meaningful clinical information, linking these features to clinical phase progression $(56)$ . Building on this, we demonstrated that single cell-based features are not only associated with phase advancement but also with successful endpoint outcomes and reduced adverse event rates. Furthermore, we showed that single-cell evidence is orthogonal to genetic evidence and that associations between single-cell features and trial outcomes remained statistically significant within trials that had no supporting genetic evidence. Together, these findings suggest that incorporating single cell-derived evidence alongside genetic support may provide important guidance in drug development programs.

This study has limitations. The Virtual Biotech is a decision-support system for early-stage human therapeutic research, and it answers queries comprehensively on target-centered questions in well-characterized human diseases with deep coverage across genetics, transcriptomics, functional genomics, chemical biology, and clinical-trial resources. Conclusions are correspondingly weaker for rare or understudied diseases, poorly annotated targets, underrepresented tissues or populations, and questions lacking informative human genetic or single-cell evidence. The present configuration is human focused rather than veterinary, and pathogen-focused infectious-disease analyses are further constrained both by model-provider safety safeguards and by the shortage of dedicated pathogen and antimicrobial resources.

Of note, these are boundaries of the current data and tool coverage rather than of the architecture: Because data access are mediated through modular MCP interfaces, public, proprietary, or user-specific resources can be connected without redesigning the multi-agent framework, though each extension requires its own curation, specialist tools, and evaluation (supplementary text IX for extended discussion).

Additionally, our trial analyses are observational and should be interpreted as such. Possible confounders include trial targets, indications, endpoint definitions, and sponsor-related influences. In this vein, we adjusted for a trial's phase, year of enrollment, therapeutic area, and drug modality to address their potential confounding, observing consistent results. The analysis was also limited to trials registered in the ClinicalTrials.gov database and drugs that have mapped molecular targets. For the case studies, the Virtual Biotech generated data-driven hypotheses, which must be tested and further validated. There is a risk that the language model training can bias the agent toward existing hypotheses. To mitigate this, we intentionally selected case studies with trial readouts that occurred months after the language model knowledge cutoff date of January 2025.

Finally, the Virtual Biotech as presently implemented captures the computational analysis, evidence integration, and prioritization components of early therapeutic development rather than the full operations of a biotechnology organization. Experimental testing remains outside its scope. Its modality assessments reflect the data resources available to the system, so the absence of known binders or established tractability should be interpreted as an evidence gap and a source of development uncertainty rather than as proof that a modality is infeasible. More broadly, the increased throughput and scope of agentic systems raise considerations of hypothesis prioritization, provenance, independent validation, biosecurity, and scientific training (see supplementary text IX for extended discussion).

In the future, we envision expanding the Virtual Biotech to encompass even more of the drug discovery pipeline, such as molecule design, virtual screening, toxicity prediction, and clinical decision-making agents, bringing the benefits of interdisciplinary collaboration, speed, and objectivity to the entire end-to-end process. The Virtual Biotech illustrates a shift from isolated AI tools toward coordinated systems that reason across biological scales and stages of translation. As agentic platforms mature, they may enable a model of scientific organization in which hypotheses are continuously generated, stress-tested against heterogeneous evidence, and refined in partnership with human experts. Rather than replacing scientists, agentic systems could expand the scope and speed of therapeutic hypothesis exploration while making the reasoning process more transparent and reproducible.

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Materials and methods

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Virtual Biotech system architecture

Virtual Biotech is a multi-agent AI system that is organized to mimic the structure of a biotechnology research and development organization to accelerate and support therapeutic development and strategy. The system uses a hierarchical orchestration model comprising a chief scientific officer (CSO) as the global strategic orchestrator who oversees domain-specialized AI scientist agents and dedicated research support agents.

The virtual CSO agent supports multi-turn conversations with users, interprets queries, and dispatches analytical tasks to appropriate scientist agents. The CSO functions exclusively as an orchestrator: It routes queries, synthesizes findings, and provides strategic recommendations, but never directly accesses data or performs analyses. This separation of roles ensures that domain expertise remains encapsulated within scientist agents while the CSO maintains a global view of the research process.

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Human interaction with the Virtual Biotech

Virtual Biotech is designed for lightweight human interaction, in which the primary role of the user is to set intent and steer the system through high-level scientific questions or instructions. After a human user submits a scientific query, the CSO agents conducts a brief clarification interview—posing follow-up questions to align on scope feasibility—before initiating computational analyses (Fig. 1C). After objectives are clarified, subsequent actions are autonomous: The CSO decomposes the task and routes subtasks to scientist agents, scientist agents perform analyses and reason over findings, and the CSO synthesizes cross-division results into recommendations. Consistent with this design, in the case studies presented in this paper, human involvement was limited to (i) responding to CSO clarification prompts and (ii) asking follow-up questions after each iteration (e.g., to probe assumptions, request sensitivity checks, or trigger additional analyses). Experimental ideation, design, and execution remained agent-driven. Users can independently verify key results by inspecting and executing the generated code, enabling human oversight.

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AI scientist agents

The Virtual Biotech consists of a virtual CSO agent, eight distinct scientist agents distributed across four research divisions, plus two additional agents in the CSO's office that oversee the scientific direction and quality of the work (Fig. 1A). Each agent is configured with domain-specific system prompts and MCP access.

1) Target Identification and Prioritization Division integrates genetic causality, functional dependency, and cellular context to validate targets. The statistical genetics agent evaluates human genetic evidence by querying GWAS, locus-to-gene (L2G) machine learning predictions for causal gene assignment, fine-mapped credible sets, rare variant burden meta-analyses, and quantitative trait locus (QTL) colocalization to determine whether genetic variation affecting a gene influences disease risk. The functional genomics and perturbation agent assesses target essentiality and pharmacological tractability using CRISPR knockout screens and drug perturbation transcriptomic profiles from the Tahoe-100M dataset to evaluate whether a target can be modulated. The single-cell atlas agent queries CELLxGENE Census, which contains 143 million harmonized single-cell profiles, to learn cell type-specific expression patterns, differential expression between disease and healthy states, and cell-cell communication patterns

2) Target Safety Division integrates pathway reasoning, interaction-based effects, cell type-specific expression, and historical FDA regulatory safety signals to assess potential on- and off-target safety concerns. The biopathways and protein-protein interaction agent reasons through the target's biological context through pathway and molecular interaction maps to identify involvement in critical cellular processes that may pose safety concerns upon modulation. The single-cell atlas agent complements this network-level assessment by examining cell type-specific expression patterns across cell types found in 27 tissues of the Tabula Sapiens v2 atlas to identify potential off-target toxicity liabilities in critical cell types (46). The FDA safety officer agent complements these mechanistic assessments with empirical safety data from OpenFDA adverse event reports for drugs with similar mechanisms, drug safety warnings and black box labels from drug labels, and mouse knockout phenotypes to reason through potential target-level safety liabilities.

3) Modality Selection Division determines the optimal therapeutic modality for validated targets using structural biology, druggability assessment, and clinical precedence. The target biologist agent evaluates target properties that constrain modality choice, including protein family classification, subcellular localization, and structural tractability predictions that assess the likelihood of developing small-molecule binders, therapeutic antibodies, or other modality types on the basis of protein structure and binding site accessibility. The pharmacologist integrates this biological evaluation with existing clinical precedence, querying ChEMBL-derived drug databases to find approved therapies, pipeline compounds, and chemical probes that share the same target or mechanism. In addition, they analyze homologous proteins to determine family-level tractability and assess development practicality for each modality, including projected timelines, manufacturing demands, and likely hurdles.

4) Clinical Officers Division bridges preclinical assessments with clinical precedence by analyzing regulatory safety data and extracting insights from prior clinical development efforts. Working in tandem with the FDA safety officer agent, the clinical trialist agent enhances regulatory assessments with clinical precedence analysis. It locates prior trials aimed at the same gene or pathway; extracts information on trial phase, enrollment, endpoints, and results to determine the level of clinical validation; and examines discontinued studies to identify reasons for failure, including futility, safety concerns, or business-related decisions. For oncology targets, the clinical trialist agent can access clinicogenomics data to determine prognostic biomarkers across tumor types and survival outcomes from cBioPortal.

5) Office of CSO Agents: The chief of staff provides rapid strategic intelligence briefings on research fields and data landscape by inventorying MCP tools and performing web searches. The scientific reviewer performs quality assurance on AI scientist agent outputs, identifying gaps, unsupported conclusions, or misalignment with user queries (supplementary text III).

The system prompts for each agent are in supplementary text X. All agents as presented operated using Claude Sonnet 4.5, except for the chief of staff and scientific reviewer, which used Claude Haiku 4.5 for efficiency and speed. Scientist agents have access to standard computational tools including file operations and code execution, plus domain-specific data access tools in the form of MCP servers (described below). Scientist agents are instructed to maintain critical scientific thinking by questioning assumptions, validating findings across complementary datasets, and classifying evidence strength as weak or strong based on the convergence of independent lines of evidence.

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Implementation and language model configuration

Agents and orchestration were implemented using the Claude Agent SDK, an Anthropic agent development framework to build AI platforms $(84)$ . The SDK provides several capabilities for multi-agent scientific workflows: hierarchical agent orchestration enabling a parent agent to spawn and coordinate child agents with independent execution contexts, native integration with MCP servers for standardized tool access, and built-in support for multi-turn conversations with persistent conversation state. These capabilities allow the Virtual Biotech to implement complex delegation patterns where the CSO orchestrator manages scientist agents that operate autonomously while maintaining coordinated access to shared data resources. Agent behavior is controlled through structured system prompts that define role identity and expertise boundaries, available tools and data access permissions, analysis workflows and decision frameworks, and output formatting requirements. We summarize the Virtual Biotech workflow algorithms in supplementary text II. Specialized scientific workflows, such as single-cell quality-control and analysis, were implemented in the form of agent Skills with progressive disclosure of workflow guidance.

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Data and Virtual Biotech tool infrastructure

The Virtual Biotech integrates data from multiple public biomedical databases to enable a comprehensive evaluation of drug targets across the translational scientific spectrum and multiple biological scales. The Open Targets Platform (version 25.09) serves as the primary data backbone (33, 42). This is an extensive database that enables systematic discovery and evaluation of candidate therapeutic drug targets. By combining publicly available datasets, including those produced by the Open Targets experimental and informatics research programs, Open Targets curates data that support the development of therapeutic hypotheses. Each component contributes specific evidence types and detailed, high-resolution information on drug targets, diseases, genetic variants, QTL colocalization, mechanisms of action of therapeutic compounds, scientific publications, drug labels, FDA-reported safety signals, clinical trials, and other related data (33, 42).

We further integrated additional data resources into the Virtual Biotech that are key evidence sources in drug discovery. Single-cell atlas data are accessed and retrieved through MCP tools that leverage the CELLxGENE Census API, which aggregates harmonized single-cell RNA-sequencing (RNA-seq) profiles from over a thousand published studies, offering standardized cell-type annotations across diverse tissues and disease conditions $(59)$ . In addition, we provided the Virtual Biotech with a local copy of the Tabula Sapiens v2 healthy reference atlas $(46)$ . Pseudobulked differential expression profiles were procured from Tahoe-100M, a gigascale single-cell perturbation atlas of 50 cancer lines exposed to 1100 small-molecule perturbations $(34)$ . Agent access to clinicogenomic and outcome data in different cancer cohorts was implemented using MCP tools powered by the cBioPortal REST API $(85)$ . Finally, clinical trial information was made available to agents via tools that leveraged the ClinicalTrials.gov API $(86)$ .

Data access to each agent is mediated through 10 MCP servers, each implemented as a FastMCP Python instance that exposes domain-specific query functions as callable tools (Fig. 1B and supplementary text I). MCP provides a standardized interface between language models and external data sources, enabling structured queries with typed parameters and formatted responses $(29, 30)$ . Each MCP tool is implemented as a Python function with comprehensive docstrings and typed parameter signatures, which FastMCP automatically introspects to generate structured tool schemas exposed to the language model at runtime, injecting required context that enables agents to discover available tools and understand their purpose, required inputs, and expected outputs without manual specification $(87)$ . Tools provide not only raw outputs but also interpretable summaries and preview results, allowing agents to rapidly gauge relevance and determine whether more in-depth analysis is warranted. This facilitates efficient multistep reasoning and iterative tool invocation across diverse data sources. Each MCP server offers specialized tools tailored to frequent analytical tasks. These tools accept structured inputs—such as gene symbols, disease identifiers, and various filter parameters—and return well-formatted outputs optimized for language model consumption. The Virtual Biotech MCP tools are intentionally composable, enabling agents to chain multiple tool invocations together to construct rich, comprehensive evidence profiles.

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Benefits of multi-agent architecture

The multi-agent architecture of the Virtual Biotech offers several key advantages when compared to single-agent approaches. The breadth of data sources and analytical tools incorporated into the Virtual Biotech, on the scale of hundreds of tools and terabytes of data spanning $\sim$ 80,000 targets, 40 million papers, and over 100 million cell profiles, makes in-depth analyses of these sources by a single agent infeasible owing to context, time, and memory constraints (33, 34, 88). By contrast, a multi-agent framework allows these analyses to be decomposed and distributed across parallel agents with isolated contexts, enabling each agent to conduct a thorough, focused analysis without overwhelming the shared context. High-level summaries from these agents are then integrated by a coordinating agent to support final decision-making.

Second, the multi-agent architecture enables parallel workflows at scale. For example, in extracting clinical trial outcomes, each extraction followed a multistep workflow: Given an input NCT ID, the clinical trialist agent first calls the ClinicalTrials.gov API to retrieve trial metadata, then evaluates whether all required fields are sufficiently populated before moving through a three-tier evidence cascade. This cascade involves searching PubMed with NCT ID confirmation and then expanding to additional web sources. Throughout this process, the agent reviews numerous information sources to understand trial designs, interpret complex clinical outcomes, determine endpoint results, map termination reasons to a standardized ontology, and consolidate all evidence into a validated JSON output that adheres to a Pydantic schema. Consequently, we assigned a dedicated agent to each trial, allowing it to use its full context window on that single study—gaining deep familiarity with its design, results, and literature—without the distraction or context dilution of managing multiple trials in one conversation. Additionally, this design enables our multi-agent parallelized workflow where 37,075 phase 2 and phase 3 trials were systematically processed in 6 hours. By contrast, processing the same number of trials with a single agent would require \~1839 hours or 76.6 days of runtime. The parallelized multi-agent architecture therefore achieves an approximately 184-fold speedup, reducing a months-long extraction to an overnight run.

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Analysis of single-cell features and clinical trial outcomes

Clinical trial manual validation: We sampled 100 trials from the Open Targets clinical trial dataset that was included in the agent-driven curation process (50 randomly sampled from all phase 2 trials, and 50 from all phase 3 trials). Two human annotators assessed agreement with the agent's annotations for primary outcomes, secondary outcomes, and adverse event (AE) rates. For both primary and secondary endpoints, trials were classified into two groups on the basis of whether or not there was sufficient evidence supporting a positive trial endpoint. Not all outcomes were applicable to each trial; for example, primary endpoints were not counted for trials stopped early. For each trial, the annotators first reviewed the ClinicalTrials.gov record for posted results and any linked publications. If none were available, they searched Google by NCT identifier and trial name to identify relevant abstracts or reports. The annotators then compared these sources against the agent's extracted outcomes, performing additional review when discrepancies arose and documenting the reasons for disagreement. The two human annotators discussed ambiguous cases to reach a consensus. Phase 1 trials were not reviewed because their success was defined algorithmically as progression to phase 2. Phase 1 trials were classified as having progressed to phase 2 if there existed at least one phase 2 trial that tested the same set of drugs for the same indications, with a subsequent or concurrent trial start date.

Among the trials where the agent's annotations differed from manual review or TDC data, the differences were confined to intrinsically ambiguous cases: studies with multiple experimental arms in which some arms achieved the primary endpoint whereas others did not; trials where the primary endpoint failed to reach conventional statistical significance (for example, $P = 0.06$ ) despite supportive secondary or longer-term outcomes; and single-arm or dosage-based study designs that did not cleanly map onto a simple success/failure dichotomous outcome. These edge cases indicated intrinsic ambiguity in reducing complex, multi-endpoint results to discrete classes, rather than systematic mistakes by either annotation source.

Single-cell feature extraction from Tabula Sapiens: Single-cell expression features were derived from the Tabula Sapiens atlas, comprising 27 human tissues (bladder, blood, bone marrow, eye, fat, heart, kidney, large intestine, liver, lung, lymph node, mammary, muscle, pancreas, prostate, salivary gland, skin, small intestine, spleen, stomach, testis, thymus, tongue, trachea, uterus, vasculature, and ear). Cell-type annotations were based on the Cell Ontology class assignments provided in the atlas. For each target gene, features were first computed per tissue and then aggregated across tissues to obtain a single global value per gene.

Cell-type specificity: Tau index: Cell-type specificity was quantified using the Tau index ( $\tau$ ), which measures the degree to which gene expression is restricted to specific cell types (47). For a gene with mean expression $\overline{x}_{j}$ in cell type j across n cell types within a given tissue:

$$

\tau_ {\mathrm{tissue}} = \frac {\sum_ {j = 1} ^ {n} \left(1 - \frac {\overline {{x}} _ {j}}{\overline {{x}} _ {\max}}\right)}{n - 1}

$$

where $\overline{x}_{\max} = \max_{j} (\overline{x}_{j})$ is the maximum mean expression across all cell types within that tissue. The Tau index ranges from 0 (ubiquitous expression, equal across all cell types) to 1 (perfectly specific expression, expressed in only one cell type). Cell types with fewer than 20 cells were excluded from Tau computation, and mean expression was computed from log-normalized counts. For a given gene target, the Virtual Biotech then aggregated Tau metrics across all tissues as the arithmetic mean of per-tissue Tau values across tissues in which the gene was expressed.

Expression heterogeneity: Bimodality coefficient: Within-population expression heterogeneity was assessed using the bimodality coefficient (BC), which detects the presence of distinct expression subpopulations (48, 49). For a gene's expression vector across n expressing cells (cells with expression > 0) within a given tissue:

$$

\mathrm{BC} _ {\mathrm{tissue}} = \frac {m _ {3} ^ {2} + 1}{m _ {4} + \frac {3 (n - 1) ^ {2}}{(n - 2) (n - 3)}}

$$

where $m_{3}$ is the sample skewness and $m_{4}$ is the Pearson kurtosis. The bimodality coefficient ranges from 0 to 1. Only expressing cells were included in the computation to focus on heterogeneity among cells that transcribe the gene. The global bimodality score for each gene was computed as the arithmetic mean of per-tissue bimodality coefficients.

Statistical analysis of single-cell atlas features with trial outcomes: Our statistical analyses of single-cell features followed the same approach in analogous studies of genetic evidence $(39, 40)$ . Clinical trial outcomes (phase progression, trial termination, endpoint success) were analyzed with univariate logistic regression to estimate the association between single-cell expression features and outcome probability. Features were z-score standardized prior to model fitting to enable comparison of effect sizes across continuous features with different scales. Model parameters were estimated via maximum likelihood using generalized linear models with a binomial family and logit link (statsmodels.GLM,Binomial family). For trials assessing drugs that act on multiple molecular targets, and thus yield several tau and bimodality features per trial, the minimum value across all targets for each feature type was used as the single-cell agent hypothesized that the least specific target likely drives the overall safety profile. For continuous percentage outcomes such adverse event rates by organ system calculated at the patient-level, we used beta regression as implemented in R's betareg package $(89)$ . The resulting regression coefficient corresponds to the change in the logit of the mean adverse event proportion associated with a one-standard-deviation increase in the predictor. These univariate analyses are the main results we present, consistent with the approaches of Razuvayevskaya et al. $(40)$ and Minikel et al. $(39)$ .

In addition to these results, we conducted robustness analyses to further support our findings. First, to assess whether observed associations exceeded chance, we conducted permutation tests with 1000 iterations per feature-outcome combination. In each iteration, the outcome vector was randomly shuffled while retaining the original feature values, and the regression was refit to obtain a null coefficient. Empirical two-sided P values were computed as the proportion of null coefficients with absolute value greater than or equal to the observed coefficient. Permutation tests were run for both the logistic (binary outcome) and beta regression (adverse event rate) analyses using model specifications identical to those of the primary analyses.

Next, to account for potential confounding by drug modality, therapeutic area, trial start year, and clinical phase, we fit generalized mixed-effects models (GMMs). For binary outcomes, we used logistic GMMs via lme4::glmer in R with crossed random intercepts for drug-type combination and therapeutic area combination. For adverse event rate outcomes, we used beta mixed-effects regression via glmmTMB::glmmTMB with a beta family and the same crossed random-effects structure.

To evaluate whether single-cell expression features provided additional information independent of genetic evidence, we fit bivariate logistic regression models adjusting for genetic evidence. For adverse event outcomes, the analogous bivariate beta regression was fit using R's betareg. As a complementary analysis, we repeated the univariate analyses restricting to the subset of trials (75%) that have no genetic evidence. Following the approach of Razuvayevskaya et al., genetic evidence was defined as a binary indicator of whether any target-disease indication pair in a trial had a direct genetic association reported in Open Targets, which aggregated evidence from GWAS, phenomewide association studies, gene burden analyses, and clinically annotated variants (ClinVar/EVA) (33, 40).

To adjust for multiple hypothesis testing, we used the Benjamini-Hochberg procedure to control for a FDR of 5% (90).

To enable interpretable quantification, we also binarized the continuous tau cell-type specificity index into either “cell-type-specific” or “broadly expressed” categories using K-means clustering $(k=2)$ on the trial-level distribution, setting the threshold at the midpoint of the two cluster centers $(\tau=0.69)$ .

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Single-cell and spatial transcriptomics analyses

Quality control and data preprocessing: Raw single-cell or single-nucleus RNA-sequencing count matrices were subjected to quality control filtering. Cells were retained if they expressed between 300 and 9000 genes and had $\leq15\%$ mitochondrial reads. To mitigate compositional biases from uneven sampling, donor-level downsampling was performed (maximum 10,000 cells per donor), stratified by cell type to preserve relative proportions. Gene expression was normalized using library-size normalization and log1p transformation via Scanpy (v1.9+) (91). Highly variable genes (3000) were selected for downstream dimensionality reduction.

Cell-type annotations across datasets were harmonized to a common vocabulary using the Cell Ontology $(92)$ . Fine-grained annotations were mapped to standardized Level 3 ontology categories through hierarchical ontology traversal. Cell types were filtered to those eligible for downstream differential expression analysis, requiring representation by $\geq3$ donors per condition and $\geq20$ cells per donor.

Dimensionality reduction was performed using principal component analysis (40 components). Batch effects were corrected using Harmony $(93)$ to preserve biological variation while mitigating technical differences across datasets. Uniform manifold approximation and projection (UMAP) embeddings were computed on the Harmony-corrected principal components for visualization. Batch mixing was assessed by comparing corrected and uncorrected embeddings.

Pseudobulk differential expression: Differential expression analysis was performed using a pseudobulk approach. Raw counts were aggregated by donor and cell type, and differential expression was tested using PyDESeq2 (94). Genes were defined as differentially expressed at FDR-adjusted P value < 0.05 and $\left|\log_{2}FC\right| > 1.0$ .

Cell-cell communication analysis: Cell-cell communication inference was performed using LIANA (60), which computes a consensus score across multiple ligand-receptor inference methods. LIANA's rank\_aggregate method was run with 1000 permutations within two groups. In SCLC, the first group was fibroblasts in the top quartile ranked by

B7-H3 expression, and the second group was fibroblasts in the bottom quartile. In LUAD, the top quartile cutoff for B7-H3 expression was not sufficiently high to isolate B7-H3-expressing fibroblasts, so the first group was therefore B7-H3-expressing fibroblasts and the second group was nonexpressing fibroblasts. Interactions were retained if they ranked in the top $10\%$ of interactions by coexpression magnitude, CellPhoneDB permutation test $P < 0.01$ , and were supported by $\geq 3$ constituent methods. Group-specific interactions were identified by comparing interaction sets that met the aforementioned criteria between conditions.

Cell--type deconvolution of spatial transcriptomics data: Cell-type deconvolution of 10x Visium spatial transcriptomics data was performed using Cell2Location on a NVIDIA H100 GPU (62). Briefly, this published workflow first trained a negative binomial regression model on the LUAD single-cell atlas to estimate gene expression signatures for each cell type. The trained reference signatures were then applied to spatial data to infer cell-type abundances per spot, with an expected cell density of eight cells per spot. We excluded the gene of interest (B7-H3) from this workflow to avoid circularity in the downstream analyses. The reference model was trained for 250 epochs and the spatial mapping model for 10,000 epochs. Cell-type proportions were computed from the top fifth percentile posterior estimates of cell abundances.

Spatial immune neighborhood analysis: To assess immune cell composition in the local microenvironment of gene-expressing spots, a k-nearest neighbor graph $(k = 6)$ was constructed for each tissue section using spatial coordinates (95). Within each sample, expressing spots were stratified into gene-high (top quartile) and gene-low (bottom quartile) groups on the basis of per-sample thresholds. The middle 50% of spots were excluded. Samples with fewer than 25 expressing spots were omitted. For each spot, the mean Cell2Location-estimated cell-type abundance across its k nearest spatial neighbors was computed. To test for immune depletion while controlling for confounders of spatial tissue architecture, mixed-effects models were fit separately for each immune cell type:

$$

\begin{array}{c} Y _ {i j k} \sim \beta_ {0} + \beta_ {1} \cdot \text {Gene} _ {\text {high}} + \beta_ {2} \cdot \text {UMI} _ {z} + \beta_ {3} \cdot \text {Fibroblast} _ {z} + \beta_ {4} \cdot \\ \text {Epithelial} _ {z} + \beta_ {5} \cdot \text {Endothelial} _ {z} + u _ {j} + v _ {j k} \end{array}

$$

where $Y_{ijk}$ is the mean neighbor immune abundance for spot i in sample k nested within patient j; total UMI serves as a proxy for sequencing quality, fibroblast, epithelial, and endothelial cell abundances (all measured at the focal spot) control for spatial compartment identity; and $u_{j} \sim \mathcal{N}(0, \sigma_{u}^{2})$ and $v_{jk} \sim \mathcal{N}(0, \sigma_{v}^{2})$ are patient- and sample-level random intercepts, respectively, to account for pseudoreplication and slide-to-slide variation. Spatial attenuation was assessed by repeating the analysis at increasing neighbor rings (neighbors 7–15, 16–30). Models were estimated using restricted maximum likelihood (REML) via lmerTest (96).

Biomarker-stratified survival analysis: To assess the prognostic significance of B7-H3 expression in LUAD, survival analysis was performed on the TCGA PanCancer Atlas LUAD cohort accessed via cBioPortal (63, 64). Gene expression profiles and clinical annotations—including age at diagnosis, AJCC pathologic tumor stage, sex, and survival endpoints—were retrieved for 566 LUAD patients. Analysis was restricted to patients with complete covariate data for age, stage, and sex. A total of 477 patients were ultimately used for the analysis. Patients were stratified into expression quartiles on the basis of B7-H3 (CD276) expression, comparing the top quartile (high expression) against the bottom quartile (low expression). Multivariable Cox proportional hazards models were fit for overall survival (OS), progression-free survival (PFS), disease-specific survival (DSS), and disease-free survival (DFS), adjusting for age (continuous), cancer stage [advanced (III/IV) versus early (I/II)], and sex. Survival analyses were performed using the lifelines Python package.

Transcription factor activity inference: To identify transcription factors with persistently altered activity in treatment-refractory UC tissue, TF activity scores were inferred from the TAURUS longitudinal single-cell atlas of anti-TNF (adalimumab) treatment in inflammatory bowel disease $74$ . The analysis focused on UC patients $n = 20; 14$ nonresponders, 6 responders) with paired pre- and posttreatment colonic biopsies, after excluding patients without outcome annotation. Raw counts were normalized to 10,000 counts per cell and log1p-transformed. TF activity was scored using the CollecTRI regulon collection $75, 97$ via decoupler using the multivariate linear model (MLM), which jointly scores TFs sharing target genes to correctly partition shared regulatory signals $75$ .

To compare TF activity between nonresponders and responders, linear mixed-effects models were fit for each TF and cell type on post-treatment cells:

$$

\mathrm{TFactivity} _ {i j} \sim \beta_ {0} + \beta_ {1} \cdot \text { Remission\_status } _ {j} + u _ {j}

$$

where $u_{j} \sim \mathcal{N}(0, \sigma_{u}^{2})$ is a sample-level random intercept. Models were fit using lmerTest (96) via rpy2, with Satterthwaite degrees of freedom for P-value estimation. P values were corrected using the Benjamini-Hochberg procedure within each cell type (90). This screen was applied across 766 TFs in 10 OSMR-expressing stromal cell types.

Shapley variance decomposition analysis across gp130-family receptors: To quantify the relative contribution of each gp130-family $\alpha$ -receptor to downstream transcription factor activity, the agents performed variance decomposition using the Lindeman–Merenda–Gold (LMG) method (98), which computes Shapley value-based relative importance shares by averaging marginal $R^{2}$ contributions over all possible predictor orderings. For each of the 10 OSMR-expressing stromal cell types in non-responder posttreatment tissue (defined as $\geq5\%$ OSMR detection), STAT1 activity was scored via univariate linear model (ULM) using a cleaned CollecTRI regulon from which any predictor receptor gene appearing as a regulon target (IL6ST) had been removed to prevent circularity (75, 97). Pseudobulk mean expression of each receptor and mean STAT1 ULM activity were computed per sample and cell type (minimum 10 cells per pseudobulk group). The outcome (z-scored STAT1 activity) was regressed onto seven gp130-family $\alpha$ -receptors (OSMR, IL6ST, LIFR, IL6R, IL11RA, IL27RA, CNTFR) with patient-level random intercepts:

$$

\mathrm {STAT1\_activity} _ {z} \sim \sum_ {r} \beta_ {r} \cdot \mathrm{Receptor} _ {r, z} + (1 | \text { Patient })

$$

where all predictors were z-scored within each cell type. LMG shares were computed by exhaustive enumeration of all $2^{7} = 128$ receptor subsets (one mixed-effects submodel per subset per cell type), extracting the marginal $R^{2}$ from each via MuMIn using r.squaredGLMM (99). Ninety-five percent confidence intervals were estimated via cluster bootstrap (2000 resamples at the patient level), using ordinary least squares for computational tractability.

gp130-axis biomarker score validation in bulk cohorts: To validate the gp130-redundancy hypothesis in independent patient cohorts, bulk gene expression data from four infliximab-treated UC clinical trial cohorts were obtained from the Gene Expression Omnibus (GSE12251, GSE16879, GSE23597, GSE73661). When multiple microarray probes mapped to the same gene, expression was summarized as the mean across probes. A gp130-axis composite score was defined as the simple mean of within-cohort z-scored baseline expression across 10 genes (OSMR, IL6ST, LIFR, IL6R, IL11RA, IL6, IL11, OSM, LIF, STAT1), selected by the agents based on the single-cell variance decomposition results with no empirical model fitting. Predictive performance for treatment nonresponse was assessed by area under the receiver operating characteristic curve (AUC) and compared to OSMR expression alone at baseline and to the established five-gene anti-TNF response signature of Arijs et al.

(IL13RA2, TNFRSF11B, STC1, PTGS2, IL11), scored using the same within-cohort z-score averaging procedure (77).

Cross-disease OSMR expression survey: To determine whether stromal OSMR up-regulation is specific to UC or reflects a conserved inflammatory response, we queried the CZ CELLxGENE Census (59) across 112 diseases that passed quality filters. For each disease, per-donor pseudo-bulk expression was calculated as $\log_{2}(\mathrm{CP10K}+1)$ for the OSMR gene, including only donors with at least 25 cells per cell type. Cell types were harmonized to Level 1 categories using the Cell Ontology (92). Disease and normal tissue-matched control arms were constructed, with normal donors prioritized by study and assay overlap. Differential expression was tested using weighted linear mixed-effects models:

$$

\text { mean\_log2\_OSMR\_cp10k } \sim \beta_ {0} + \beta_ {1} \cdot \text { condition } +

$$

$$

\beta_ {2} \cdot \log \_ d e p t h [ + \beta_ {3} \cdot a s s a y \_ g r o u p ] + (1 | d a t a s e t \_ i d)

$$

where condition indicates disease versus normal, log depth controls for residual sequencing depth differences, assay group (included when more than one assay type was present) accounts for platform differences, and the dataset-level random intercept accounts for study heterogeneity. Observations were weighted by the number of cells contributing to each pseudobulk estimate. Models were fit using lmerTest with Satterthwaite degrees of freedom; when fewer than two studies were available, an ordinary weighted linear model was used instead $96$ . P values were corrected globally across all disease–cell type–gene tests controlling for a FDR of 5% $90$ .

---

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98. R. H. Lindeman, P. F. Merenda, R. Z. Gold, Introduction to Bivariate and Multivariate Analysis, vol. 4 (Scott, 1980).

99. K. Barton, MuMIn: Multi-Model Inference (R package version 1.18, 2015).

100. H. G. Zhang, P. Eckmann, J. Miao, A. B. Mahon, J. Zou, The Virtual Biotech: Case Study Documentation, Zenodo (2026); https://doi.org/10.5281/zenodo.22259123.

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ACKNOWLEDGMENTS

The authors thank S. He, S. Alber, W. Deng, and other members of the Zou Lab at Stanford University for their valuable input and useful discussions on this work. Funding: National

Institutes of Health (T32-GM145402 to H.G.Z.); Knight-Hennessy Scholarship (to H.G.Z.) National Science Foundation Graduate Research Fellowship Program (DGE-2146755 to P.E.); Stanford Graduate Fellowship (to P.E.). Author contributions: H.G.Z. and J.Z. conceived and supervised the study. H.G.Z. developed, implemented, and optimized the framework. H.G.Z. oversaw analyses and visualization of the case studies. A.B.M. provided input and guidance on the case studies. P.E. designed the human expert evaluation and performed benchmarking of the framework. H.G.Z. and J.M. designed the user interface. H.G.Z., P.E., and J.Z. drafted the manuscript. All authors discussed, reviewed, and edited the final manuscript. Competing interests: A.B.M. is an employee of PHD Biosciences. All other authors declare that they have no competing interests. AI use declaration: An AI coding tool (Claude Code) was used to assist with code generation and debugging. All AI-generated code were reviewed and verified by the authors. Data, code, and materials availability: Data from the Open Targets Platform can be directly accessed at https://platform.opentargets.org. CELLxGENE data can be accessed at https://cellxgene.cziscience.com. The Tabula Sapiens dataset can be accessed at https://tabula-sapiens.sf.czbiohub.org/. The Visium lung adenocarcinoma dataset can be accessed at https://pubmed.ncbi.nlm.nih.gov/38782901/. The TCGA PanCancer Atlas lung adenocarcinoma cohort was accessed through cBioPortal (study ID luad\_tcga\_pan\_can\_atlas\_2018; https://www.cbioportal.org/study/summary?id=luad\_tcga\_pan\_can\_atlas\_2018). The microarray data for the four UC trials analyzed can be accessed with GEO

accession IDs GSE12251, GSE16879, GSE23597, and GSE73661. The TAURUS dataset can be accessed at https://pubmed.ncbi.nlm.nih.gov/39438660/. The full case study documentation including the codebase, intermediate results, agent-generated reports, figures, Virtual Biotech clinical trials dataset, and benchmarking outputs are available at Zenodo (100). The code for the Virtual Biotech, including a runnable command line interface and the complete set of system prompts and MCP servers, can be found at: https://github.com/harrisongzhang/TheVirtualBiotech. No new materials were generated in this study. License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.aeg6779

Supplementary Text; Figs. S1 to S7; Tables S1 to S4; MDAR Reproducibility Checklist

Submitted 23 February 2026; resubmitted 25 May 2026; accepted 2 September 2026; published online 17 September 2026

10.1126/science.aeg6779

Wireless electrocatalytic closed-loop system for drug-free management of diabesity

Debasis Maity, Preetam Guha Ray, Peter Buchmann, Ghislaine Charpin-El Hamri, Martin Fussenegger\*

Full article and list of author affiliations: https://doi.org/10.1126/science.ady8560

INTRODUCTION: Type 2 diabetes and obesity frequently coexist (as “diabesity”) and affect billions of people worldwide. Current treatments rely largely on drugs that lower blood glucose or body weight, but these therapies can produce side effects, require lifelong administration, and may lose effectiveness over time. A subcutaneous implant containing a solid electrocatalyst that directly removes excess glucose from the bloodstream at an electrically adjustable rate could provide a dose-controllable, drug-free therapeutic alternative.

RATIONALE: Electrocatalysts use electricity to accelerate chemical reactions. We developed an implantable device containing platinum (Pt)-decorated gold (Au) nanoclusters embedded in a porous graphite matrix. When wirelessly powered, the ECHO (electrocatalytic closed-loop health optimization) device selectively oxidized glucose into gluconate, a lower-energy metabolite that is readily cleared through the kidneys. Because electrical stimulation can be precisely controlled, the rate of glucose removal could also be precisely regulated. We designed the implant to restore glucose homeostasis, reshape energy metabolism, and enable autonomous closed-loop control when coupled to a commercial continuous glucose monitor.

RESULTS: The electrocatalyst selectively converted glucose into gluconate under physiologically relevant conditions and retained its activity during prolonged operation. After implantation in mice with diabesity, wireless activation rapidly restored elevated blood glucose to the normal range, with repeated treatment maintaining glucose control for 6 weeks without detectable hypoglycemia.

Lowering glucose shifted whole-body metabolism toward the use of stored fat. Treated mice exhibited reduced circulating triglyceride concentrations and body weight, together with increased concentrations of free fatty acids and ketone bodies. The implanted device remained functional throughout the 6-week treatment period, and treatment produced no detectable adverse physiological, inflammatory, or behavioral effects.

Coupling the implant to a commercial continuous glucose monitor enabled autonomous closed-loop operation. The system activated the electrocatalyst only when glucose exceeded a predefined threshold, thereby maintaining glucose within a desired range.

CONCLUSION: A wirelessly powered electrocatalytic implant directly removed excess blood glucose while promoting the use of stored fat, all without administering drugs. Coupling the implant to continuous glucose monitoring enabled autonomous closed-loop metabolic control and demonstrated the potential of electrocatalysis as a drug-free approach to managing diabetes and obesity. □

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Wireless electrocatalytic control

of diabesity. The ECHO system combines continuous glucose monitoring with a wirelessly powered electrocatalytic implant that oxidizes excess glucose to gluconate for renal clearance. In mice with diabesity, autonomous closed-loop control restored glucose homeostasis, reduced body weight, and promoted fat utilization without glucose-lowering drugs. [Figure created with BioRender.com. Maity, D. (2026) https://BioRender.com/r5kl19g]

Wireless electrocatalytic closed-loop system for drug-free management of diabesity

Debasis Maity $^{1}$ , Preetam Guha Ray $^{1}$ , Peter Buchmann $^{1}$ , Ghislaine Charpin-El Hamri $^{2}$ , Martin Fussenegger $^{1,3*}$

Lifestyle-related type 2 diabetes and associated obesity (diabesity) affect >2.5 billion people worldwide and impose nearly \$3 trillion in annual health care costs. We developed an implantable, wirelessly powered electrocatalytic closed-loop health optimization (ECHO) device containing platinum-decorated gold nanoclusters embedded in graphite felt that enabled selective, electrically tunable oxidation of blood glucose to renally cleared gluconate. In type 2 diabetic mice, wireless, low-power activation (0.75 volts, 10 milliamperes) restored glucose homeostasis within 1 hour, shifted metabolism from glucose to lipid utilization, reduced body weight and triglycerides, and increased circulating free fatty acids and ketone bodies without detectable hypoglycemia or adverse physiological, inflammatory, or behavioral effects during 6 weeks of treatment. Coupling this ECHO device to a commercial continuous glucose monitoring system enabled autonomous, smartphone-controlled, drug-free closed-loop management of experimental diabesity.

Diabetes and obesity are two genetic predisposition-enhanced interlinked chronic physiological lifestyle conditions associated with deregulation of metabolic energy homeostasis (1–5), the combination of which is known as diabesity. The physiological relationship between obesity and diabetes is bidirectional and self-reinforcing, involving a complex interplay of metabolic, hormonal, and inflammatory changes (1, 5–7). In particular, carbohydrate-triggered fat storage is a central driver for the development and reinforcement of diabetes and obesity, thereby creating a vicious cycle fueling the diabesity pandemic, which affects nearly 30% of the global population and incurs health care costs reaching >1% of the global gross domestic product (GDP) (1–3, 5, 8–10). As diabesity-promoting lifestyle changes correlate with welfare and increasing GDP, the diabesity pandemic continues to drastically increase globally (2, 3, 5, 10, 11).

With no cure available and low compliance with recommended lifestyle changes, current diabesity strategies focus on lifelong drug-based management of diabetes and obesity $(5, 11-13)$ . Diabetes management remains particularly challenging given the limited precision of manual open-loop interventions and the lack of real-time dynamic dosing, resulting in chronically deregulated glucose metabolism and persistent insulin administration, which may lead to acute emergencies and numerous devastating comorbidities $(14, 15)$ . Continuous glucose-monitoring devices and their closed-loop integration with drug-delivery systems such as insulin pumps have greatly improved real-time blood glucose profiling, precision insulin dosing, and prompt delivery, but technical and mechanical issues, such as insufficient sensor accuracy, sensor biofouling and signal drift, poor reliability, lack of personalization, and limited flexibility, as well as high cost and limited availability, remain major limitations $(16-20)$ .

These challenges have spurred the development of advanced cell-based proof-of-concept therapies using designer cells (21) that secrete blood glucose-modulating proteins (22–26) in response to molecular (27–30) or physical cues (31–34). These cells can be coupled with real-time in situ molecular blood glucose monitoring for closed-loop control (35, 36), a concept that has also been explored in obesity management (31, 37–40). For instance, cells engineered to sense food intake (37) or blood lipid levels (39) can regulate the production of biopharmaceuticals or satiety hormones, thereby reducing food consumption, restoring metabolic homeostasis, and maintaining a healthy body weight (37–40). Despite the promise of these engineered cells, multiple hurdles—including tumorigenicity, immune rejection, and manufacturing costs—currently impede clinical implementation (41–44). In parallel, glucagon-like peptide 1 (GLP-1) and glucose-dependent insulinotropic polypeptide (GIP) receptor agonists [semaglutide (45–47) and tirzepatide (22, 23), respectively] have emerged as a recent advance in treating diabesity by simultaneously addressing diabetes and obesity (48–52). However, high cost, frequent adverse gastrointestinal effects, and ongoing questions about long-term safety, including risks that may not yet be apparent, leave the population-level impact of these widely used therapies on the diabesity burden uncertain. Despite their early success, these drugs illustrate key challenges associated with modern medication: cost, dosing, and side effects (47, 48, 52–58). Enzyme-catalyzed glucose oxidation, exemplified by glucose oxidase-based biosensors, is among the most successful biomedical applications of catalysis. However, enzyme-based systems can suffer from limited stability and operational lifetime, and implantation introduces additional challenges that restrict long-term in vivo use. These limitations motivated the development of durable nonenzymatic electrocatalytic approaches for sustained, externally tunable, closed-loop glucose control.

In particular, electrocatalysis—accelerating chemical reactions at electrode surfaces—has recently come into the limelight in a variety of fields, such as sustainable energy storage (hydrogen production) $(59, 60)$ and carbon re- and upcycling $\left(\mathrm{CO}_{2}\right.$ reduction $(61, 62)$ . Electrocatalysts such as Pt-Ag nanoclusters $(63)$ , Au-doped $\mathrm{Co(OH)}_{2}$ nanoparticles $(64)$ , and Pt anchored on defective $TiO_{2}$ $(65)$ enable oxidation of glucose to high-value glucaric acid, which is found in fruits, honey, and wine. Also, nanoparticular electrode structures containing noble metals such as Pt and Au closely mimic the activity of glucose oxidase and can capture electrical energy, leading to applications in sensors and biofuel cells $(35, 66–72)$ . These advances underscore the promise of nonenzymatic electrocatalysts, which can offer improved robustness and tunability for sustained glucose modulation. Prior glucose biofuel cell studies established that catalytic materials can oxidize glucose in vivo $(35)$ , and classic metabolic work showed that gluconate is largely cleared or metabolized after systemic exposure $(43)$ . However, existing nonenzymatic glucose biofuel cells oxidize glucose continuously and do not enable externally tunable, on-demand glucose clearance $(66–72)$ .

Motivated by the need for controllable glucose clearance and by the limitations of chronic pharmacotherapy, including tolerability, adherence, and uncertain long-term safety (5, 14, 15, 56, 73–80), we developed an implantable, wirelessly powered electrocatalytic closed-loop health optimization (ECHO) device containing a composite electrocatalyst comprising platinum (Pt)-decorated gold (Au) nanoclusters integrated into a graphite felt (GF) matrix (GF\_Au@Pt). This ECHO device enables specific, electrically tunable oxidation of blood glucose to renally excreted gluconate at low input power. In a proof-of-concept study in obese mice with type 2 diabetes, the ECHO implant, linked through a smartphone to a commercial continuous glucose monitoring (CGM) device, automatically restored blood glucose homeostasis and shifted metabolic energy balance without drugs.

Figure 1 summarizes the operating principle and metabolic consequences of the ECHO system. The device operates in a closed loop to detect hyperglycemia and trigger on-demand electrocatalysis. When CGM readings exceed a preset threshold, the smartphone initiates wireless power transfer to the subcutaneous implant, where the GF\_Au@Pt catalyst oxidizes glucose to gluconate. This reduces circulating glucose and creates a controlled caloric sink, shifting substrate utilization toward lipid catabolism. Consequently, adipose lipolysis increases, free fatty acid concentrations rise, and hepatic ketogenesis is promoted. By maintaining glucose within the normoglycemic range without exogenous insulin, this closed-loop strategy couples glycemic control to a metabolic shift that can counteract diabetes-associated obesity.

Fig. 1. Closed-loop ECHO-CGM system for electrochemical management of diabesity. (A) Schematic of glucose regulation by the implanted ECHO system. Dietary glucose absorbed in the intestine enters the circulation and is monitored by a CGM. Under hyperglycemia, the subcutaneous ECHO implant catalyzes oxidation of glucose to gluconate, lowering circulating glucose. Reduced glucose availability promotes adipose lipolysis, converting triglycerides to glycerol and free fatty acids, which are further metabolized to ketone bodies and cleared via the kidneys. (B) Operating principle of the closed-loop ECHO-CGM system incorporating the GF\_Au@Pt electrocatalyst. When glucose is elevated (20 mM; ECHO ON), CGM feedback activates wireless power transfer and drives electrocatalytic conversion of glucose to gluconate. Under normoglycemia (10 mM; ECHO OFF), the wireless controller deactivates stimulation to maintain homeostatic glucose levels. (C) Conceptual therapeutic outcome. Subject A (pretreatment) exhibits elevated glucose and triglycerides, whereas subject B (posttreatment) shows restored metabolic balance after ECHO-assisted therapy. [Figure created with BioRender.com. Maity, D. (2026) https://BioRender.com/to7go11]

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Results

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Development and characterization of the GF\_Au@Pt electrocatalyst

Capitalizing on the intrinsic ability of Pt and Au to break down glucose, we synthesized a GF\_Au@Pt heterogeneous electrocatalyst by first assembling Au nanoflakes (around 150 nm in size) into spherical Au nanostructures (around 600 nm in size) on conductive high-porosity GF, then decorating these Au nanostructures with Pt dots. We constructed this structure by chemical deposition from Au and Pt salts using reducing $(\mathrm{NaBH}_{4})$ and complexing (ascorbic acid) agents in a hydrothermal reaction (24 hours, 150°C; and 1 hour, 80°C) (Fig. 2A).

We extensively characterized GF\_Au@Pt using scanning electron microscopy (SEM) (Fig. 2, B to D), low-magnification energy-dispersive spectroscopy (EDS) mapping (Fig. 2, E to H), high-resolution transmission electron microscopy (HR-TEM) (Fig. 2I), and high-magnification EDS mapping (Fig. 2, J to L), which confirmed the surface morphology of the Pt-decorated Au nanoclusters (Fig. 2, B to D). The Au nanoflakes (100 to $200\mathrm{nm}$ ) formed spherical structures (500 to $1000\mathrm{nm}$ ) on the porous nodule framework of the GF, providing ample internal space and a large surface area for catalytic activity. At higher magnification, Pt dots (<10 nm) are visible on the spherical Au clusters (Fig. 2I). EDS line-scanning spectra indicate homogeneous distribution of carbon (C), Au, and Pt, suggesting successful formation of the Au@Pt catalyst on the GF (Fig. 2, E to H). HR-TEM visualization and EDS elemental mapping of single Au flakes (around 100 nm in diameter) confirmed their decoration with Pt dots (<10 nm) (Fig. 2, I to L). Au flakes provide a stable, conductive, high-surface-area scaffold that supports Pt deposition and facilitates electron transport. Decorating the Au flakes with nanoscale Pt dots concentrates highly active surface motifs while minimizing precious-metal loading. Whereas Au alone exhibits limited glucose oxidation activity, Pt provides the dominant catalytic sites, and together, this Au flake/Pt dot architecture shows improved catalytic efficiency, selectivity, and stability relative to Au alone.

The high-resolution C 1s x-ray photoelectron spectroscopy (XPS) spectrum of pristine GF reveals characteristic peaks corresponding to $\mathfrak{sp}^2$ -hybridized carbon (284.49 eV), C-O bonds (285.97 eV), and O=C-O groups (289.56 eV), indicating the presence of oxygen-containing functional groups on the graphene framework (fig. S1A). After the incorporation of Au@Pt nanoparticles, the C 1s spectrum of GF\_Au@Pt shows dominant $\mathfrak{sp}^2$ carbon (284.42 eV) with a reduced intensity of oxygen-containing species (C-O

at 285.32 eV), suggesting partial reduction or surface modification during the synthesis process (fig. S1B). The Au 4f spectrum of GF\_Au@Pt shows well-defined doublets at 83.81 eV (Au $^{0}$ 4f $_{7/2}$ ) and 87.52 eV (Au $^{0}$ 4f $_{5/2}$ ), confirming the presence of metallic gold (Au $^{0}$ ) in the composite structure (Fig. 2M). The Pt 4f spectrum reveals the coexistence of metallic platinum (Pt $^{0}$ ) and oxidized platinum (Pt $^{2+}$ ) species, with peaks assigned to Pt $^{0}$ 4f $_{7/2}$ (71.13 eV) and Pt $^{0}$ 4f $_{5/2}$ (74.52 eV), along with Pt $^{2+}$ 4f $_{7/2}$ (71.72 eV) and Pt $^{2+}$ 4f $_{5/2}$ (74.90 eV) (Fig. 2N). The presence of both Pt oxidation states suggests partial surface oxidation of Pt nanoparticles during or after synthesis.

Electrochemical analysis of glucose oxidation by GF\_Au and GF\_Au@Pt

We first assessed the electrocatalytic glucose oxidation reaction (GOR) in a standard three-electrode setup under alkaline (1 M KOH) conditions at 21°C. We recorded linear sweep voltammetry profiles at a scan rate of 100 mV s $^{-1}$ for GF, Au-anchored GF (GF\_Au), and Pt-decorated Au-anchored GF (GF\_Au@Pt) in the presence and absence of 20 mM glucose (Fig. 3A). The profiles confirm the occurrence of the oxygen evolution reaction (OER) in the presence of GF, GF\_Au, and GF\_Au@Pt at a potential of 1.26 V versus RHE (reversible hydrogen electrode) delivering a current density of 30 mA cm $^{-2}$ . Upon addition of 20 mM glucose, GOR of GF\_Au and GF\_Au@Pt could be recorded at 0.7 and 0.6 V versus RHE knee voltage, respectively (no knee voltage for pure GF), indicating that GOR is kinetically more favorable than OER (Fig. 3A). Notably, there is no GOR in the absence of electrical power and below the knee voltage of 0.6 V. GOR's catalytic current densities of 25 mA cm $^{-2}$ (GF\_Au) and

Fig. 2. Synthesis and analysis of gold-platinum nanoclusters on graphite felt substrate. (A) Schematic illustration of the synthesis of platinum-decorated gold nanoclusters integrated into a graphite felt matrix, serving as electrocatalyst for electro-controlled glucose oxidation. $C_{6}H_{8}O_{6}$ , ascorbic acid; GF, graphite felt; GF\_Au, GF-integrated gold nanocluster; GF\_Au@Pt, GF-integrated platinum-decorated gold nanocluster; HAuCl $_{4}$ , chloroauric acid; H $_{2}$ PtCl $_{4}$ , chloroplatinic acid; NaBH $_{4}$ , sodium borohydride; NaOH, sodium hydroxide. [Panel created with BioRender.com. Maity, D. (2026) https://BioRender.com/jwq27ew] (B to D) Scanning electron micrographs of GF\_Au@Pt at different magnifications: 2360× (B), 20,070× (C), and 76,730× (D). (E to H) EDX spectroscopy mapping of GF\_Au@Pt (E) showing elemental distribution of carbon (F), gold (G), and platinum (H). (I to L) Scanning transmission electron micrographs of a single Au@Pt nanoflake at 600,000× (I) and 200,000× (J) magnification with corresponding EDX spectroscopy mapping of Au (K) and Pt (L). (M and N) XPS spectra of GF\_Au@Pt showing Au 4f (M) and Pt 4f (N) regions, confirming surface composition and chemical states. a.u., arbitrary units.

50 mA cm $^{-2}$ (GF\_Au@Pt) were reached at 0.75 V. GF\_Au@Pt's catalytic activity outperformed that of GF\_Au, as it reached higher current density (50 mA cm $^{-2}$ ) at lower voltage (0.75 and 1.25 V versus RHE, respectively), confirming both the synergistic effect of Pt decoration on the Au flakes and efficient glucose oxidation by GF\_Au@Pt (Fig. 3A). Nyquist plots confirmed that GF\_Au@Pt shows lower charge-transfer resistance owing to higher glucose adsorption, consistent with faster glucose oxidation compared with GF\_Au (Fig. 3B). Double-layer capacitance ( $C_{dl}$ ) values of GF, GF\_Au, and GF\_Au@Pt in the non-Faradaic region were 0.14, 0.27, and 0.30 mF cm $^{-2}$ , respectively (fig. S1, C to F), confirming the higher active surface area of GF\_Au@Pt and GF\_Au compared with GF. Overall, the GF\_Au@Pt catalyst outperformed GF\_Au in all respects and showed a direct correlation between glucose level and glucose oxidation over the entire physiological glucose concentration range without saturation of catalytic activity (Fig. 3C). GF\_Au@Pt exhibits maximal GOR activity in an alkaline electrolyte, while retaining substantial activity under near-physiological conditions (fig. S2).

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Performance profiling and specificity of GF\_Au@Pt-based glucose oxidation

The voltage decrease associated with electrified GF\_Au@Pt indicates a shift from OER to GOR, and we identified gluconate as the glucose oxidation product. Liquid chromatography–mass spectrometry (LC-MS) and ${}^{1}H-{}^{13}C$ heteronuclear multiple bond correlation (HMBC) analyses confirm selective electrochemical oxidation of glucose to gluconate (glucose → gluconate), supporting high reaction selectivity under ECHO operating conditions (figs. S3 and S4). This confirms that GF\_Au@Pt-based glucose oxidation proceeds via the following two-electron transfer process: $C_{6}H_{12}O_{6}$ (glucose) + 2 OH $^{-}$ → $C_{6}H_{12}O_{7}$ (gluconate) + H $_{2}$ O + 2e $^{-}$ . When GF\_Au@Pt, immersed in 30 mM glucose solution, was powered at 0.75 V and 10 mA, the glucose concentration started to decrease within 30 min and reached 7 mM after 2 hours. Concomitantly, the gluconate concentration increased to 12 mM (Fig. 3D). While glucose oxidation reached a steady state under these in vitro conditions, GF\_Au@Pt activation continuously converted glucose to gluconate, demonstrating sustained electrochemical glucose clearance. In vivo, \~90% of gluconate is renally cleared, whereas a smaller fraction enters intermediary metabolism. We therefore hypothesized that ECHO-mediated glucose oxidation would lower circulating glucose while removing part of its caloric load (35, 43, 81, 82).

Comprehensive performance analyses showed that electro-triggered GF\_Au@Pt-mediated glucose oxidation is robust across conditions and exhibits little dependence on glucose concentration over the tested range (Fig. 3E). In contrast, the glucose oxidation rate increases with

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Fig. 3. GF\_Au@Pt-mediated electrocatalytic glucose oxidation. (A) Linear sweep voltammetry of GF, GF\_Au, and GF\_Au@Pt-mediated glucose oxidation (20 mM glucose, 1 M KOH, scanning rate 100 mV/s). (B) Electrochemical impedance spectroscopy of GF, GF\_Au, and GF\_Au@Pt during glucose (20 mM) oxidation recorded at 0.75 V against a RHE. (C) Changes in current density of GF\_Au@Pt catalyst with glucose concentration in the range of 1 to 50 mM. (D to G) Dependence of GF\_Au@Pt-mediated electrocatalytic glucose oxidation [Dulbecco's phosphate-buffered saline (DPBS), 10 ml, 10 mA, 0.75 V] and gluconate production on (D) electrostimulation time, (E) glucose concentration (DPBS, 10 ml, 10 mA, 0.75 V), (F) GF\_Au@Pt electrode surface area (DPBS, 20 mM glucose, 10 mA, 10 ml, 1 hour, 0.75 V), and (G) sample volume (DPBS, 10 mA, 2 hours, 0.75 V). (H) Reversibility of GF\_Au@Pt-mediated electrocatalytic glucose oxidation (30 mM glucose, 10 ml, 2 hours, 0.75 V, 10 mA, 1 cm by 1 cm surface area). (I) Chronoamperometric analysis of GF\_Au@Pt-mediated electrocatalytic glucose specificity in the presence of physiological concentrations of the indicated metabolites (0.75 V, 10 ml, PBS). Data are represented as mean ± SEM ( $n = 5$ biological replicates). Statistical significance was determined using two-way analysis of variance (ANOVA) with Dunnett's multiple comparisons test.

GF\_Au@Pt working area (Fig. 3F) and decreases with increasing reaction volume (Fig. 3G). Furthermore, performance is reversible and stable during prolonged operation (Fig. 3H), consistent with the material integrity of GF\_Au@Pt (fig. S5).

Under all conditions examined, electro-triggered GF\_Au@Pt activation exclusively oxidized glucose without targeting other sugars or representative electroactive molecules (Fig. 3I). Linear sweep voltammetry and amperometric analyses showed that GF\_Au@Pt was electrochemically specific for glucose under the tested conditions, as metabolites, proteins, hormones, vitamins, and drugs tested at 5- to 10-fold physiological concentrations produced negligible current responses and did not measurably interfere with glucose oxidation (figs. S6 and S7).

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Electrotunability of GF\_Au@Pt-mediated glucose oxidation

Restoring blood glucose homeostasis in type 2 diabetes and resetting the metabolic energy balance for the treatment of obesity require precise and dynamic control of electrocatalytic GF\_Au@Pt activity. To comprehensively analyze electrotunability of GF\_Au@Pt-mediated electrocatalytic glucose oxidation, we immersed GF\_Au@Pt in a physiological saline solution containing $30~\mathrm{mM}$ glucose and varied the voltage at a fixed current while profiling glucose-clearance kinetics. The electrochemical onset (knee) voltage for GF\_Au@Pt-mediated glucose oxidation was approximately 0.6 V, while 0.75 V was used as the practical operating voltage to achieve efficient glucose oxidation (Fig. 3A). Next, with the activation threshold voltage set to 0.75 V, we recorded the glucose oxidation rate while varying the current (Fig. 3D). The results confirmed that the glucose concentration could be precisely adjusted to desired levels by tuning the input power. GF\_Au@Pt displays a concentration-dependent increase in glucose oxidation rate over the tested range (fig. S8). Overall, these findings demonstrate that GF\_Au@Pt-mediated GOR can be fine-tuned and scaled as required by adjusting (i) the surface area of GF\_Au@Pt, (ii) the operating time, and (iii) the electrical power, suggesting that the electrocatalyst can be flexibly adapted to different systems and conditions. Chlorine and reactive oxygen species (ROS) assays showed no detectable oxidant generation at the ECHO operating potential of 0.75 V, supporting a nonoxidative operating window and good biocompatibility in accordance with the results of cytotoxicity testing (figs. S9 and S10).

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Electrocatalytic closed-loop control of GF\_Au@Pt-mediated glucose oxidation

Having established that GF\_Au@Pt-mediated glucose oxidation can be electrically tuned, we next asked whether this reaction could be coupled to real-time glucose sensing to create closed-loop control over glucose clearance. In preparation for using GF\_Au@Pt-mediated GOR for dynamic closed-loop control of blood glucose, we first simulated prandial glucose intake by addition of glucose at regular intervals during electrocatalyst operation. Then, to simulate closed-loop control, we connected electrotunable GF\_Au@Pt activation to glucose-level input data from a commercial CGM device. In this system, the CGM detected simulated postprandial glucose spikes in real time and repeatedly activated GF\_Au@Pt electrocatalysis. This setup maintained glucose near the preset 5 mM target by dynamically switching electrocatalytic glucose oxidation on and off (fig. S11).

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Construction of wirelessly powered ECHO implants for tunable glucose oxidation

To enable drug-free real-time wireless-powered electrotunable blood glucose control, we assembled the GF\_Au@Pt electrocatalyst and associated switchboard electronics in a sealed IPX7-certified waterproof (IEC 60529) 3D-printed US Food and Drug Administration (FDA)-licensed polyamide casing [26 mm by 14 mm by 5 mm, length × width × height (LWH)] (fig. S12). The ECHO module features a compact, polyamide-encapsulated printed circuit board that provides biocompatible electrical insulation (fig. S12). A dual-layer radiofrequency regulator stabilizes wireless power delivery (fig. S13), and a 13.56 MHz transmitter enables efficient power transfer and synchronized activation for closed-loop electrocatalysis (figs. S14 and S15). The switchboard also contains a receiver coil synchronizing power transfer from the emitter coil of the extracorporeal power generator at an industrial, scientific, and medical (ISM) band frequency of 13.56 MHz. For increased biocompatibility, we encapsulated the bioelectronic GF\_Au@Pt-containing implant in a three-layer structure consisting of a BioGlue-sealed polycellulose bag and alginate coating, with EDC-NHS [1-ethyl-3-(3-dimethylaminopropyl)carbodiimide-N-hydroxysuccinimide] surface functionalization of the alginate layer. The ECHO-CGM system integrates continuous glucose sensing with wireless electrocatalytic feedback to enable autonomous, biocompatible glucose regulation through closed-loop electrochemical control (fig. S16). The final GF\_Au@Pt-containing ECHO implants retained their electrochemical glucose-oxidation activity after 3 months of subcutaneous implantation in obese type 2 diabetic (db/db) mice (fig. S17).

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Electrocatalytic blood glucose control managing type 2 diabetes and associated obesity

To validate drug-free electrocatalytic control of blood glucose concentrations and diabetes-associated obesity, we implanted the ECHO device in db/db mice (fig. S18) and measured the blood glucose responses across applied voltages from 0 to $0.9\mathrm{V}$ (Fig. 4A) and currents from 0 to $10\mathrm{mA}$ (Fig. 4B). We found that operating at $0.75\mathrm{V}$ and $10\mathrm{mA}$ was sufficient to drive efficient blood glucose oxidation. Upon activation of the ECHO implant at $0.75\mathrm{V}$ and $10\mathrm{mA}$ , normoglycemia is achieved within 60 to $90\mathrm{min}$ (Fig. 4C), which is comparable to the postprandial blood glucose profile of wild-type (WT) mice (Fig. 4D) as also observed in glucose tolerance test (GTT) (fig. 4E). These results show that electrocatalytic glucose clearance can reduce hyperglycemia on a timescale comparable to physiological postprandial glucose normalization in WT mice. Hyperglycemia gradually returned after switching off electrocatalysis (Fig. 4D). Repeated activation of ECHO-controlled electrocatalytic glucose oxidation for different time periods confirmed rapid and reversible blood glucose control, suggesting that ECHO can provide robust, reproducible, and precise dynamic control of blood glucose in experimental type 2 diabetes (Fig. 4F). With optimal stimulation power $(0.75\mathrm{V}, 10\mathrm{mA})$ and activation time $(60\mathrm{min/day})$ , hyperglycemic excursions could be consistently attenuated to reach normoglycemia and manage experimental type 2 diabetes for at least a 6-week period (Fig. 4, F and G). Blood pH remained stable and never decreased below 7.35, indicating that the bicarbonate buffering system (37) was unaffected by gluconate produced by ECHO-triggered glucose oxidation, and suggesting the absence of ketoacidosis (fig. S19). Inductively coupled plasma mass spectrometry (ICP-MS) and SEM-EDX (energy-dispersive x-ray) analyses support the chemical and structural stability of the GF\_Au@Pt electrocatalyst, with no Au or Pt detectable in serum or organ tissues under the tested conditions (table S1 and fig. S20). These findings indicate that the alginate-polycellulose encapsulation effectively limits systemic metal exposure, and they also support in vivo biostability of the ECHO system.

In contrast to classical blood glucose management, which focuses on insulin-triggered glucose uptake and metabolism by individual cells, ECHO-based electrocatalytic conversion of glucose into renally cleared gluconate results in a decrease of overall systemic metabolic energy, which is expected to favor a shift from glucose- to fat-based energy metabolism and may therefore reduce diabetes-associated obesity. Indeed, db/db mice treated for a 6-week period with ECHO-based electrocatalytic glucose oxidation not only had their normoglycemia restored but also lost up to 10% of their body weight (Fig. 5A). Reduced insulin concentrations in ECHO-treated type 2 diabetic (T2D) mice are consistent with improved glycemic control and may reflect enhanced insulin sensitivity (Fig. 5B). Furthermore, the animals showed lower concentrations of blood triglycerides (Fig. 5C) as well as higher amounts of free fatty acids (Fig. 5D) and ketone bodies (Fig. 5, E and F) compared with untreated T2D and WT animals, confirming the electrocatalytically mediated transition from glucose- to fat-based metabolism. Notably, ECHO's electrocatalyst remained fully intact, and explanted devices exhibited native performance (fig. S17). Electrocatalytic glucose oxidation may therefore provide a drug-free route to modulate both hyperglycemia and obesity-associated metabolic features in experimental diabesity. During the clamp procedure, the ECHO system maintained glucose within the euglycemic range, supporting effective control without evidence of hypoglycemia under the tested conditions.

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Closed-loop electrocatalytic blood glucose oxidation for treatment of diabesity

As with any open-loop therapeutic intervention, hypoglycemic excursions and excessive metabolic energy depletion associated with open-loop drug-free electrocatalytic glucose oxidation cannot be completely mitigated. We therefore constructed a dynamic, closed-loop system by interfacing the ECHO implant with a commercial CGM device (fig. S18). This CGM device profiles interstitial glucose concentration in real time and wirelessly transfers the data to a compatible reader or smartphone, which was programmed to wirelessly activate the ECHO implant whenever glucose reached hyperglycemic levels (Fig. 6A and movie S1). To optimize the closed-loop control dynamics and prevent hypoglycemic excursions, we profiled the closed-loop ECHO-CGM communication and control system at various threshold glucose concentrations (5 to 15 mM glucose; Fig. 6B) and ECHO activation cycles (5 to 30 min; Fig. 6C). This characterization revealed that the closed-loop ECHO-CGM system could be set to any glucose threshold in the above range and that short ECHO activation cycles of 5 min were sufficient to provide stable glucose homeostasis and prevent hypoglycemic excursions (Fig. 6C and movie S2). During the licensed lifespan of the CGM (12 days) (83–86), the closed-loop ECHO-CGM system provided automatic, robust, and stable glucose homeostasis in implanted T2D mice (Fig. 6D and movie S2). Cytokine profiling together with histological and immunohistochemical analyses revealed no marked differences in systemic inflammatory cytokines or local inflammatory cell infiltration between stimulated and nonstimulated T2D cohorts, supporting preserved tissue integrity and controlled remodeling at the device-tissue interface over 30 days in vivo (figs. S21 to S23).

The loss of metabolic energy resulting from the glucose drain driven by the electrocatalytic glucose oxidation also induced a shift to fat-based energy metabolism, characterized by lower blood triglyceride concentrations (Fig. 6E), higher blood fatty acids (Fig. 6F), and higher ketone body concentrations (Fig. 6, G and H), indicating that ECHO stimulation induced a shift from glucose-based to fat-based metabolism. Consistent with this, hyperinsulinemic-euglycemic clamp studies showed that ECHO-treated diabetic mice required significantly higher glucose infusion rates than unstimulated diabetic controls under controlled glycemic conditions (fig. S24; P < 0.0001). Under the tested dosing regimens, ECHO electrocatalysis produced rapid glucose lowering with stable CGM profiles and no hypoglycemic overshoot compared with the pharmacological comparator groups (fig. S25). The platform further showed scalable and stable glucose oxidation in a 5-liter-scale circulation setup, with larger GF\_Au@Pt electrodes increasing catalytic capacity and enabling near-complete oxidation. These results support further preclinical development and demonstrate scalable glucose oxidation under human volume-relevant perfusion conditions (fig. S26).

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Fig. 4. ECHO-controlled blood-glucose levels in experimental type 2 diabetes. (A and B) Blood glucose profiles of ECHO-implanted T2D mice stimulated with different voltages (A) and currents (B). (C) Blood glucose profiles of ECHO-implanted T2D mice [T2D-ECHO (On)] stimulated with 0.75 V and 10 mA compared with WT, untreated T2D, unstimulated ECHO-implanted [WT+ECHO (Off)], and unstimulated ECHO-implanted [T2D+ECHO (Off)] animals. (D) Real-time ECHO-mediated blood glucose control of T2D mice repeatedly stimulated for different periods of time with 0.75 V and 10 mA. (E) GTTs of WT, T2D, WT+ECHO (Off), and T2D+ECHO (Off) animals, and ECHO-implanted stimulated (0.5 cm $^{2}$ , 0.75 V and 10 mA) T2D mice. (F and G) Long-term blood glucose profiling of WT, T2D, and ECHO-implanted T2D mice stimulated once daily with 0.75 V and 10 mA. Blood glucose levels were monitored daily for 7 days (F) and weekly for 6 weeks (G). Error bars represent mean ± SEM ( $n = 8$ biological replicates). Statistical significance was determined using two-way ANOVA with Tukey's multiple comparisons test.

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Discussion

Glucose is the major metabolic energy carrier in mammals, providing short-term power (87, 88). It is supplied by dietary intake and internally produced by gluconeogenesis in the liver, and blood glucose homeostasis is maintained by insulin-triggered cellular glucose uptake and consumption as well as by conversion into fatty acids and triglycerides for reversible longer-term energy storage (1, 88). Imbalanced and chronically elevated blood glucose is the root cause of diabesity, with interlinked pathophysiology and comorbidities of diabetes and obesity (5, 14, 15). The range of drug-based therapies for diabesity, designed to directly or indirectly address chronically elevated blood glucose concentrations, includes treatments such as gluconeogenesis blockers (79, 89), insulin and insulinogenic peptide hormones [GLP-1 (90), GIP (91), and adiponectin (92)], and drugs such as semaglutide (23, 45, 46) and tirzepatide (22, 23). Additionally, advanced cell therapies are currently undergoing proof-of-concept studies or are in preclinical development (87). However, like all drug-, gene-, or cell-based treatment strategies, current diabesity therapies are limited by challenging control dynamics, side effects, poor patient adherence, high cost per dose, and the need for lifelong administration (93, 94). Therefore, for next-generation medicine, the quest for control modalities providing reversible, adjustable, and

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Fig. 5. Impact of ECHO-controlled blood glucose homeostasis on interlinked obesity. Body weight (A) and concentrations of insulin (B), triglycerides (C), free fatty acids (D), $\beta$ -hydroxybutyrate (E), and acetoacetate (F) in WT, T2D, and ECHO-implanted T2D mice stimulated once daily with $0.75\mathrm{V}$ and $10\mathrm{mA}$ for at least 6 weeks. Error bars represent mean $\pm$ SEM ( $n = 8$ biological replicates). Statistical significance was assessed using two-way ANOVA with Tukey's multiple comparisons test.

dynamic control of therapeutic interventions is ongoing (24, 25, 95, 96). Early efforts centered on open-loop therapeutic transgene control using small-molecule compounds enabling oral (21, 24, 25, 29, 30, 40, 96–106), percutaneous (100, 107), and inhaled administration (27–30, 105). Subsequently, pioneering closed-loop systems that dynamically coordinate biomarker input to control implanted designer cells (21) have been successfully used for the treatment of diverse conditions (35, 36, 103, 108). A range of gene switches and therapeutic gene networks responsive to nonmolecular physical cues such as light (31–34), temperature (109, 110), mechanical pressure (111), and sound (112, 113) have similarly advanced genetic precision control, and the emerging science of electrogenetics, which interfaces wearable electronics with metabolism using electrical fields (114), direct current (115), and electromagnetic fields (116), has enabled remote control of therapeutic gene expression (31, 32, 117, 118). Recent advances in electrogenetics have also incorporated material science to expand the reaction space by using catalytic nanocomposite materials. A notable example includes a metabolic fuel cell, in which a cuprous oxide-containing nanocomposite material continuously catalyzes blood glucose oxidation, producing a glycemia-correlated direct current (35, 108). An electronic power-management circuit draws direct current only during hyperglycemia and electrostimulates coimplanted designer cells either optogenetically or directly to produce and release insulin, restoring normoglycemia in a closed-loop manner $(35, 108)$ . Wireless control and information exchange are mediated by wearable devices and smartphones. However, as the glucose-to-direct current conversion is irreversible, the nanocomposite material of the metabolic fuel cell cannot operate in the reverse mode: fine-tuning blood glucose concentrations by adjusting direct current input.

Building on prior work showing that nanocomposite materials can interface glucose oxidation with bioelectronics $(35)$ and on advances in noble metal electrocatalyst design $(35, 119–121)$ , we designed GF\_Au@Pt for a distinct purpose: externally powered, reversible, and tunable glucose oxidation rather than continuous glucose-to-current conversion. The resulting electrocatalyst consists of high-porosity conductive graphite felt with Au nanoflakes assembled into spherical nanostructures decorated with Pt dots. This structure facilitates efficient electron transfer and enhances glucose accessibility owing to its high surface area. The flower-shaped Pt dot-decorated Au framework promotes glucose adsorption and improves oxidation kinetics, resulting in superior overall reaction performance compared with conventional noble metal catalysts. This hierarchical structure showed high morphological stability over extended operation times, rapid electron-transfer kinetics, and high specificity for glucose, and it enabled reversible and

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Fig. 6. Smartphone-enabled closed-loop control of glucose homeostasis using a commercial continuous glucose monitoring device integrated with the ECHO system. (A) Schematic representation of the smartphone-enabled wireless closed-loop CGM-ECHO integration to control glucose homeostasis in T2D mice. The commercial CGM continuously profiles glucose levels in real time and initiates wireless stimulation of the ECHO implant when glucose levels rise above a preset threshold concentration. [Panel created with BioRender.com. Maity, D. (2026) https://BioRender.com/Obj48wp] (B) Glucose homeostasis kinetics in response to different preset glucose threshold concentrations. (C) Impact of different ECHO stimulation times (0.5 cm $^{2}$ , 0.75 V, 10 mA) and glucose homeostasis kinetics in ECHO-implanted T2D mice. (D) Autonomous maintenance of glucose homeostasis of T2D mice controlled by the integrated closed-loop CGM-ECHO device during the licensed CGM lifespan of 12 days. (E to H) Impact of CGM-ECHO treatment on obesity. Concentrations of triglycerides (E), free fatty acids (F), acetoacetate (G), and β-hydroxybutyrate (H). Animal groups included WT mice and T2D mice, both with CGM; WT mice and T2D mice equipped with the closed-loop CGM-ECHO system but not stimulated (Off); and T2D mice equipped with the closed-loop CGM-ECHO system and stimulated (On). Data are represented as mean ± SEM ( $n = 8$ biological replicates). Statistical significance was assessed using two-way ANOVA with Dunnett's multiple comparisons test.

precisely tunable glucose oxidation in the physiological range using low electrical power (less than or equal to the power required by pacemakers). Most importantly, the GF\_Au@Pt electrocatalyst exhibited rapid electrotunability, efficiently restoring postprandial blood glucose concentrations with kinetics comparable to those observed in WT or insulin-treated T2D mice, without occurrence of hypoglycemia or associated behaviors such as shivering. In contrast to native physiology or insulin-based therapies where the body's overall metabolic energy level remains constant after hormone-triggered cellular glucose uptake, electrocatalytic glucose oxidation produces gluconate, 90% of which is rapidly cleared by the kidneys, resulting in a net decrease in overall systemic metabolic energy (35, 43, 81, 82). Notably, we did not observe gluconate-associated acidosis during this process, indicating that the body's bicarbonate buffering system remains effectively regulated (37). These results suggest that the electrocatalytic gluconate-based approach to reducing net metabolic energy (43, 81) can reset the body's overall metabolic load by promoting fat mobilization while preventing further fat accumulation. Electrocatalytic regulation of blood glucose homeostasis also resulted in lower blood triglyceride concentrations, higher circulating free fatty acids, increased ketone body production, and reduced body weight—all achieved with no detectable change in food intake. These effects align closely with outcomes previously observed using cell-based appetite suppression strategies tailored for managing diet-induced obesity (39).

Throughout prolonged periods of diabesity management, the electrocatalytic implant was stable, maintaining its native performance without apparent local inflammation or elevation in systemic inflammatory biomarkers. Moreover, ECHO operation did not alter feeding habits or overall behavior of the animals, further supporting tolerability under the tested in vivo conditions. In particular, the absence of altered eating behavior and hypoglycemic episodes highlights a potential advantage of drug-free electrocatalytic glucose modulation, which avoids systemic exposure to glucose-lowering drugs in this experimental setting. This drug-free mode of action is relevant because current pharmacological therapies for diabesity can be limited by adverse effects, tolerability, adherence, cost, and unresolved long-term safety questions (122).

The electrocatalytic ECHO device can seamlessly integrate with modern electronics and can in principle connect to a variety of wearable devices, smartphones, and cloud-based Internet of Things networks. This enables real-time monitoring, online diagnostics, and therapeutic interventions, by either the patient or medical professionals, or through artificial intelligence-driven algorithms that anticipate daily routines and lifestyle changes. As a proof of concept, we wirelessly linked the ECHO device implanted in T2D obese mice to a commercial CGM system. The CGM system tracked glucose concentrations and transmitted the data to a smartphone, which processed the data and sent instructions back to the ECHO device, which in turn rapidly adjusted glucose concentrations to maintain homeostasis in response—achieving this without hypoglycemic episodes or the need for small-molecule drugs or biopharmaceuticals. Standard practice for CGM-licensed applications is to replace the CGM every 12 days (16, 83–86). Because the electrocatalyst was not consumed or degraded over this timescale, and because the ECHO implant showed preserved local tissue compatibility, longer-term drug-free modulation of glucose and metabolic energy balance may be feasible with routine CGM replacement, provided that implant performance and tissue compatibility remain stable over extended periods. We believe that closed-loop electrocatalytic devices could establish a platform concept for regulating disease-relevant metabolites, offering a potential route toward drug-sparing, dynamically controlled metabolic interventions.

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Materials and methods Chemicals

Chloroplatinic acid (H $_2$ PtCl $_6$ ), chloroauric acid (HAuCl $_4$ ), sodium borohydride (NaBH $_4$ ), ascorbic acid (C $_6$ H $_8$ O $_6$ ), glucose (C $_6$ H $_{12}$ O $_6$ ), hydroxylamine hydrochloride (NH $_2$ OH·HCl), $N$ -hydroxysuccinimide (NHS, C $_4$ H $_5$ NO $_3$ ), phosphate-buffered saline (PBS), $N,N'$ -bis(acryloyl)cystamine (BAC), polycellulose, sodium dodecyl sulfate (SDS), 1-ethyl-3-(3-dimethylaminopropyl) carbodiimide (EDC), 2,2'-azobis(2-methylpropionamidine)dihydrochloride (AAPH), and bovine serum albumin (BSA) were purchased from Sigma-Aldrich. Glucose-to-gluconate conversion was quantified using a colorimetric D-Gluconate Assay Kit (Sigma-Aldrich, MAK279). Alginate was purchased from Buechi AG (cat. no. 11061528). Acetone, carbon black, ethanol, potassium hydroxide (KOH), and sodium hydroxide (NaOH) were sourced from ThermoFisher Scientific. Platinum (Pt) round wire (0.50 mm diameter, density 20.10 g/cm $^3$ ) was bought from Cooksongold, silver ink (cat. no. 186-3600) from RS Components, graphite felt (GF, cat. no. G100) from Fuel Cell Store, and BioGlue (cat. no. BG3510-5-US) from CryoLife Inc. Integrated circuits (LT3092ETS8), ceramic capacitors (MC0402), diodes (Diodes Inc., 1N4148; ST Microelectronics, BAT54J), and other small electronic components such as resistors were obtained from Digi-Key Inc.

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Electrocatalyst fabrication

Graphite felt preparation: GF was cut into 5 cm by 5 cm squares, which were washed once with 70% (v/v) ethanol, dried overnight at 21°C, autoclaved in double-distilled water (ddH₂O) at 120°C for 24 hours to remove loose nanofibers and activate the GF surface, washed in ddH₂O, and vacuum-dried at 40°C overnight.

Synthesis of GF\_Au electrocatalyst: Au nanoclusters were synthesized by mixing 10 ml of HAuCl $_4$ solution (10 mM) with 10 ml of NaOH solution (0.1 M). The mixture was stirred for 30 min and sonicated for 30 min at 21°C (82% amplitude, 20 kHz, 250 W, 5 s on/off cycles; Sonopuls

HD4100, Bandelin Electronic GmbH), then the activated GF was added, followed by 1 ml of $NaBH_{4}$ (0.001 M) and 1 ml of ascorbic acid (0.1 mM). After mixing for 5 min, the immersed GF was collected and incubated in an airtight hydrothermal autoclave reactor for 24 hours at 150°C to complete the flake-based Au cluster formation on the GF. The hydrothermal autoclave reactor was then rapidly cooled in a water bath set to 21°C—this is crucial to maintain the flake-based Au clusters anchored on the GF (GF\_Au) (Fig. 2C). The GF\_Au was collected, washed five times with 70% (v/v) ethanol, and vacuum-dried at 50°C overnight.

Synthesis of GF\_Au@Pt electrocatalyst: To decorate the flake-based Au clusters anchored on the GF with platinum, we immersed GF\_Au in 30 ml of $H_{2}PtCl_{6}$ (1 mM) and centrifuged it at 8000g for 20 min. The GF\_Au was transferred to a mixture of 40 ml of ascorbic acid (0.1 mM) and 5 ml of $NaBH_{4}$ (0.001 M), incubated for 1 hour at 80°C under stirring at 100 rpm, washed six times in an acetone- $ddH_{2}O$ mixture (1:10), and vacuum-dried at 45°C for 48 hours to afford Pt-decorated flake-based Au cluster-anchored GF, the final GF\_Au@Pt electrocatalyst, which was ready to be placed in the wireless-powered implant.

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ECHO device

The ECHO device was assembled sequentially, including the wireless-powered electronics, the GF\_Au@Pt plug-in and the encapsulation of the biocompatible implant. Electronics: (i) Field generator. We constructed a field generator to wirelessly power and control the bioelectronic ECHO implant. The 35.5 cm by 19.5 cm by 10 cm (LWH) field generator incorporates components such as a frequency generator using an oscillating circuit and impedance converter amplifying the transistor's output signal, which drives the resonance unit (13.56 MHz) of the transmitter coil and wirelessly transfers electromagnetic power to the receiver coil of the ECHO implant. (ii) Wireless-powered bioelectronic ECHO implant. The wireless-powered bioelectronic ECHO implant casing (26 mm by 14 mm by 5 mm, LWH), fabricated from 3D-printed (Formiga P110 3D printer; EOS GmbH, Krailling, Germany) FDA-licensed polyamide (Fabb-It 3D Druckservice, Loerrach, Germany), contains the receiver coil that collects the electromagnetic output of the power generator at the resonance frequency and rectifies it to direct current through diodes. The direct current power activates ECHO's custom-printed switchboard (22 mm by 8 mm by 0.7 mm) containing a programmable two-terminal current source (IC LT3092) that regulates device operation, capacitors (C4, C5) to adjust the resonance frequency, resistance (R1) to control the output current, and diodes (D3, D4) to control the output voltage at the anode containing the plugged-in GF\_Au@Pt electrocatalyst (0.5 cm $^{2}$ ), fixed with conductive silver ink. To prevent any short circuit, the anode and catalyst were insulated with BioGlue. The cathode consisted of a platinum wire (diameter 0.5 mm, length 10 mm). The circuit diagram and a list of electronic components are provided in figs. S12 to S16 and table S2. Overall, the ECHO device was rated IPX7 waterproof according to the International Protection Marking standards (IEC 60529). (iii) ECHO implant encapsulation. To improve its biocompatibility, we encapsulated the ECHO implant in a three-layer structure consisting of polycellulose, alginate, and EDC-NHS for surface functionalization. We first packed the ECHO device in a polycellulose membrane bag sealed with BioGlue and then covered the bag with alginate by immersing it in 0.2 (wt %) alginate solution for 6 hours at 21°C and dipping it for 30 min in 0.1 M CaCl $_{2}$ to allow polymerization. The alginate-covered ECHO bag was then washed three times with ddH $_{2}$ O and functionalized on its surface with EDC-NHS by immersing it for 2 hours in a 1:1 solution containing 0.2 M EDC and 0.05 M NHS, then incubating it for 2 hours in 1 M Na $_{2}$ HPO $_{4}$ , followed by washing four times in ddH $_{2}$ O. This process was repeated three times. The EDC-NHS-alginate ECHO-bag was then immersed for 10 min in 0.1 M BSA, washed once in PBS, and UV-sterilized for 30 min. The final ECHO implant (30 mm by 17.5 mm by 10 mm, LWH) was stored at 4°C until required.

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GF\_Au@Pt analysis

Scanning electron microscopy (SEM, FEI Versa 3D DualBeam) and scanning transmission electron microscopy (STEM, JEOL JEM-F200 cFEG) were used to analyze the structural properties of GF\_Au@Pt. X-ray photoelectron spectroscopy (XPS) was performed using a VG ESCALAB 210 system (VG Scientific Ltd., East Grinstead, UK). Infrared thermal imaging was performed using a FLIR E8 Pro (Teledyne FLIR LLC, USA). Elemental mapping was conducted using energy-dispersive x-ray spectroscopy (EDS, Zeiss GeminiSEM 450). Selected-area electron diffraction (SAED, JEM-F200(HRP)) was used for crystallographic characterization. Electrochemical analyses such as cyclic voltammetry (-0.2 to 0.2 V, 20 to 100 mV/s), linear sweep voltammetry (0 to 1.4 V, 100 mV/s), and electrical impedance spectroscopy (100 kHz to 0.1 Hz, 100 mV amplitude) were performed on a CH Instruments electrochemical workstation (CHI660) using GF\_Au@Pt, RHE as a reference and platinum as counter electrodes immersed in PBS (pH 7.4, 37°C and 1 M KOH, 21°C). Electrocatalysis dynamics of GF\_Au@Pt were recorded using GF\_Au@Pt as the anode and platinum as the cathode. The RND LAB DC Power Supply (Model: RND 320-KD3005D, China) was used to provide a stable DC power source during the electrocatalysis experiments.

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Measurement of chlorine gas

Dissolved chlorine was measured using DPD-1 test strips (cat. no. 486637) with an eXact EZ photometer (cat. no. 486205) (ITS Europe).

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ROS quantification

Electrostimulated DCINS cells were washed with PBS (300 $\mu$ l; cat. no. 14190-094, Thermo Fisher Scientific) and incubated for 45 min in serum-free Dulbecco's modified Eagle's medium (DMEM; 500 $\mu$ l) containing 25 $\mu$ mol liter $^{-1}$ 2',7'-dichlorofluorescein diacetate (cat. no. D6883, Sigma-Aldrich) (115). Cells were rinsed with PBS (300 $\mu$ l), and ROS levels were quantified fluorometrically (excitation/emission, 485/535 nm) using a Tecan Infinite 200 PRO plate reader.

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Infrared thermal imaging

Infrared thermal imaging (FLIR E8 Pro, Teledyne FLIR LLC, USA) detected no measurable temperature increase ( $\pm0.1^{\circ}C$ ) after 2 hours of operation at 0.75 V and 10 mA in 10 ml DMEM (fig. S27).

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Analytical characterization

LC-MS analysis: LC-MS measurements were performed on a Bruker Maxis 4G ESI-Q-TOF mass spectrometer coupled to a high-performance liquid chromatography system. Separations used a Reprospher 100 C18-Aqua column (2.0 mm by 125 mm, 5 $\mu$ m) maintained at 40°C. The mobile phase consisted of (i) H $_{2}$ O containing 0.1% formic acid and (ii) acetonitrile containing 0.1% formic acid. The gradient program was: 0 to 2 min, 10% B; 2 to 12 min, linear increase to 95% B; 12 to 18 min, 95% B; 18 to 22 min, return to 10% B. The flow rate was 0.5 ml min $^{-1}$ , and the injection volume was 1 $\mu$ l. The MS was operated in positive electrospray ionization (ESI $^{+}$ ) mode with the following settings: capillary voltage, 4500 V; nebulizer pressure, 2.0 bar; dry gas, 8 L min $^{-1}$ ; dry gas temperature, 200°C; scan range, mass/charge ratio 75 to 700. Data were processed using Bruker Compass DataAnalysis.

Nuclear magnetic resonance (NMR) spectroscopy: NMR spectra were acquired on a Varian 600 MHz spectrometer ( $^{1}$ H, 600 MHz; $^{13}$ C, 151 MHz) using a gradient-selected echo-antiecho HMBC pulse sequence. D-Glucose was electro-oxidized in an ECHO cell for 2 hours under aqueous conditions, and the reaction mixture was then redissolved in D $_{2}$ O for NMR analysis at 298 K. Spectra were collected over spectral widths of 10 ppm ( $^{1}$ H) and 220 ppm ( $^{13}$ C), using 2048 × 512 data points and 32 scans per increment. Chemical shifts were referenced to residual HDO ( $\delta$ H = 4.79 ppm). Data were processed in MestReNova (v14.2) with sine-bell apodization and zero-filling before Fourier transformation.

ICP-MS analysis: Gold ( $^{197}$ Au) and platinum ( $^{195}$ Pt) were quantified using an ICP-MS NexION 350D (PerkinElmer) operated in kinetic energy discrimination (KED) mode with helium as the collision gas. Yttrium [2 parts per billion (ppb)] was used as an internal standard. External calibration employed standards from 0.05 to 50 ppb. Limits of detection were 0.005 ppb for Au and 0.010 ppb for Pt. Serum samples (0.75 ml) were digested in concentrated HNO $_{3}$ (69%) using a DigiPREP Jr. heating block at 100°C for 55 min. Digests were diluted to 5 ml with Milli-Q water, then further diluted 20-fold in 2% HNO $_{3}$ before ICP-MS measurement.

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Animal experiments

Mouse models: This study used two mouse models: type 2 diabetic (T2D), male BKS(D)- $Lepr^{db}$ /JOrlRj mice (6 to 12 weeks old, average weight $\sim$ 35 to 45 g, purchased from Janvier Labs), male and female BKS.Cg-Dock7m+/+Lepr $^{db}$ J (db/db) (6 to 10 weeks old; Charles River Laboratories, Germany) and WT, male and female C57BL/6JRJ WT mice (6 to 12 weeks old, 18 to 28 g, purchased from Janvier Labs). Experiments were performed predominantly in male mice to reduce variability associated with sex-dependent hormonal effects. For the experiments presented in fig. S28, blood glucose profiles during electrical stimulation and glucose tolerance tests (GTTs) were evaluated in female T2D mice. The glucose-lowering effects were comparable to those observed in male T2D mice (Fig. 4, C and E), and no significant sex-dependent differences were detected. The mice were housed in controlled conditions with a stable temperature ( $21^{\circ} \pm 2^{\circ}\mathrm{C}$ ), ambient environment and controlled humidity ( $55 \pm 10\%$ ). They were maintained on a 12-hour reverse light-dark cycle and provided unrestricted access to standard chow and water. Each experimental group consisted of randomly assigned mice ( $n = 8$ ).

Animal experimentation license: All experimental procedures were conducted following ethical guidelines established by the Swiss animal welfare legislation and approved by the Veterinary Office of the Canton Basel-Stadt, Switzerland (license number: 2996\_34477 and 3341\_38467) as well as the French Republic (project no. DR2018-40v5 and APAFIS no. 16753). Experiments were conducted by licensed researchers: P.G.R (license number: LTK 5507) and G. Charpin-El Hamri (license number: 69266309) at the ETH Zurich and/or at the University of Lyon, Institut Universitaire de Technologie.

Experimental procedures: To prepare for surgical interventions, the dorsal region of the mice was shaved, and the surgical area was disinfected with mild ethanol and betadine solution. To provide preoperative analgesia, a mixture of bupivacaine (0.25%) and lidocaine (0.5%) was administered locally at the implantation site before the procedure. Meloxicam (5 mg kg $^{-1}$ , subcutaneous) was additionally administered 30 min before surgery. General anesthesia was induced using 4% isoflurane to ensure the mice were fully anesthetized and maintained using 2% isoflurane during the surgical procedures to keep the animals in a stable, unconscious state while minimizing the potential for anesthetic-related complications. The ECHO device was surgically implanted in a subcutaneous pocket and the incision was closed using clinically approved sutures (110). After surgery, the animals were stabilized for 24 hours before conducting ECHO stimulation and blood glucose profiling. The wireless-powered ECHO device was stimulated at 0.75 V and 10 mA to confirm the performance of the catalyst compared with control groups. Then, voltage (0 to 0.9 V) and current (0 to 10 mA) parameters of the implanted ECHO device were standardized for blood-glucose oxidation by continuous stimulation for 2 hours. Subsequently, the optimized voltage (0.75 V) and current (10 mA) were used to standardize the stimulation time. To enable closed-loop control, the ECHO device was wirelessly connected to a commercial CGM system (FreeStyle Libre 3) (figs. S16 and S18 and movie S1). The electronic circuit interconnecting CGM and ECHO to achieve a bioelectronic closed-loop system is shown in fig. S16. To equip animals with this bioelectronic closed-loop system, the ECHO device was implanted on the dorsal side, and this was followed by a 24-hour recovery period before the dorsoventral area of the mice was shaved and sterilized prior to placement of the CGM device. A compatible CGM reader was used for continuous data acquisition and monitoring (FreeStyle Libre 3 reader). To establish closed-loop control between the CGM and ECHO devices, we calibrated and programmed the CGM reader to vibrate at high-normal levels of 10 mM or more interstitial glucose. These vibrations were captured by a vibration sensor (SW-420 Vibration Sensor Module; BerryBase.ch) and relayed via an Arduino Controller (Arduino Nano A000005 by ATmega328; DigiKey.ch) to switch on the aforementioned power generator and activate the ECHO implant with step-sized stimulation periods of 5 min to safely lower glucose levels without the risk of hypoglycemic excursions. After each control interval, the radio frequency generator was reactivated on the basis of feedback from the vibrational sensor connected to the CGM reader's vibration unit. The wireless vibration-communication interface was established because CGM communication is proprietary and not accessible for open-source modifications.

Glucose tolerance test: Mice were fasted for 6 hours before blood glucose measurements. For the GTT, mice received an intraperitoneal injection of glucose (1.5 g/kg). The mice were then stimulated with optimized electrical parameters (0.75 V, 10 mA), and the glycemic profiles were recorded at regular intervals using ContourNext test strips and the ContourNext ONE reader (Ascensia Diabetes Care; cat. nos. 84191451 and 85659367). For long-term analyses, electrical power (0.75V, 10 mA, 60 min) was used to stimulate the ECHO device for the indicated intervals. After stimulation, blood glucose was measured, and blood samples were collected for further analysis.

Blood collection and analysis: Blood samples were collected in microtainer serum separator tubes (Becton Dickinson, cat. no. 365967), centrifuged at 6000g for 10 min at 4°C, and stored at -80°C for further analysis. Blood metabolites were profiled using triglyceride assay (Abcam, cat. no. b65336), free fatty acid quantitation (Sigma, cat. no. MAK044), and ketone body assay kits (Sigma, cat. no. MAK134). Glucagon (Mercodia, cat. no. 10-1271-01) and insulin (Mercodia, cat. no. 10-1249-01) in the blood serum were measured using the corresponding ELISA kit. In vivo biocompatibility of the ECHO device was evaluated by quantifying the inflammatory cytokines interferon- $\gamma$ (IFN- $\gamma$ ), interleukin-6 (IL-6), and tumor necrosis factor- $\alpha$ (TNF- $\alpha$ ) levels using corresponding ELISA kits [IFN- $\gamma$ (cat. no. BMS606-2), IL-6 (cat. no. BMS603HS), and TNF- $\alpha$ (cat. no. BMS607HS), all from Thermo Fisher Scientific]. In open-loop experiments, glucose was measured from tail-vein blood samples. In closed-loop studies, glucose was monitored continuously using a CGM positioned near the implant, with periodic tail-vein sampling for validation. In contrast to insulin-based regulation, ECHO modulates glucose through direct electrocatalytic oxidation at the electrode surface, governed by transport processes, including blood flow and molecular diffusion.

Resin embedding and section preparation: Samples were processed by Morphisto GmbH (Offenbach am Main, Germany) according to protocol AF-086388. Specimens were rinsed in distilled water for 1 hour to remove residual fixative and sectioned using an EXAKT diamond band saw (Model 312). Samples were dehydrated at room temperature through graded ethanol (30 to 99%), followed by isopropanol treatment and xylene clearing. Preinfiltration was performed at 4°C using a 1:1 mixture of xylene and stabilized Technovit 9100 base solution (Kulzer/Morphisto GmbH), followed by infiltration in Technovit 9100 supplemented with Hardener I and final infiltration in Technovit 9100 containing Hardener I and PMMA powder at 4°C. Samples were embedded in freshly prepared Technovit 9100, degassed (\~200 mbar, 10 min), hermetically sealed to exclude oxygen, and polymerized at $-4^{\circ}$ to $-8^{\circ}\mathrm{C}$ for 48 hours. Polymerized blocks were off-gassed overnight. Ground sections were prepared using EXAKT cutting, grinding, and thin-section technology (Donath method) with an Exakt Micro Grinder 400 CS, Diamond Band Saw 300 CP, and 402 Precision Adhesive Press. Sections were subsequently deplasticized with xylene and 2-methoxyethyl acetate, rinsed in acetone, and rehydrated.

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Histological staining and image acquisition

ECHO device sections: Rehydrated resin-embedded sections were stained with hematoxylin and eosin using an automated Leica Multistainer ST5020 system or manually with Paragon stain at $38^{\circ}$ C. Slides were dehydrated, cleared in xylene, and coverslipped with xylene-based CV Mount (Leica). After drying at $40^{\circ}$ C, slides were digitized using a ZEISS Axio Scan.Z1 slide scanner equipped with a $20\times$ objective under standardized acquisition settings.

Surrounding tissue sections: Peri-implant tissue samples embedded in paraffin blocks were sectioned using a Leica HistoCore AUTOCUT (5 $\mu$ m thick) (Leica Biosystems, Germany). Sections were stained with hematoxylin and eosin (Roth; cat. no. 9194.2) according to the manufacturers' protocols. Micrographs of the stained tissue were acquired using a Nikon Eclipse Ti2 microscope equipped with a color camera.

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Immunofluorescence analysis

Peri-implant tissue surrounding the ECHO device was harvested at the designated endpoints, fixed in 4% paraformaldehyde, paraffin-embedded, and sectioned at 5 $\mu$ m using a motorized rotary microtome (Leica HistoCore AUTOCUT, Leica Biosystems, Germany). Sections were mounted on glass slides, dried, deparaffinized in xylene, and rehydrated through graded ethanol. Heat-mediated (95°C) antigen retrieval was performed in 10 mM citrate buffer (pH 6.0) using the EZ Retriever IR antigen retrieval system (Biogenex; cat. no. MW015-IR). After cooling, sections were permeabilized with 0.1% Triton X-100 and blocked with 5% normal goat serum for 1 hour at room temperature. Sections were incubated overnight at 4°C with rabbit primary antibodies diluted in blocking buffer: anti-CD68 recombinant monoclonal antibody (clone 230504G10; Cat# 83014-5-RR; Thermo Fisher Scientific; 1:500), anti-TNF- $\alpha$ polyclonal antibody (Cat# BS-0078R; Thermo Fisher Scientific; 1:500), and anti-TGF- $\beta$ 1 recombinant monoclonal antibody (clone PD00-17; Cat# MA5-44667; Thermo Fisher Scientific; 1:500). After washing with PBS, sections were incubated for 1 hour at room temperature with Alexa Fluor 488-conjugated goat anti-rabbit IgG (H+L), cross-adsorbed secondary antibody (Cat# A-11008; Thermo Fisher Scientific; 1:250), following the manufacturer's instructions. Stained samples were imaged using a Nikon Eclipse Ti2 microscope equipped with a color camera.

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Jugular vein catheterization and hyperinsulinemic-euglycemic clamp assay

Hyperinsulinemic-euglycemic clamp assays were performed to assess device efficacy. For catheter implantation, mice received meloxicam (5 mg kg $^{-1}$ , subcutaneous) before isoflurane anesthesia. The right jugular vein was exposed and cannulated with a PE-10 catheter (C20PU-MJV2814; Instech Laboratories, Inc., Plymouth Meeting, PA, USA) filled with heparinized saline (50 U ml $^{-1}$ ). The catheter was advanced toward the right atrium, secured with silk ligatures, and tunneled subcutaneously to exit dorsally, and the incision was closed. Postoperative analgesia was maintained for 48 hours. For clamp experiments, mice were fasted for 5 to 6 hours with free access to water, and baseline blood glucose was measured from the tail vein. A priming insulin bolus (80 mU kg $^{-1}$ ) was administered through the jugular catheter, followed by a continuous glucose infusion using a precision syringe pump (Pump 11 Plus, Harvard Apparatus, Holliston, MA, USA). Blood glucose was measured every 10 min, and the glucose infusion rate (GIR) required to maintain stable glycemia was recorded. At the end of the experiment, infusions were stopped, catheters were flushed with heparinized saline, and animals were either euthanized or allowed to recover under warming conditions.

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Statistics

Unless specified otherwise, all data presented are representative of two independent experiments done in triplicate. Details of data presentation, sample sizes of biological replicates $(n)$ , statistical analyses, and significance levels are provided in the figures or their respective legends. Statistical evaluations were conducted to assess the significance of differences between datasets two-way ANOVA either with Tukey's multiple comparisons test or Dunnett's multiple comparisons test (as mentioned in figure legends). Data processing and analysis were performed using Microsoft Excel (version 16.51) and GraphPad Prism (version 9.2.0).

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ACKNOWLEDGMENTS

We thank H. Zulewski, A. P. Teixeira, and A. Hierholzer for generous advice. We thank M. Pfeffer (Department of Chemistry, University of Basel) for LC-MS analyses, I. Cornu (University of Basel) for assistance with NMR measurements, and N. Gasilova (EPFL, ISIC-GE-VS, Sion) for performing ICP-MS analyses. We thank M.-D. Hussherr (D-BSSE Animal Facility, ETH Zurich) for expertise in performing jugular vein catheterization and surgical procedures. Funding: This work was financially supported through a European Research Council advanced grant (ElectroGene, no. 785800; M.F.) and in part by the Swiss National Centre of Competence in Research (NCCR) for Molecular Systems Engineering (M.F.). Author contributions: D.M. and M.F. designed the project. D.M. and M.F. analyzed the results and wrote the manuscript. D.M. conducted the in vitro work, and P.G.R. and G.C.-E.H. performed the animal experiments. D.M. and P.B. designed ECHO and fabricated the wireless power circuit. Competing interests: The authors declare that they have no competing interests. Data, code, and materials availability: All data supporting the findings of this study are available in the paper and its supplementary materials. Original data are provided in data S1. The materials generated during this study, including the GF\_Au@Pt electrocatalyst and the ECHO implant components, are available from the corresponding author upon reasonable request. License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse. This research was funded in whole or in part by the European Research Council (785800); as required, the author will make the Author Accepted Manuscript (AAM) version available under a CC BY public copyright license.

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.ady8560

Figs. S1 to S28; Tables S1 and S2; MDAR Reproducibility Checklist; Movies S1 and S2; Data S1 Submitted 8 May 2025; resubmitted 30 May 2026; accepted 31 August 2026

10.1126/science.ady8560

BAK and BAX form a multiprotein complex to drive mtDNA efflux and caspase-independent cell death

Full article and list of author affiliations: https://doi.org/10.1126/science.aea2181

Shaoyuan Yang†, Hyungjin Kim†, Guanghong Liao, Na Ta, Ho-Chou Tu, Shriram Ramani, Chih-Yu Chen, Zih-Yu Li, Nobuhiro Tanno, James J. Hsieh, Emily H. Cheng\*

INTRODUCTION: Mitochondria have a pivotal role in mammalian cell death. In response to apoptotic signals, activator BH3-only proteins activate BAX and BAK, leading to mitochondrial outer membrane permeabilization (MOMP), cytochrome c release, apoptosome assembly, and caspase-mediated apoptosis. In cells lacking apoptosome function, activation of BAX and BAK instead leads to sustained release of mitochondrial DNA (mtDNA) into the cytosol, activation of cGAS-STING-type I interferon signaling, and caspase-independent cell death. The apoptotic caspase cascade normally suppresses this innate immune pathway, rendering apoptosis immunologically silent. Given that impaired apoptosome function is common in human cancers, BAX-BAK activation-induced mtDNA efflux and immunogenic cell death may provide a new avenue for cancer therapy. However, the molecular and biochemical basis of mtDNA efflux was not understood.

RATIONALE: BAX-BAK activation-induced mtDNA efflux has been attributed to MOMP-associated mitochondrial inner membrane (MIM) herniation. After cytochrome c efflux, BAX and BAK coalesce to form macropores in the mitochondrial outer membrane (MOM), through which the MIM herniates and subsequently loses membrane integrity, resulting in mtDNA efflux. However, only a minority of herniated MIM structures lose membrane integrity, suggesting that mtDNA efflux may also involve an active biochemical process. We therefore used biochemical and genetic studies to determine whether BAK and BAX engage distinct protein complexes that differentially regulate cytochrome c and mtDNA efflux. We further examined this process in human cancer cells with impaired apoptosome function.

RESULTS: BAK and BAX, once activated by activator BH3-only proteins, assembled into two functionally distinct mitochondrial complexes. The machinery responsible for cytochrome c release probably consisted of a BAK or BAX hexamer. By contrast, we purified a preexisting 600-kD complex comprising BAK, VDAC1, VDAC2, PHB1, and PHB2, which may localize at contact sites between the MOM and MIM. Activation by BH3-only proteins appears to remodel this complex and promote recruitment of cytosolic BAX to form mtDNA-releasing machinery, which directly released mtDNA from mitoplasts. This remodeling was associated with VDAC channel closure and increased mitochondrial calcium influx. Loss of VDAC1, VDAC2, or prohibitins impaired mtDNA efflux and caspase-independent cell death without affecting MOMP or MIM herniation. Depletion of mtDNA also protected cells from this form of death, supporting a contribution of cytosolic mtDNA to cellular demise. We designated this BAX-BAK activation-induced caspase-independent cell death “baciptosis.” Baciptosis displayed necrotic morphology, lacked widespread genomic DNA fragmentation, and was accompanied by a progressive decline in

Graphical model illustrating distinct BAK-BAX complexes mediating cytochrome c and mtDNA efflux. Activator BH3-only proteins activate BAK and BAX to form a hexameric complex that mediates cytochrome c release. In parallel, they remodel a preexisting 600-kD complex containing BAK, VDAC1, VDAC2, PHB1, and PHB2, and recruit cytosolic BAX to generate mtDNA-releasing machinery. The model highlights the mechanistic separation between cytochrome c release and mtDNA efflux.

ATP concentrations before cellular demise. These findings were recapitulated in apoptosome-deficient human kidney and lung cancer cells.

CONCLUSION: Our findings identify mtDNA-releasing machinery that is distinct from the cytochrome c-releasing MOMP machinery. Thus, mtDNA efflux is not simply a downstream consequence of MOMP or MIM herniation but instead involves a distinct, active biochemical process. mtDNA efflux contributes to bacitosis, a form of BAX-BAK activation-induced programmed necrosis that occurs when apoptosome function is impaired. This work provides a mechanistic basis for exploring BAX-BAK activation-induced bacitosis as a potential therapeutic avenue in apoptosome-deficient cancers. □

CELL BIOLOGY

BAK and BAX form a multiprotein complex to drive mtDNA efflux and caspase-independent cell death

Shaoyuan Yang $^{1\dagger}$ , Hyungjin Kim $^{2\dagger\ddagger}$ , Guanghong Liao $^{1}$ , Na Ta $^{1}$ , Ho-Chou Tu $^{1}$ , Shriram Ramani $^{1}$ , Chih-Yu Chen $^{1}$ , Zih-Yu Li $^{1}$ , Nobuhiro Tanno $^{1}$ , James J. Hsieh $^{2}$ , Emily H. Cheng $^{1,3,4*}$

The apoptotic regulators BAX and BAK, once activated, form homo-oligomers to trigger mitochondrial outer membrane permeabilization (MOMP), activating the apoptosome and caspases. Activation of BAX-BAK without apoptosome activation triggers sustained efflux of mitochondrial DNA (mtDNA) and caspase-independent cell death. However, the molecular basis of mtDNA efflux remains unclear. We purified a macromolecular complex comprising BAK, BAX, activator BH3-only molecules, voltage-dependent anion channels 1 and 2 (VDAC1 and VDAC2), and prohibitins that released mtDNA from mitoplasts. BAX-BAK activation resulted in VDAC closure, mitochondrial calcium influx, and mtDNA efflux. Loss of VDAC1, VDAC2, or prohibitins prevented BAX-BAK activation-induced mtDNA efflux and caspase-independent cell death without affecting MOMP or mitochondrial inner membrane herniation. These findings support differential regulation of cytochrome c and mtDNA efflux by distinct BAX-BAK complexes.

Mitochondria have a pivotal role in mammalian cell death. Diverse apoptotic signals trigger cytochrome c release from the mitochondrial intermembrane space, enabling apoptotic protease activating factor 1 (APAF1) to assemble the heptameric apoptosome and activate caspases $(1, 2)$ . The multidomain proapoptotic proteins BAX and BAK permeabilize the mitochondrial outer membrane (MOM), whereas antiapoptotic BCL-2, BCL-X $_{L}$ , and MCL-1 preserve mitochondrial integrity $(3–5)$ . BH3-only molecules (BH3s) integrate upstream apoptotic signals to promote apoptosis by either directly activating BAX and BAK or inactivating BCL-2, BCL-X $_{L}$ , or MCL-1 $(4–13)$ . In response to apoptotic signals, activator BH3s bind directly to BAX or BAK to induce their homooligomerization, leading to MOM permeabilization (MOMP) $(4–13)$ . BCL-2 family proteins regulate apoptosis in normal physiological and disease processes and are targets for anti-cancer drugs that disrupt protein-protein interactions $(14–16)$ .

Activation of BAX and BAK not only triggers APAF1-mediated caspase activation but also initiates caspase-independent mitochondrial dysfunction and cellular demise (4). Activation of BAX and BAK in cells lacking APAF1, caspase-9, or caspase-3 and caspase-7 leads to sustained release of mitochondrial DNA (mtDNA) into the cytosol, activating the cGAS-STING pathway and type I interferon (IFN) response (17, 18). Imaging analyses revealed that cytochrome $c$ exits from BAX or BAK pores that are too small to be resolved by super-resolution microscopy (19). After cytochrome $c$ efflux, BAX and BAK coalesce to form macropores in the MOM through which the mitochondrial inner membrane (MIM) herniates and then loses membrane integrity, resulting in efflux of mtDNA $(19)$ . Only a minority of herniated MIM loses membrane integrity and most transcription factor A, mitochondrial (TFAM)-bound mtDNA remains inside the mitochondria during this process $(19)$ . During caspase-mediated apoptosis, mtDNA efflux occurs transiently on the verge of cell death because of rapid caspase-mediated killing $(19)$ . Even if a small amount of mtDNA is released during apoptosis, cGAS-STING-type I IFN signaling is abrogated by caspase-3-mediated cleavage of cGAS and IRF3, rendering apoptosis immunologically silent $(17, 18, 20, 21)$ .

The discovery of mtDNA efflux induced by activation of BAX or BAK and subsequent activation of immunogenic cell death opens new avenues for cancer cell death research, particularly given that impaired apoptosome function is common in human cancers $(22)$ . However, the molecular and biochemical basis of mtDNA efflux is not understood. Specifically, it remains unclear whether mtDNA efflux is simply a consequence of MOMP and MOMP-associated MIM herniation or if it involves yet-to-be-identified active biochemical processes. Furthermore, it is unknown whether mtDNA release contributes to caspase-independent cell death. Given that neurons and myocardium express little APAF1 $(23, 24)$ , mtDNA efflux may contribute to the pathogenesis of diseases associated with neuronal and myocardial cell death. We used biochemical and genetic studies to identify and characterize a macromolecular complex associated with BAK and BAX, which regulated mtDNA efflux and caspase-independent cell death in various cell types, including apoptosome-deficient human cancer cells.

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Results

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Identification of a 600-kD BAK-associated macromolecular complex

To determine whether BAK engages distinct protein complexes to regulate the efflux of cytochrome c and mtDNA, $Bax^{-/-}Bak^{-/-}$ mouse embryonic fibroblasts (MEFs) were reconstituted with N-terminal protein C-tagged BAK to facilitate the affinity purification of BAK-associated complexes. We focused on BAK because it is an integral MOM protein, whereas BAX translocates from the cytosol to mitochondria upon apoptosis (8, 25). To enhance the extraction of detergent-resistant BAK and associated integral membrane proteins, mitochondria were sequentially extracted with 1% and 2% 3-[(3-cholamidopropyl)dimethylammonio]-1-propanesulfonate (CHAPS) detergent. The 1% CHAPS-insoluble, 2% CHAPS-soluble subfraction was subjected to anti-protein C affinity chromatography, followed by silver staining and tandem mass spectrometry. The voltage-dependent anion channel 1-3 (VDAC1-3) isoforms, adenine nucleotide translocator 1 (ANT1), and prohibitin 2 (PHB2) were copurified with BAK at nearly 1:1 stoichiometry (Fig. 1A and table S1). The identity of these proteins was further verified by immunoblotting (Fig. 1B). The mitochondrial matrix protein cyclophilin D, a critical regulator of the mitochondrial permeability transition pore complex (mPTP) (26), and the MIM protein ATP synthase β served as negative controls. The association of BAK with proteins localized to both the MOM (VDAC1-3) and the MIM (ANT1 and PHB2) indicates that these components may assemble into a complex at contact sites between the MOM and MIM. Indeed, fractionation of submitochondrial vesicles on a discontinuous sucrose gradient revealed overlapping localization of BAK, VDAC1, VDAC2, ANT1, and PHB2 at MOM-MIM contact sites (Fig. 1C).

To further characterize this complex, we used gel filtration chromatography of the 2% CHAPS-soluble mitochondrial subfraction. BAK, VDACs, ANT1, and PHB2 eluted in high-molecular-weight fractions around 600 kD, consistent with these proteins forming a 600-kD complex. Cyclophilin D, cytochrome c oxidase subunit IV (COX IV), and ATP synthase β were not found in these fractions, supporting the specificity of this complex (Fig. 1D). To further confirm that these proteins form a 600-kD complex, fractions of high molecular size were collected from gel filtration chromatography and subjected to immunoprecipitation with antibody to protein C. The resulting silver-stained gel showed patterns similar to those obtained without size fractionation shown in Fig. 1A (Fig. 1E), and their identity was further confirmed by immunoblotting (Fig. 1F). This 600-kD complex appears to exist in healthy cells, distinguishing it from oligomerized BAK, which is only detected upon activation by BH3s (8, 10).

A

D

c

B

G

E

F

H

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J

Fig. 1. BAK exists in three protein complexes with distinct death-regulatory activities. (A) Mitochondria from $Bax^{-/-}Bak^{-/-}$ MEFs ± protein C (PrC)-tagged BAK were sequentially extracted with 1% and 2% CHAPS. The 2% CHAPS-soluble subfraction was purified by anti-PrC affinity chromatography and silver stained. Bands were excised for tryptic digestion and liquid chromatography-tandem mass spectrometry. (B) $Bax^{-/-}Bak^{-/-}$ MEFs ± PrC-tagged BAK were subjected to anti-PrC immunoprecipitation and immunoblotting. (C) Mitochondria from WT MEFs were subjected to hypotonic swelling and sonication, fractionated on a discontinuous sucrose gradient into MOM, MIM, and contact site (CS) fractions, and analyzed by immunoblotting. FIS1 marks the MOM. (D) The 2% CHAPS-soluble mitochondrial subfraction from WT MEFs was analyzed by Superdex 200 (HR 10/30) gel filtration and immunoblotting. Protein standards indicate apparent molecular size in kilodaltons. (E and F) The 2% CHAPS-soluble mitochondrial subfraction from $Bax^{-/-}Bak^{-/-}$ MEFs ± PrC-tagged BAK was subjected to gel filtration. Fractions around 600 kD were purified by anti-PrC affinity chromatography and analyzed by silver staining (E) or immunoblotting (F). (G) Mitochondria from WT MEFs ± recombinant tBID were sequentially extracted with 1% and 2% CHAPS and analyzed by gel filtration chromatography and immunoblotting. The control anti-BAK immunoblot (2% CHAPS-soluble) is identical to that in (D). (H) The 1% CHAPS-soluble mitochondrial subfraction from $Bax^{-/-}Bak^{-/-}$ MEFs ± PrC-tagged BAK was analyzed by gel filtration. Fractions around 160 kD were purified by anti-PrC affinity chromatography and silver stained. (I and J) The 2% CHAPS-soluble mitochondrial subfraction from WT MEFs was analyzed by gel filtration. The 60-kD fraction before tBID and the 160- and 600-kD fractions after tBID were subjected to BMH cross-linking (I) or incubated with $Bax^{-/-}Bak^{-/-}$ mitochondria to assess cytochrome c release by ELISA (J). Data are shown as mean ± SD ( $n = 3$ independent experiments). \*\*\*P < 0.001 (Student's t test).

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BAK exists in three protein complexes with distinct death-regulatory activities

To investigate the existence of distinct BAK-associated complexes, gel filtration chromatography (Superdex 200 HR 10/30) was performed on 1% or 2% CHAPS-soluble subfractions obtained by sequential extraction of wild-type (WT) MEF mitochondria before or after incubation with recombinant truncated BID protein (tBID) to activate BAK in vitro. BAK eluted in three distinct complexes (Fig. 1G). In both the 1% and 2% CHAPS-soluble subfractions, BAK eluted at 60 kD before tBID treatment and shifted to 160 kD after tBID treatment (Fig. 1G). We reasoned that the 160-kD complex might represent oligomerized BAK induced by tBID to mediate cytochrome c release, whereas the 60-kD complex could contain inactive BAK. BAK eluted around 600 kD from the 2% CHAPS-soluble subfraction both before and after tBID treatment (Fig. 1G). The 600-kD complex was less abundant in the 1% CHAPS-soluble subfraction, consistent with its lower solubility in 1% CHAPS. Recombinant tBID protein predominantly eluted with the 600-kD complex (Fig. 1G).

To further assess the 160-kD BAK complex, the 160-kD gel filtration fractions were subjected to anti-protein C affinity chromatography. No distinct proteins were detected in association with BAK (Fig. 1H). Therefore, the 160-kD complex probably represents a BAK hexamer composed of six 25-kD BAK monomers. To assess the functional significance of distinct BAK complexes, protein cross-linking and cytochrome c release assays were done with the 60-, 160-, and 600-kD fractions. Only BAK present in the 160-kD fraction was cross-linked into dimers and trimers by the bismaleimidohexane (BMH) crosslinker (Fig. 1I) and released cytochrome c from $Bax^{-/-}Bak^{-/-}$ mitochondria (Fig. 1J). These data indicate that the 600-kD BAK complex is functionally distinct from the 160-kD BAK complex that promotes cytochrome c release (Fig. 1J).

We next investigated whether BAK formed the same complexes after doxycycline-induced tBID expression in $Apaf1^{-/-}$ MEFs. This system enabled analysis of tBID-induced mtDNA efflux. It also allowed us to determine whether BAX formed distinct complexes and was recruited to the 600-kD complex after tBID expression, because most BAX is absent from mitochondria in healthy cells (Fig. 1G). The 2% CHAPSSoluble mitochondrial subfraction from tBID-inducible $Apaf1^{-/-}$ MEFs before or after 6 hours of tBID induction was analyzed by gel filtration chromatography. Using a different Superdex 200 (10/300 GL) column, BAK similarly shifted from 60- to 160-kD fractions upon tBID induction and consistently eluted with VDAC1, VDAC2, ANT1, and PHB2 at an apparent size of \~600 kD regardless of tBID expression (Fig. 2A). Consistent with BAX translocation from the cytosol to mitochondria during apoptosis, mitochondrial BAX increased and shifted from primarily 40 kD to 140 kD and 600 kD after tBID expression (Fig. 2A). These findings indicate that BAX, once activated by tBID, is recruited to the 600-kD complex. BAX still formed the 140- and 600-kD complexes after tBID accumulation in BAK-deficient cells (fig. S1A), indicating that these BAX-associated complexes assemble independently of BAK. We reasoned that the 40-kD BAX complex contains inactive BAX, whereas the 140-kD BAX complex is composed of a BAX hexamer analogous to the 160-kD BAK hexameric complex, representing the MOMP machinery. tBID was also recruited to the 600-kD complex, although the elution profile of endogenously overexpressed tBID differed from that of exogenously added recombinant tBID (Figs. 2A and 1G). Coimmunoprecipitation of BAK, BAX, tBID, and PHB2 with hemagglutinin (HA)-VDAC1 was confirmed in tBID-inducible $Apaf1^{-/-}$ MEFs in which endogenous VDAC1 was replaced with HA-tagged VDAC1 (fig. S1B).

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Loss of VDAC1 or VDAC2 inhibits BAX-BAK-dependent caspase-independent cell death

To assess the function of the 600-kD BAK-BAX complex, we targeted each Vdac gene with Cas9 and single-guide RNAs (sgRNAs) in tBID-inducible $Apaf1^{-/-}$ MEFs. Targeting Vdac1 or Vdac2, but not Vdac3, protected $Apaf1^{-/-}$ cells from cell death triggered by tBID or by combined inhibition of BCL-2, BCL- $\mathrm{X_L}$ , and MCL-1 using ABT-263 (navitoclax, a dual inhibitor of BCL-2 and BCL- $\mathrm{X_L}$ ) and S63845 (an MCL-1 inhibitor) (Fig. 2B) (27, 28). Simultaneous targeting of both Vdac1 and Vdac2 conferred greater protection. These findings were further validated in tBID-inducible $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ MEFs (Fig. 2C). By contrast, targeting both Vdac1 and Vdac2 failed to prevent and even slightly increased apoptosis in WT MEFs (Fig. 2D). However, WT MEFs lacking Vdac1 and Vdac2 were protected from tBID-induced cell death when caspase activity was inhibited by the pan-caspase inhibitor Q-VD-OPh (fig. S1C). As reported previously (4), BAX-BAK activation killed $Apaf1^{-/-}$ MEFs at a much slower rate than it did WT MEFs (fig. S1D). ABT-263 plus S63845 (AS) failed to activate BAX or BAK in the absence of activator BH3s (fig. S1E), consistent with their displacement of endogenous activator BH3s to indirectly activate BAX-BAK (10, 12, 29). Moreover, retroviral transduction of tBID, BIM, or PUMA triggered cell death in $Apaf1^{-/-}$ MEFs, which was suppressed by the loss of VDAC1-VDAC2 (fig. S1F). Genetic studies indicate that VDACs are dispensable for MOMP (30), and deficiency of Vdac2 alone or of all three Vdac isoforms even accelerates caspase-dependent apoptosis (30–32).

Consistent with the viability data, loss of VDAC1-VDAC2 did not inhibit tBID-induced cytochrome c release, although it appeared to reduce baseline mitochondrial cytochrome c levels (Fig. 2E). tBID-induced oligomerization of BAX or BAK was still detected by cross-linking in $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ cells (Fig. 2F). VDAC2 not only keeps BAK in an inactive monomeric form but also stabilizes its mitochondrial localization (31–34). Accordingly, BAK became BAX-like in the absence of VDAC2: Once activated by death signals, it translocated from the cytosol to mitochondria (Fig. 2E) and formed homo-oligomers, although BAK was unstable and less abundant (Fig. 2F). Consistent with VDAC2-mediated BAK stabilization, loss of VDAC2, but not VDAC1 or VDAC3, led to reduced abundance of BAK (fig. S1G). A small molecule reportedly binds VDAC2 and enhances its inhibition of BAK-driven apoptosis (35). Collectively, VDAC2 appears to negatively regulate BAK-dependent apoptosis while promoting BAK-mediated caspase-independent cell death, likely through association with distinct BAK complexes (60 versus 600 kD).

Our findings that loss of VDAC1-VDAC2 inhibits tBID-induced death in $Apaf1^{-/-}$ cells without blocking MOMP (Fig. 2E) indicate that BAX-BAK-dependent, caspase-independent cell death is not merely a consequence of MOMP. Furthermore, MEFs survived and proliferated in the absence of cytochrome $c$ , and its deficiency did not affect tBID-induced killing of $Apaf1^{-/-}$ cells (fig. S1H). We tested specific inhibitors of other known cell death pathways in BAX-BAK activation-induced caspase-independent cell death that we call baciptosis (fig. S1I). None of these inhibitors prevented baciptosis, thereby excluding the involvement of pyroptosis (inhibited by Q-VD-OPh), necroptosis (inhibited by the protein kinase RIPK1 inhibitor necrostatin-1 and the RIPK3 inhibitor GSK'872), ferroptosis (inhibited by ferrostatin-1 and deferoxamine), and mPTP (inhibited by cyclosporin A). Conversely, CRISPR-Cas9-mediated targeting of mitochondrial DNA polymerase gamma (Polg) depleted mtDNA and protected $Apaf1^{-/-}$ cells from tBID-induced cell death (Fig. 2G). Similar protection was observed in cells treated with ethidium bromide to deplete mtDNA (fig. S1J), supporting the notion that cytosolic release of mtDNA contributes to baciptosis.

We characterized the morphological and biochemical features of bac-iptosis. Time-lapse live-cell imaging showed that WT MEFs expressing tBID exhibited classical apoptotic features, including membrane blebbing, cell shrinkage, and fragmentation (movie S1), whereas $Apaf1^{-/-}$ MEFs expressing tBID displayed prominent balloon-like swelling before cell death, consistent with necrotic morphology (movie S2). Electron microscopy revealed that tBID expression in WT MEFs produced characteristic apoptotic features, including chromatin condensation along the nuclear periphery and plasma membrane blebbing (fig. S2A). By contrast, tBID expression in $Apaf1^{-/-}$ MEFs resulted in necrotic features, including plasma membrane and organelle disruption, induction of autophagy and mitophagy, and lysosomal accumulation (fig. S2, B and C). Consistently, developmental cell death in the interdigital webs of $Apaf1^{-/-}$ mice has necrotic rather than apoptotic morphology (36). These observations support the classification of baciptosis as a distinct form of programmed necrosis. To exclude additional death modalities, we assessed lysosomal membrane permeabilization and detected no evidence of lysosomal disruption in either $Apaf1^{-/-}$ or $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ MEFs (fig. S2D). We also evaluated genomic DNA integrity by terminal deoxynucleotidyl transferase-mediated deoxyuridine triphosphate nick end labeling (TUNEL) staining. Apoptotic cells showed TUNEL staining, whereas baciptotic cells did not (fig. S2E). Baciptosis was accompanied by a progressive decline in ATP concentrations preceding cellular demise, whereas loss of VDAC1-VDAC2 preserved ATP concentrations (fig. S2F). Thus, baciptotic cell death appears to cause catastrophic bioenergetic failure downstream of mtDNA release.

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Fig. 2. Loss of VDAC1 or VDAC2 inhibits BAX-BAK-dependent caspase-independent but not caspase-dependent cell death. (A) The 2% CHAPS-soluble mitochondrial subfraction from tBID-inducible $Apaf1^{-/-}$ MEFs ± doxycycline (1 μg/ml) for 6 hours was analyzed by Superdex 200 (Increase 10/300 GL) gel filtration chromatography, followed by immunoblotting. (B) tBID-inducible $Apaf1^{-/-}$ MEFs transduced with Cas9 and the indicated sgRNAs were analyzed by immunoblotting. Cells were treated with doxycycline or ABT-263 (2 μM) plus S63845 (10 μM), and cell death was quantified by PI staining and flow cytometry at 48 hours. (C) tBID-inducible $Apaf1^{-/-}$ or $Apaf1^{-/-}$ Vdac1 $^{-/-}$ -Vdac2 $^{-/-}$ MEFs were treated as in (B), and cell death was quantified by PI staining at 48 hours. (D) tBID-inducible WT MEFs transduced with Cas9 and the indicated sgRNAs were treated as in (B), and cell death was quantified by annexin V staining at 6 hours. (E) tBID-inducible $Apaf1^{-/-}$ or $Apaf1^{-/-}$ -Vdac1 $^{-/-}$ -Vdac2 $^{-/-}$ MEFs ± doxycycline for the indicated times were subjected to subcellular fractionation and analyzed by immunoblotting. (F) tBID-inducible $Apaf1^{-/-}$ or $Apaf1^{-/-}$ -Vdac1 $^{-/-}$ -Vdac2 $^{-/-}$ MEFs ± doxycycline (6 hours) were treated with BMH and analyzed by immunoblotting. An asterisk denotes an intramolecularly cross-linked BAK monomer. (G) tBID-inducible $Apaf1^{-/-}$ MEFs transduced with Cas9 and the indicated sgRNAs were subjected to qPCR-based mtDNA quantification (left). Cell death was quantified by PI staining at 48 hours after doxycycline treatment (right). Data in (B) to (D) and (G) are shown as mean ± SD ( $n = 3$ independent experiments). \* $P < 0.05$ ; \*\*\* $P < 0.001$ ; \*\*\*\* $P < 0.0001$ ; ns, not significant (Student's t test).

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Loss of VDAC1, VDAC2, or prohibitins impairs BAX-BAK-dependent mtDNA efflux

Because mtDNA efflux contributes to baciptosis, which is inhibited by VDAC1 and VDAC2 loss, we tested whether the 600-kD BAK-BAX complex promotes mtDNA release. tBID-induced mtDNA efflux depended on BAK and BAX (Fig. 3A). As in apoptosis, BAK and BAX functioned redundantly to drive baciptosis (fig. S3A). Loss of both VDAC1 and VDAC2 reduced mtDNA efflux induced by tBID or AS in $Apaf1^{-/-}$ cells (Fig. 3, B and C). Retroviral transduction of VDAC1 or VDAC2, but not VDAC3, restored tBID-induced mtDNA efflux and baciptosis in $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ cells (Fig. 3D). Consistent with the role of VDAC2 in stabilizing BAK, reexpression of VDAC2, but not VDAC1 or VDAC3, in $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ cells restored BAK abundance (Fig. 3D). Thus, VDAC1 and VDAC2, but not VDAC3, have critical roles in BAX-BAK-dependent mtDNA efflux and baciptosis.

To determine whether loss of VDAC1-VDAC2 affects the formation of distinct BAK-BAX complexes, we performed gel filtration chromatography on the 2% CHAPS-soluble mitochondrial subfraction from $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ cells before and after tBID expression. Consistent with BAK becoming BAX-like in the absence of VDAC2, both BAK and BAX were present exclusively in small-molecular-size fractions (40 to 60 kD) before tBID expression and shifted to 140- to 160-kD and 600-kD fractions after tBID expression (Fig. 3E). Thus, loss of VDAC1-VDAC2 did not impair the formation of the MOMP machinery, as supported by gel filtration chromatography (Fig. 3E) and protein cross-linking (Fig. 2F). It also did not alter the elution profiles of tBID, ANT1, or PHB2 (Fig. 3E), indicating that deficiency of VDAC1-VDAC2 does not grossly disrupt the formation of the 600-kD BAK-BAX complex. Similarly, loss of BAX-BAK did not affect the localization of VDAC1, VDAC2, prohibitins, and tBID to the 600-kD complex (fig. S3B). These data indicate that components of the 600-kD complex may be independently targeted to contact sites between the MIM and MOM, where the specialized lipid and protein microenvironment may facilitate their assembly.

Because mtDNA efflux requires passage across both mitochondrial membranes, PHB2, ANT1, or both (MIM proteins associated with the 600-kD BAK-BAX complex) may contribute to this process. We could not generate stable Phb2-deficient cell lines due to its essentiality $(37)$ . Nonetheless, transient targeting of Phb2 significantly attenuated tBID-induced mtDNA efflux and bacitosis in $Apaf1^{-/-}$ MEFs (Fig. 3, F to H). By contrast, depletion of Phb2 did not affect tBID-induced apoptosis in WT MEFs (fig. S3C). Consistent with the interdependence of PHB1 and PHB2 within a heterodimeric MIM complex (37, 38), targeting Phb2 reduced the abundance of both PHB2 and PHB1 but slightly increased the abundance of BAK (Fig. 3F). PHB1 also eluted with the 600-kD BAK-BAX complex and coimmunoprecipitated with BAK (fig. S3, D and E). Loss of PHB1-PHB2 did not impair recruitment of BAX, BAK, VDAC1, VDAC2, or tBID to the 600-kD complex (fig. S3F). Thus, prohibitins appear to be required for mtDNA release but not complex assembly. Loss of VDAC1-VDAC2 or prohibitins significantly attenuated accumulation of IFN- $\beta$ , an indicator of mtDNA-mediated activation of the cGAS-STING-type I IFN pathway, in tBID-expressing $Apaf1^{-/-}$ MEFs (fig. S3, G and H).

Because ANT1 interacts with ANT2, which also eluted with the 600-kD complex (fig. S3D), we evaluated both isoforms. Lentiviral transduction of Cas9 and sgRNAs targeting both Ant1 and Ant2 had minimal effects on tBID-induced mtDNA efflux and baciptosis (Fig. 3, I and J). Thus, despite their presence in the 600-kD complex, ANTs and VDAC3 are not key mediators of BAX-BAK-dependent mtDNA efflux and baciptosis and may instead have structural or auxiliary roles. Although VDAC-mediated mitochondrial calcium influx could potentially activate the mPTP, depletion of cyclophilin D had little effect on tBID-induced mtDNA efflux and baciptosis (fig. S3I), arguing against mPTP involvement. Similar results were obtained with cyclosporin A treatment (fig. S1I). The roles of VDAC1, VDAC2, and PHB2 in BAX-BAK activation-induced mtDNA efflux and baciptosis were further validated in B16-F10 mouse melanoma cells (fig. S4).

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Characterization of BAX-BAK activation-induced mtDNA efflux and cell death in apoptosome-deficient human cancers

Given the multiple mechanisms of apoptosome inactivation in human cancers (22), we investigated whether baciptosis occurs under these conditions and whether it requires VDAC1, VDAC2, and prohibitins. We screened commonly used human cancer cell lines for minimal effector caspase activity after BAX-BAK activation with AS. AS effectively triggered MOMP, as evidenced by cytochrome c release, in A498 kidney cancer, PC9 lung cancer, and MDA-MB-231 breast cancer cells; however, minimal effector caspase activity was detected in A498 and PC9 cells, likely due to their low APAF1 expression (Fig. 4A and fig. S5, A to C). Consistent with caspase activation, MDA-MB-231 cells died faster than A498 and PC9 cells, and only cell death in MDA-MB-231 cells was blocked by Q-VD-OPh (Fig. 4B and fig. S5D). Depletion of both BAX and BAK protected A498 and PC9 cells from AS-induced cell death (fig. S5E). Thus, activation of BAX-BAK by AS induces baciptosis in A498 and PC9 cells.

To determine whether human BAK and BAX form the aforementioned complexes upon activation, we isolated mitochondria from A498 cells before and after AS treatment and analyzed the 2% CHAPSSoluble mitochondrial subfraction by gel filtration chromatography (Fig. 4C). Similar to mouse BAK, apparent size of human BAK shifted from 60 to 160 kD after AS treatment and eluted with VDAC1, VDAC2, PHB1, and PHB2 at \~600 kD both before and after treatment (Fig. 4C). Consistent with mouse BAX, human BAX eluted exclusively with apparent size of 40 kD before treatment and shifted to 140 and 600 kD after treatment (Fig. 4C). BIM predominantly eluted in fractions with apparent size of \~50 kD before treatment but shifted to 600 kD after AS treatment (Fig. 4C). These findings indicate that AS displaces BIM from antiapoptotic BCL-2 family members to activate BAX-BAK present within the 40- to 60-kD and 600-kD complexes, one for the formation of the MOMP machinery and the other for the mtDNA-releasing machinery, respectively.

We investigated the roles of VDACs and prohibitins in AS-induced mtDNA efflux and bacitosis in A498 and PC9 cells. Targeting $VDAC1$ or $VDAC2$ , but not $VDAC3$ , significantly attenuated both responses (Fig. 4, D and E, and fig. S5, F and G). Simultaneous depletion of VDAC1 and VDAC2 could not be assessed because these cells did not tolerate loss of both proteins. As in MEFs, loss of VDAC2, but not VDAC1 or VDAC3, reduced BAK abundance (fig. S5, F and G). Because prohibitins are essential and human cells did not tolerate CRISPR-Cas9-mediated PHB2 depletion, we transiently depleted PHB2 with lentiviral short hairpin RNAs (shRNAs). Depletion of PHB2 reduced the abundance of both PHB2 and PHB1 and significantly attenuated AS-induced mtDNA efflux (Fig. 4, F and G, and fig. S5, F and G). However, we were unable to assess the effect of PHB1-PHB2 loss on bacitosis, because cells deficient in both proteins died before the onset of AS-induced bacitosis. By contrast, loss of VDAC1 or VDAC2 failed to inhibit AS-induced apoptosis in MDA-MB-231 cells or in APAF1-reconstituted A498 cells (Fig. 4, H and I, and fig. S5, H to J). Loss of VDAC1, VDAC2, or prohibitins also attenuated AS-induced IFN- $\beta$ expression in A498 and PC9 cells (fig. S5, K and L), consistent with their participation in BAX-BAK-dependent mtDNA efflux. Thus, human cancer cells recapitulated the mouse phenotypes, confirming that apoptosome-deficient cancers can undergo bacitosis after BAX-BAK activation, a process regulated by VDAC1 and VDAC2.

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Fig. 3. Loss of VDAC1, VDAC2, or prohibitins impairs BAX-BAK-dependent mtDNA efflux and caspase-independent cell death. (A) tBID-inducible $Apaf1^{-/-}$ MEFs transduced with Cas9 and the indicated sgRNAs ± doxycycline or AS were subjected to cell death quantification at 48 hours and immunoblotting at 6 hours. Cytosolic mtDNA was assessed by qPCR at 6 hours after doxycycline treatment and 4 hours after AS treatment. (B and C) tBID-inducible $Apaf1^{-/-}$ or $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ MEFs were untreated or treated with doxycycline (B) or AS (C). Cytosolic mtDNA was assessed by qPCR at 6 and 4 hours, respectively. (D) tBID-inducible $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ MEFs transduced with control retrovirus or retroviruses expressing VDAC1, VDAC2, or VDAC3 ± doxycycline (6 hours) were analyzed by immunoblotting. Cell death was quantified at 48 hours, and cytosolic mtDNA was assessed at 6 hours. (E) The 2% CHAPS-soluble mitochondrial subfraction from tBID-inducible $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ MEFs ± doxycycline (6 hours) was analyzed by Superdex 200 (Increase 10/300 GL) gel filtration chromatography, followed by immunoblotting. (F to J) tBID-inducible $Apaf1^{-/-}$ MEFs transduced with Cas9 and the indicated sgRNAs ± doxycycline or AS were subjected to cell death quantification at 48 hours and immunoblotting at 6 hours [(F) and (I)]. Cytosolic mtDNA was assessed by qPCR at 6 hours (G and J) or 4 hours (H). Data in (A) to (D) and (F) to (J) are shown as mean ± SD ( $n = 3$ or 4 independent experiments). \*P < 0.05; \*\*P < 0.01; \*\*\*P < 0.001; \*\*\*\*P < 0.0001; ns, not significant (Student's t test).

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Fig. 4. Loss of VDAC1, VDAC2, or prohibitins impairs BAX-BAK activation-induced mtDNA efflux and cell death in apoptosome-deficient human cancer cells.

(A) Caspase activity was quantified using the Caspase-Glo 3/7 assay in the indicated cells ± AS at the indicated times. (B) The indicated cells ± AS and ± Q-VD-OPh (QVD) were analyzed for cell death by flow cytometry after annexin V and PI staining at the indicated times. (C) The 2% CHAPS-soluble mitochondrial subfraction from A498 cells ± AS for 6 hours was analyzed by Superdex 200 (Increase 10/300 GL) gel filtration chromatography, followed by immunoblotting. (D and E) The indicated A498 (D) or PC9 (E) cells ± AS were analyzed for cytosolic mtDNA by qPCR after 12 or 6 hours, respectively, and for cell death by flow cytometry after 3 or 5 days, respectively. (F and G) A498 (F) or PC9 (G) cells transduced with the indicated shRNAs ± AS were analyzed for cytosolic mtDNA by qPCR after 3 hours. (H) The indicated MDA-MB-231 cells ± AS were analyzed for cell death by flow cytometry after 24 hours. (I) A498 cells reconstituted with APAF1 and transduced with the indicated sgRNAs ± AS were analyzed for cell death by flow cytometry after 24 hours. Data in (A) and (B) and (D) to (I) are shown as mean ± SD (n = 3 or 4 independent experiments). \*P < 0.05; \*\*P < 0.01; \*\*\*P < 0.001; \*\*\*\*P < 0.0001; ns, not significant (Student's t test).

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VDAC1- and VDAC2-mediated mtDNA efflux is impaired by calcium-regulatory mutations

Mitochondrial exchange of adenosine triphosphate (ATP) and adenosine diphosphate (ADP) is mediated by the coordinated actions of VDAC and ANT, which exchange matrix ATP for cytosolic ADP during oxidative phosphorylation $(39)$ . Because the 600-kD BAK-associated complex includes both VDACs and ANT, we tested whether tBID recruitment might inhibit this exchange. We engineered a BH3-inducible system in which a floxed green fluorescent protein (GFP) cassette positioned upstream of BH3s prevented their expression from the long terminal repeat (LTR) promoter. 4-Hydroxytamoxifen (4-OHT) activated CreERT2 to excise the GFP cassette and induce BH3 expression, leading to cell death in $Apaf1^{-/-}$ MEFs (fig. S6, A to C). 4-OHT treatment reduced mitochondrial ADP import in tBID-induced but not control cells (fig. S6D). To determine whether this impairment was due to defects in VDAC or ANT, we measured ADP uptake in mitoplasts that retain ANT but lack VDAC. ADP uptake was fully restored in mitoplasts despite tBID expression (fig. S6D), indicating that tBID inhibits VDAC- but not ANT-mediated ADP import. BIM or PUMA overexpression similarly impaired mitochondrial ADP import (fig. S6E). Because VDAC1-VDAC2 loss inhibits rather than promotes baciptosis, activator BH3-induced closure of the VDAC nucleotide channel is unlikely to be a direct cause of baciptosis. Instead, VDAC closure may reflect conformational remodeling required to enable mtDNA efflux.

VDAC becomes highly permeable to calcium when closed to metabolite transport, thereby promoting mitochondrial calcium influx (40). E73 and E203 of VDAC1 are implicated in calcium regulation (41–44). E73 also regulates VDAC1 conformation, lipid interactions, and hexokinase-I-induced channel closure (42, 44). E73 is conserved in VDAC2 (E85) but not VDAC3 (Q73) (fig. S6F), which may explain why VDAC3 does not contribute to BAX-BAK-dependent mtDNA efflux and bacitosis (Figs. 2B and 3D). We tested whether BAX-BAK activation-induced closure of VDAC1 and VDAC2 could increase mitochondrial calcium influx. Using a mitochondria-targeted fluorescent protein-based calcium indicator, mito-G-GECO1.2 (45), we found that tBID expression increased mitochondrial calcium influx, which was abrogated in $Bax^{-/-}Bak^{-/-}$ cells (Fig. 5A and fig. S7A). Loss of VDAC1 and VDAC2 reduced tBID-induced mitochondrial calcium influx (Fig. 5B and fig. S7B). Similarly, AS increased mitochondrial calcium influx in a manner dependent on VDAC1 and VDAC2 (Fig. 5C and fig. S7C).

To determine whether residues in VDAC1 and VDAC2 implicated in calcium regulation might contribute to tBID-induced mitochondrial calcium influx, we reconstituted $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ cells with

WT or calcium-regulatory mutants of VDAC1 (E73Q/E203Q) and VDAC2 (E85Q/D215N). These mutations partially impaired the ability of VDAC1 and VDAC2 to restore BAX-BAK activation-induced mitochondrial calcium influx (Fig. 5D and fig. S7D). Reconstitution of WT but not mutant VDAC1 and VDAC2 rescued tBID-induced mtDNA efflux and baciptosis in $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ cells (Fig. 5E). The mutants fully restored BAK stability, mitochondrial localization, and baseline cytochrome $c$ levels to those seen with WT VDAC1 and VDAC2 yet failed to promote mtDNA efflux or baciptosis (Fig. 5F). Consistent with the loss-of-function findings (fig. S1G), WT or mutant VDAC2 but not VDAC1 restored BAK abundance in $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ cells (fig. S7E). Mutants of VDAC1 and VDAC2 remained associated with the 600-kD BAK-BAX complex and did not alter the formation of other BAK-BAX complexes (Fig. 5G). We further extended our analysis to mtDNA efflux triggered by hydrogen peroxide or ionomycin, which increase concentrations of mitochondrial calcium (46, 47). Loss of VDAC1-VDAC2, BAX-BAK, or prohibitins attenuated mtDNA efflux induced by these stimuli, although cell death still occurred under these conditions (fig. S8). These findings further support potential roles for VDAC1-VDAC2, BAX-BAK, and prohibitins in mtDNA efflux beyond canonical activation of BAX and BAK by tBID or BH3 mimetics.

VDAC1 or VDAC3 oligomers are reported to mediate mtDNA release from mitochondria under oxidative stress in nondying MEFs, a process independent of BAX and BAK (48). The N-terminal lysine residues of VDAC1 mediate its interaction with mtDNA, which is required for VDAC1 oligomerization and subsequent mtDNA release (48). We therefore compared N-terminal lysine and calcium-regulatory mutations in VDAC1 for their effects on BAX-BAK activation-induced mtDNA efflux. Retroviral transduction of both WT and the N-terminal lysine mutant (K12A/R15A/K20A) of VDAC1 restored tBID-induced mtDNA efflux and bacitosis in $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ cells (Fig. 5H). By contrast, the E73Q/E203Q mutant of VDAC1 failed to rescue these phenotypes (Fig. 5H). We propose that activation of BAX-BAK by activator BH3 proteins is associated with conformational remodeling of VDAC1 and VDAC2 that reduces nucleotide transport, increases mitochondrial calcium influx, and enables the cytosolic release of mtDNA.

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The 600-kD BAK complex containing tBID can permeabilize mitoplasts to induce mtDNA efflux

To determine whether the 600-kD BAK complex containing tBID can directly permeabilize the MIM, we incubated mitoplasts from $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}Bax^{-/-}Bak^{-/-}$ cells with the 60-kD (pre-tBID expression), 160-kD (post-tBID expression), and 600-kD (pre- or post-tBID expression) fractions collected from gel filtration chromatography of $Apaf1^{-/-}$ cells. The post-tBID 600-kD complex exhibited the highest mtDNA-releasing activity, whereas the pre-tBID 600-kD complex showed only minimal activity (Fig. 6A). By contrast, the 600-kD complex derived from tBID-expressing $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ cells failed to permeabilize the MIM for mtDNA release (Fig. 6A), underscoring a critical role for VDAC1 and VDAC2. Furthermore, the 600-kD complex obtained from tBID-expressing $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ cells reconstituted with VDAC1 and VDAC2 mutants ( $Apaf1^{-/-}Vdac1^{\mathrm{MT}}$ $Vdac2^{\mathrm{MT}}$ ) exhibited minimal mtDNA-releasing activity (Fig. 6A). These in vitro assays complement our cell-based findings and support the 600-kD complex comprising BAK, BAX, tBID, VDAC1, VDAC2, and prohibitins as the mtDNA-releasing machinery.

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Loss of VDAC1 and VDAC2 does not prevent BAX-BAK activation-induced MIM herniation

Given that MIM herniation through BAX-BAK macropores is proposed to mediate mtDNA release (19), we investigated whether loss of VDAC1 and VDAC2 impaired this process. Because MIM herniation is expected to reduce MOM-MIM colocalization, translocase of outer mitochondrial membrane 20 (TOMM20)-GFP and translocase of inner mitochondrial membrane 50 (TIMM50)-mCherry were transduced into

Apaf1 $^{-/-}$ -Vdac1 $^{-/-}$ -Vdac2 $^{-/-}$

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Fig. 5. Calcium-regulatory mutations impair VDAC1- and VDAC2-dependent mitochondrial calcium influx and mtDNA efflux during BAX-BAK activation. (A and B) The indicated tBID-inducible $Apaf1^{-/-}$ MEFs expressing mito-G-GECO1.2 ± doxycycline (4 hours) were analyzed by confocal fluorescence microscopy. Two independent clones were analyzed in (B). Fluorescence intensity was quantified using ImageJ; each dot represents one cell. (C) The indicated $Apaf1^{-/-}$ MEFs expressing mito-G-GECO1.2 ± AS (4 hours) were analyzed as in (A). Two independent clones were analyzed. (D) tBID-inducible $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ MEFs expressing WT VDAC1/2 (VDAC1/2 $^{\mathrm{WT}}$ ) or calcium-regulatory VDAC1/2 mutants (VDAC1/2 $^{\mathrm{MT}}$ ) together with mito-G-GECO1.2 ± doxycycline (4 hours) were analyzed as in (A). (E) tBID-inducible $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ MEFs expressing VDAC1/2 $^{\mathrm{WT}}$ or VDAC1/2 $^{\mathrm{MT}}$ ± doxycycline were analyzed for cell death at 48 hours and for cytosolic mtDNA and protein expression at 6 hours. (F) The indicated cells ± doxycycline for the indicated times were subjected to subcellular fractionation and immunoblotting. (G) The 2% CHAPS-soluble mitochondrial subfraction from tBID-inducible $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ MEFs expressing VDAC1/2 $^{\mathrm{MT}}$ ± doxycycline (6 hours) was analyzed by Superdex 200 (Increase 10/300 GL) gel filtration chromatography and immunoblotting. (H) The indicated cells expressing VDAC1 $^{\mathrm{WT}}$ or the indicated VDAC1 mutants ± doxycycline were analyzed for cell death at 48 hours and for cytosolic mtDNA and protein expression at 6 hours. Statistical significance in [(A) to (D)] was assessed using Student's t test to determine whether the mean fluorescence intensity of one sample exceeded 150% of that of the other ( $n = 3$ independent experiments). Data in (E) and (H) are shown as mean ± SD ( $n = 3$ independent experiments). \*\* $P < 0.01$ ; \*\*\* $P < 0.001$ ; \*\*\*\* $P < 0.0001$ ; ns, not significant (Student's t test).

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Fig. 6. The 600-kD BAK complex containing tBID can permeabilize mitoplasts deficient for BAX, BAK, VDAC1, and VDAC2 to induce mtDNA efflux. (A) Mitochondria from tBID-inducible $Apaf1^{-/-}$ , $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ , and $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ MEFs expressing calcium-regulatory VDAC1/2 mutants ( $Apaf1^{-/-}Vdac1^{MT}Vdac2^{MT}$ ) ± doxycycline (6 hours) were analyzed by Superdex 200 (Increase 10/300 GL) gel filtration chromatography as in Fig. 2A. Fractions at the indicated molecular sizes were incubated with mitoplasts from $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}Bax^{-/-}Bak^{-/-}$ MEFs, and mtDNA release was assessed by qPCR. Data are shown as mean ± SD ( $n = 3$ independent experiments). (B) tBID-inducible $Apaf1^{-/-}$ and $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ MEFs expressing TOMM20-GFP and TIMM50-mCherry ± doxycycline (2.5 hours) were analyzed by immunofluorescence using anti-TOMM20 and anti-mCherry antibodies (see also fig. S9A). Data are presented as Manders' colocalization coefficients between TOMM20-GFP and TIMM50-mCherry ( $n = 22$ , 38, 24, and 33 for $Apaf1^{-/-}$ control, $Apaf1^{-/-}$ tBID, $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ control, and $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ tBID, respectively). (C and D) Representative transmission electron microscopy images of the indicated cells treated with doxycycline for 3.5 hours (C). Red arrowheads indicate MIM herniation; insets show enlarged views. Scale bars, 1 μm. MIM herniation was quantified in the indicated cells ± doxycycline (D). Each dot represents the percentage of mitochondria with inner membrane herniation per cell. Data are shown as mean ± SD ( $n = 15$ , 15, 14, and 18 for $Apaf1^{-/-}$ control, $Apaf1^{-/-}$ tBID, $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ control, and $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ tBID, respectively). (E) Schematic model of caspase-dependent and caspase-independent cell death regulated by BAK and BAX. \* $P < 0.05$ ; \*\* $P < 0.01$ ; \*\*\*\* $P < 0.0001$ ; ns, not significant (Student's t test).

tBID-inducible $Apaf1^{-/-}$ and $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ cells to visualize the MOM and MIM, respectively. tBID expression caused comparable reductions in MOM-MIM colocalization in both $Apaf1^{-/-}$ and $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ cells (Fig. 6B and fig. S9A), indicating that VDAC1 and VDAC2 loss does not impair tBID-induced MIM herniation. Electron microscopy confirmed comparable MIM herniation in both cell types (Fig. 6, C and D). Prohibitin disruption likewise did not prevent the tBID-induced reduction in MOM-MIM colocalization (fig. S9B), indicating that prohibitins are also dispensable for tBID-induced MIM herniation.

Collectively, we interpret our data to indicate that MIM herniation may be a consequence of BAX-BAK macropore formation in the MOM rather than an active mechanism driving mtDNA efflux. Consistent with this notion, only a minority of herniated MIM exhibits loss of membrane integrity (19). MIM herniation likely persists without VDAC1 and VDAC2 because their loss does not prevent BAX-BAK oligomerization and MOMP (Figs. 2, E and F, and 3E). This persistence may explain why loss of VDAC1-VDAC2 neither completely blocks mtDNA efflux nor promotes the long-term clonogenic survival of $Apaf1^{-/-}$ cells after BAX-BAK activation (Fig. 3, B and C, and fig. S9, C and D). Altogether, our data indicate that the 600-kD BAK-BAX complex containing tBID, VDAC1, VDAC2, and prohibitins constitutes the primary machinery responsible for most mtDNA release, whereas MIM herniation contributes to secondary mtDNA leakage after BAX-BAK activation.

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Discussion

We have presented biochemical evidence that BAK and BAX, once activated by activator BH3-only proteins, assemble into two distinct mitochondrial protein complexes that independently mediate cytochrome c and mtDNA efflux (Fig. 6E). The cytochrome c-releasing MOMP machinery probably consists of a BAK or BAX hexamer, consistent with reported in vitro studies $(49, 50)$ . Our identification of these hexamers as the cytochrome c-releasing machinery may explain why these pores are too small to be visualized by super-resolution microscopy $(19)$ . By contrast, the mtDNA-releasing machinery comprises BAK, BAX, activator BH3s, VDAC1 and VDAC2 (MOM proteins), and prohibitins (MIM proteins) and may localize at contact sites between the MOM and MIM. Thus, mtDNA efflux is not simply a downstream consequence of MOMP but instead involves a distinct, active biochemical process. Conversely, MIM herniation through BAX or BAK macropores after cytochrome c release appears to be a consequence of MOMP and occurs independently of VDAC1 and VDAC2.

Although BAX-BAK-dependent mtDNA efflux occurs during caspase-mediated apoptosis, its delayed onset makes it unlikely to contribute to rapid caspase-driven death. By contrast, mtDNA efflux contributes to caspase-independent BAX-BAK-mediated death, because its disruption, through knockout of Vdac1, Vdac2, or Phb2 or through mtDNA depletion in $Apaf1^{-/-}$ cells, suppresses this form of cell death. These findings were recapitulated in human cancer cells. Low APAF1 expression impaired effector caspase activation, whereas APAF1 restoration above a critical threshold reestablished it. Apoptosome-deficient human cancers can undergo bacitosis after BAX-BAK activation, a process regulated by VDAC1 and VDAC2. These findings suggest that therapy-induced activation of BAX-BAK may have a greater impact on tumor-immune interactions in apoptosome-deficient cancers than in apoptosome-proficient cancers (16).

Because cells undergoing baciptosis lack the defining ultrastructural features of apoptosis (fig. S2B), a new term is warranted to describe this distinct form of programmed cell death. Although previously described as MOMP-induced caspase-independent cell death $(51)$ , our findings identify a BAK-BAX complex that is mechanistically separable from MOMP. We designate this necrotic form of programmed cell death as baciptosis to distinguish it from other forms of caspase-independent cell death such as ferroptosis and necroptosis. Depletion of Cgas, Ifi16, or Zbp1 did not inhibit baciptosis (fig. S10, A and B), and MEFs expressed minimal Aim2, Nlrp3, and Tlr9. Thus, baciptosis appears not to be mediated by canonical cytosolic DNA-sensing pathways. The precise mechanism by which cytosolic mtDNA promotes cell death remains to be defined.

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Materials and methods Cell lines

All MEFs were SV40 transformed and cultured as previously reported $(4)$ . Tetracycline-inducible tBID-expressing $Apaf1^{-/-}$ MEFs were generated by lentiviral transduction and single-cell subcloning, and tBID was induced with doxycycline (1 $\mu$ g/ml; Sigma). BH3-inducible $Apaf1^{-/-}$ MEFs were generated by retroviral transduction with MSCV-CreERT2-Neo and MSCV-LoxP-GFP-LoxP-BH3-pPGK-Puro, followed by single-cell subcloning. BH3 expression after treatment with 4-OHT (500 nM; Sigma) was confirmed by immunoblotting. To generate $\rho^{0}$ cells, $Apaf1^{-/-}$ MEFs were cultured with 200 ng/ml ethidium bromide (Thermo Fisher Scientific) for three passages. Knockout cell lines were generated by CRISPR-Cas9-mediated genome editing as described $(52, 53)$ . Briefly, cells were transduced with lentiviruses expressing Cas9 and sgRNAs targeting genes of interest, followed by single-cell subcloning. Knockout clones were identified by immunoblotting for loss of the target protein. Vdac1 and Vdac2 were deleted in $Apaf1^{-/-}$ MEFs to generate $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ cells. Reconstitution of WT or mutant Vdac in $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ cells was performed by retroviral transduction.

B16-F10 cells (RRID: CVCL\_0159) were obtained from the American Type Culture Collection (ATCC) and cultured as recommended by the manufacturer. MDA-MB-231 (RRID: CVCL\_0062) and A498 (RRID: CVCL\_1056) cells were obtained from the National Cancer Institute Developmental Therapeutics Program and cultured in RPMI 1640 supplemented with 10% fetal bovine serum, 1% penicillin/streptomycin, 1% nonessential amino acids, 1% sodium pyruvate, 1% L-glutamine, and 1% HEPES (Thermo Fisher Scientific). PC9 cells (human lung adenocarcinoma, male origin; RRID: CVCL\_B260) were obtained from D. Scheinberg at Memorial Sloan Kettering Cancer Center (MSKCC) and cultured as described previously $(54)$ . All cell lines were routinely tested for mycoplasma using the Venor GeM mycoplasma detection kit (Sigma).

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Plasmid construction, CRISPR-Cas9-mediated genome editing, and RNA interference

The lentiviral tetracycline-inducible hygromycin-resistance vector TRE-gene of interest-pPGK-Hygro-T2A-rtTA3 was assembled from pCW-Cas9, LentiCRISPRv2, and MSCV-Hygro (Addgene) using the NEBuilder HiFi DNA Assembly Cloning Kit (New England Biolabs). Mouse Bid lacking the N-terminal 177 base pairs of the coding region (tBID) was cloned into this vector. sgRNAs designed using Optimized CRISPR Design were cloned into LentiGuide-Puro or LentiCRISPRv2 (Addgene) (55). Mouse Vdac1, Vdac2, and Vdac3 were cloned into MSCV-Hygro (Clontech) or MSCV-IRES-GFP (4), and Vdac mutants were generated by polymerase chain reaction (PCR)-based site-directed mutagenesis. mito-G-GECO1.2 was generated by fusing the mitochondrial targeting signal from CMV-mito-R-GECO1 to G-GECO1.2 from CMV-G-GECO1.2 (Addgene) (45) and cloning the fusion into pBABE-Puro (Addgene). Mouse Apaf1 was cloned into MSCV-IRES-GFP (4). All constructs were sequence verified. Lentivirus was produced by cotransfecting 293T cells with pCMV-dR8.2 and pHCMV-VSV-G using Lipofectamine 2000 (Thermo Fisher Scientific) as described previously (52). The sgRNA sequences are listed in table S2. Lentiviral shRNA targeting human PHB2 was obtained from Sigma (TRCN0000060921), and lentiviral shRNA targeting GFP was described previously (56).

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Cell viability and caspase activity assays

Cells were plated in 12-well plates at $8 \times 10^{4}$ or $1 \times 10^{5}$ cells per well and treated with the indicated agents the next day. Cells were treated with doxycycline (1 $\mu$ g/ml; Sigma) to induce tBID expression or with ABT-263 (2 $\mu$ M; Selleck Chemicals) plus S63845 (5 or 10 $\mu$ M; Chemietek) to induce cell death. Where indicated, cells were treated with Q-VDOPh (20 $\mu$ M; MedKoo Biosciences), necrostatin-1 (5 $\mu$ M; Sigma), GSK'872 (10 $\mu$ M; Sigma), ferrostatin-1 (20 $\mu$ M; Selleck Chemicals), deferoxamine (50 $\mu$ M; Selleck Chemicals), or cyclosporin A (2 $\mu$ M; Selleck Chemicals). Cell death was quantified by annexin V (BioVision or Abcam) and/or propidium iodide (PI, 2 $\mu$ g/ml; Sigma) staining as described previously (56), followed by flow cytometric analyses using an LSRFortessa and FACSDiva software (BD Biosciences). For IncuCyte assays, cells were seeded in 96-well plates at 8000 cells per well, treated the next day, stained with SYTOX Green (100 nM; Thermo Fisher Scientific), and monitored for up to 7 days using an IncuCyte S3 Live-Cell Analysis Instrument (Sartorius). Images were acquired every 2 to 6 hours. Cell death was quantified as SYTOX Green-positive confluence normalized to total confluence in phase-contrast images using IncuCyte Basic Analysis Software. For caspase activity assays, cells were plated in 96-well plates, treated the next day, and analyzed using the Caspase-Glo 3/7 Assay System (Promega) according to the manufacturer's instructions.

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Subcellular fractionation, antibodies, and immunoblot analyses

Cells were harvested at the indicated times after tBID induction and incubated for 5 min on ice in digitonin permeabilization buffer containing 0.025% digitonin, 10 mM KCl, 5 mM MgCl $_{2}$ , 1 mM EDTA, 1 mM

EGTA, 250 mM sucrose, and 20 mM HEPES (pH 7.2) supplemented with complete protease inhibitor cocktail (Roche). Organelles containing mitochondria were separated from the cytosolic fraction by centrifugation at 15,000g and lysed in phosphate-buffered saline (PBS) containing 1% Triton X-100 and protease inhibitors. Cytosolic, mitochondrial, and whole-cell lysates were resolved by NuPAGE (Thermo Fisher Scientific) or SDS-polyacrylamide gel electrophoresis (SDS-PAGE) (Bio-Rad), transferred to polyvinylidene difluoride (PVDF) membranes (Immobilon-P; Millipore), detected by enhanced chemiluminescence (Western Lightning Plus-ECL; PerkinElmer), and imaged using an LAS-3000 system (Fujifilm) or Amersham Imager 680 (GE Healthcare). Primary antibodies used for immunoblotting were anti-BID (Cell Signaling Technology (CST), #2003, RRID:AB\_10694562), anti-BIM (Covance) (52), anti-PUMA (CST, #98672, RRID:AB\_3096180), anti-BAX (Santa Cruz Biotechnology, #sc-493, RRID:AB\_2227995; CST, #2772, RRID:AB\_10695870; Proteintech, #60267-1-Ig, RRID:AB\_2848213), anti-BAK (Upstate, #06-536, RRID:AB\_310159; CST, #12105, RRID:AB\_2716685), anti-VDAC1 (Calbiochem, Porin 31HL, RRID:AB\_565262; Abcam, #ab186321 (RRID:AB\_3739918) or #ab16814), anti-VDAC2 (Covance rabbit polyclonal antibody against the amino acid 212 to 228 peptide (31); CST, #9412, RRID:AB\_10828727), anti-VDAC3 (31), anti-ANT1 (MitoSciences, #MSA02, RRID:AB\_478281; Abcam, #ab110322, RRID:AB\_10862212), anti-ANT2 (CST, #14671, RRID:AB\_2798562), anti-PHB1(CST, #2426, RRID:AB\_823689), anti-PHB2 (Upstate, #07-234), anti-Cyclophilin D (Affinity BioReagents, #PA1-028, RRID:AB\_2169135), anti-ATP synthase β (BD Biosciences, #612518, RRID:AB\_399819), anti-COX IV (CST, #4844, RRID:AB\_2085427), anti-TOMM20 (CST, #42406, RRID:AB\_2687663), anti-PolG (Abcam, #ab128899, RRID:AB\_11145308), anti-cytochrome c (Pharmingen, #556433, RRID:AB\_396417), anti-LDHA (CST, #3558, RRID:AB\_2135109), anti-APAF1 (CST, #8723, RRID:AB\_10829610; Chemicon, #06-957), anti-Procaspase-9 (CST, #9502, RRID:AB\_2068621), anti-Procaspase-3 (BD bioscience, #611048), anti-FIS1 (Axxora, #ALX-210-907), anti-cGAS (CST, #31659, RRID:AB\_2799008), anti-ZBP1 (Santa Cruz Biotechnology, #sc-271483, RRID:AB\_10650130), anti-IFI204 (Abcam, #ab307201, RRID:AB\_3166180), anti-β-Actin (Sigma, #A1978, RRID:AB\_476692), and anti-tubulin (Sigma, #T9026, RRID:AB\_477593).

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Identification of mitochondrial BAK-associated complexes

Mitochondria were isolated from $Bax^{-/-}Bak^{-/-}$ MEFs or $Bax^{-/-}Bak^{-/-}$ MEFs reconstituted with N-terminal protein C-tagged BAK as described previously (4, 7, 8). Mitochondria were sequentially extracted with 1% and 2% CHAPS lysis buffers containing 1% or 2% CHAPS, 142.5 mM KCl, 2 mM CaCl₂, 20 mM Tris-Cl (pH 7.4), and EDTA-free protease inhibitor cocktail (Roche), followed by sonication. Lysates were applied to an anti-protein C affinity matrix (Roche), and bound complexes were eluted with 10 mM EDTA, precipitated with trichloroacetic acid, resolved on 4 to 12% NuPAGE gels (Thermo Fisher Scientific), and silver stained (Silver Staining Plus Kit; Bio-Rad). Gel slices of interest were excised, digested with trypsin, and analyzed by liquid chromatography-tandem mass spectrometry at the Taplin Mass Spectrometry Facility (Harvard Medical School, Boston, MA).

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Mitochondrial subfractionation

Isolation of MOMs, MIMs, and contact sites was adapted from a published method with minor modifications $(57)$ . All steps were performed at $4^{\circ}C$ or on ice. Mitochondria were isolated in MB buffer (200 mM sucrose, 1 mM EGTA, and 10 mM HEPES, pH 7.5), washed in EB buffer (125 mM KCl, 4 mM MgCl $_{2}$ , 5 mM KH $_{2}$ PO $_{4}$ , and 10 mM HEPES, pH 7.5), and pelleted at 10,000g for 10 min. Pellets were resuspended in swelling buffer (20 mM HEPES, 0.5 mM EDTA, pH 7.5) for 30 min, passed five times through a 30-gauge needle, and incubated with an equal volume of shrinking buffer (0.90 M sucrose, 20 mM HEPES, 0.5 mM EDTA, pH 7.5) for 15 min. Samples were sonicated to generate vesicles and centrifuged at 10,000g for 10 min. Supernatants were layered onto a discontinuous sucrose gradient (1.6, 1.35, 1.1, and 0.85 M) and centrifuged at 35,000 rpm for 14 hours in an Optima MAX-XP ultracentrifuge (Beckman Coulter). Fractions corresponding to \~1.0 M sucrose (MOM), 1.2 M (contact sites), and 1.36 M (MIM) were collected, lysed in 2% CHAPS buffer (142.5 mM KCl, 2 mM CaCl₂, and 20 mM Tris, pH 7.5), precipitated with trichloroacetic acid, and analyzed by immunoblotting.

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Gel filtration chromatography, immunoprecipitation, and protein cross-linking

Gel filtration chromatography was performed on a Superdex 200 HR 10/30 column (GE-Amersham) using an ÄKTA purifier system (Cytiva) or a Superdex 200 Increase 10/300 GL column (Cytiva) using an ÄKTA basic 10 FPLC system (GE-Amersham), as described previously (8). Columns were equilibrated in buffer containing 1% or 2% CHAPS, 300 mM NaCl, 0.2 mM dithiothreitol, and 20 mM HEPES (pH 7.5). Molecular weight standards used for calibration were thyroglobulin (669 kD), ferritin (440 kD), catalase (232 kD), aldolase (158 kD), conalbumin (75 kD), bovine serum albumin (BSA, 66 kD), ovalbumin (44 kD), and cytochrome c (14 kD). Mitochondrial lysates were loaded onto the column and eluted at 0.3 ml/min. Fractions (0.6 ml) were collected, precipitated with trichloroacetic acid, resolved by 8 to 16% SDS-PAGE or 4 to 12% NuPAGE, and analyzed by immunoblotting. For immunoprecipitation of N-terminal protein C-tagged BAK, the indicated fractions were pooled and incubated with anti-protein C matrix (Roche) in the presence of 2 mM Ca $^{2+}$ and EDTA-free protease inhibitors. Immunoprecipitates were resolved by 4 to 12% NuPAGE and analyzed by silver staining and immunoblotting. For anti-HA immunoprecipitation, lysates prepared in 2% CHAPS buffer (142.5 mM KCl, 2 mM CaCl $_{2}$ , and 20 mM Tris-Cl, pH 7.4) were incubated with anti-HA antibody (12CA5) and captured with protein A agarose (Pierce). To detect BAK or BAX oligomerization, tBID-inducible cells were treated with doxycycline for 6 hours and then incubated with 5 mM BMH (Thermo Fisher Scientific) for 30 min at room temperature.

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In vitro cytochrome c release and protein cross-linking

Gel filtration fractions containing BAK-associated complexes were concentrated and buffer exchanged using Amicon Ultra centrifugal filters (10-kD MWCO; Sigma) with mitochondrial isolation buffer (200 mM mannitol, 70 mM sucrose, 1 mM EGTA, and 10 mM HEPES, pH 7.5). Samples (1.2 ml per complex) were diluted >20-fold to reduce the CHAPS concentration to <0.1% and concentrated to 50 $\mu$ l. Each complex recovered from a gel filtration run of 200 $\mu$ g of mitochondria was incubated with $Bax^{-/-}Bak^{-/-}$ mitochondria (1 mg/ml) in a final volume of 100 $\mu$ l. Cytochrome c release was quantified by colorimetric enzyme-linked immunosorbent assay (ELISA, R&D Systems) as described previously (7) and normalized to gel filtration buffer controls. To detect BAK oligomers, elution fractions were incubated with 2.5 mM BMH (Thermo Fisher Scientific) for 30 min at room temperature, quenched with NuPAGE sample buffer, resolved by 4 to 12% NuPAGE, and analyzed by anti-BAK immunoblotting.

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ADP import assay

The ADP import assay was performed as described previously $(58)$ . Mitochondria were isolated $(4, 7, 8)$ and resuspended at 0.5 mg/ml in ADP import buffer (250 mM sucrose, 20 mM HEPES, 10 mM KCl, 5 mM succinate, 3 mM $KH_{2}PO_{4}$ , 1.5 mM $MgCl_{2}$ , 1 mM EGTA, 5 $\mu$ M rotenone, pH 7.2). Mitochondrial suspensions (400 $\mu$ l) were incubated with or without 50 $\mu$ M atractyloside (Sigma), supplemented with 0.5 $\mu$ Ci of ${}^{14}C$ -ADP (PerkinElmer NEN Radiochemicals), and incubated on ice for 10 min. Reactions were stopped by adding 700 $\mu$ l of ADP import buffer containing 50 $\mu$ M atractyloside. Samples were washed twice, mixed with scintillation cocktail, and analyzed using an LS6000 liquid scintillation counter (Beckman Coulter). ANT-dependent ADP uptake was calculated as the difference in counts between samples with and without atractyloside preincubation. To isolate mitoplasts, purified mitochondria (0.5 mg/ml) were treated with 0.15% (w/v) digitonin (Sigma) in mitoplast isolation buffer (220 mM mannitol, 70 mM sucrose, 2 mM HEPES, pH 7.5) for 10 min on ice and pelleted at 10,000g for 10 min.

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Quantification of mitochondrial DNA efflux

Cells $(1.5 \times 10^{6})$ were harvested and divided into two portions. One-fifth was pelleted at 2000 rpm for 4 min, and total DNA was extracted using the DNeasy Blood and Tissue Kit (Qiagen). The remaining cells were pelleted, permeabilized for 5 min on ice in digitonin permeabilization buffer (0.025% digitonin, 10 mM KCl, 5 mM MgCl $_{2}$ , 1 mM EDTA, 1 mM EGTA, 250 mM sucrose, 20 mM HEPES, pH 7.2), and centrifuged at 15,000g for 10 min at 4°C. Supernatants were centrifuged at 100,000g for 60 min at 4°C using an Optima MAX-XP ultracentrifuge (Beckman Coulter). The resulting supernatants were collected as the cytosolic fraction, and DNA was purified using the QIAquick Nucleotide Removal Kit (Qiagen). Whole-cell and cytosolic DNA were analyzed by quantitative PCR (qPCR) using SYBR Green Master Mix on a ViiA 7 or QuantStudio 3 Real-Time PCR System (Thermo Fisher Scientific). Nuclear DNA was detected using primers for mouse Tert or human ACTB, and mtDNA using D-loop primers. Nuclear DNA was undetectable in cytosolic fractions, confirming the absence of nuclear lysis. Cytosolic mtDNA Ct values were normalized to whole-cell mtDNA, and fold increases in mtDNA efflux were calculated from the normalized cytosolic mtDNA abundance. Primers used for qPCR were as follows: mouse D-loop, 5'-CATCTCGATGGTATCGGGTC-3' and 5'-GGTGCGTCTAGACTGTGTGC-3'; mouseTert,5'-CTAGCTCATGTGTCAAGACCCTCTT-3' and 5'-GCCAGCACGTTTCTCTCGTT-3'; human D-loop,5'-GGATCACAGGTCTATCACCCTA-3' and 5'-CAGCGTCTCGCAATGCTATC-3'; and human ACTB 5'-GGCACCCAGCACAATGAAGATC-3' and 5'-TGAGGACCCTGGATGTGACAG-3'.

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In vitro mitochondrial DNA release from mitoplasts

Mitochondria (200 $\mu$ g) isolated from untreated or doxycycline-treated tBID-inducible $Apaf1^{-/-}$ , $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ , and $Apaf1^{-/-}Vdac1^{MT}Vdac2^{MT}$ MEFs were sequentially extracted with CHAPS lysis buffers to obtain the 2% CHAPS-soluble mitochondrial subfraction. This subfraction was separated on a Superdex 200 Increase 10/300 GL column, and fractions corresponding to the indicated molecular weights were collected. To isolate mitoplasts, mitochondria (0.5 mg/ml) from $Bax^{-/-}Bak^{-/-}Vdac1^{-/-}Vdac2^{-/-}Apaf1^{-/-}$ MEFs were treated with 0.15% (w/v) digitonin (Sigma) in mtDNA release buffer (142.5 mM KCl, 250 $\mu$ M CaCl $_{2}$ , 20 mM Tris-Cl, pH 7.4) supplemented with EDTA-free protease inhibitor cocktail for 10 min on ice and pelleted at 10,000g for 10 min. Gel filtration fractions containing BAK-associated complexes were buffer exchanged and concentrated using Amicon Ultra Centrifugal Filters (10 kD MWCO, Sigma). Samples (1.2 ml per complex) were diluted >20-fold with mtDNA release buffer to reduce CHAPS to <0.1% and concentrated to 50 $\mu$ l. Each BAK-associated complex, recovered from a gel filtration run of 200 $\mu$ g of mitochondria, was incubated with mitoplasts derived from 50 $\mu$ g of mitochondria in 100 $\mu$ l for 30 min at 30°C. Samples were centrifuged at 10,000g for 10 min at 4°C, and DNA was extracted from the pellets using the DNeasy Blood and Tissue Kit (Qiagen). Supernatants were centrifuged at 100,000g for 60 min at 4°C using an Optima MAX-XP ultracentrifuge (Beckman Coulter), and DNA was purified from the resulting supernatants using the QIAquick Nucleotide Removal Kit (Qiagen). mtDNA was quantified by qPCR using D-loop primers on a ViiA 7 or QuantStudio 3 Real-Time PCR System (Thermo Fisher Scientific). mtDNA Ct values in ultracentrifugation supernatants were normalized to those of the 10,000g pellets, and mtDNA release was calculated from the normalized values relative to mitoplasts incubated with buffer alone.

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Reverse transcription and qPCR

Total RNA was extracted from cells using TRIzol (Thermo Fisher Scientific). Reverse transcription was performed with oligo(dT) and random decamer primers using SuperScript II (Thermo Fisher Scientific). qPCR was performed in duplicate using SYBR Green Master Mix (Thermo Fisher Scientific) and gene-specific primers on a ViiA 7 or QuantStudio 3 Real-Time PCR System (Thermo Fisher Scientific). Data were normalized to β-Actin. qPCR primers were mouse Ifnb1, 5'-CCTTTGCCATCCAAGAGATGCTC-3' and 5'-AGTTGAGGACATCTCCCACGTC-3'; mouse Actb, 5'-GCCATGTACGTAGCCATCCAGGC-3' and 5'-CTCCAGGGAGGAAGAGGATGCGGC-3'; human IFNB1, 5'-GCTCTCCTGTTGTGCTTCTCCA-3' and 5'-TGAGGCAGTATTCAAGCCTCCC-3'; and human ACTB, 5'-TCCCTGGAGAAGAGCTACGAG-3' and 5'-AGGAAGGAAGGCTGGAAGAGTG-3'.

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Quantification of mitochondrial calcium

Cells were seeded in 4-well chamber slides (Nunc Lab-Tek II) at $4.5 \times 10^{4}$ cells per well and treated the next day with doxycycline (1 $\mu$ g/ml; Sigma) or ABT-263 (2 $\mu$ M; Selleck Chemicals) plus S63845 (10 $\mu$ M; Chemietek) for 4 hours; untreated cells served as controls. Cells were fixed with 4% paraformaldehyde, stained with 4',6-diamidino-2-phenylindole (DAPI, Sigma), and imaged using a Leica SP5 inverted confocal microscope equipped with a 40×/1.2 numerical aperture (NA) water-immersion objective (HCX PL APO; #506341). Mean green fluorescence intensity per cell ( $F_{0}$ ) was calculated as $F_{0} = F\_c/S$ , where $F\_c$ is the total green fluorescence intensity of each cell and S is the corresponding cell area. Nuclear segmentation and cell-region delineation were adapted from a previously described method (59), and quantification was performed using ImageJ. For each condition, 50 to 200 cells were quantified, and relative fluorescence intensity was calculated by normalization to the mean of control cells across three independent experiments. Statistical significance was assessed by Student's t test to determine whether the mean relative fluorescence intensity of one sample exceeded 150% of that of the other.

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Confocal microscopy and colocalization analysis

Cells expressing TOMM20-GFP and TIMM50-mCherry were plated in 4-well chamber slides (EMD Millipore) and treated with the indicated agents at 37°C. Cells were fixed with 4% paraformaldehyde (Sigma) for 15 min, washed three times with PBS, and incubated for 1 hour at room temperature in permeabilization and blocking buffer containing 0.1% Triton X-100 (Sigma), 1% BSA (EMD Millipore), and 5% goat serum (Sigma) in PBS. Cells were incubated overnight at 4°C with primary antibodies against TOMM20 (Abcam, #ab13970) and mCherry (CST, #43590S) diluted in blocking buffer. After three washes, cells were incubated for 1 hour with goat anti-chicken AF488 (Invitrogen, #A-11039) and goat anti-rabbit AF594 (Thermo Fisher Scientific, #A-11012) secondary antibodies. After two additional washes, cells were stained with DAPI (Sigma) and imaged using a Zeiss LSM 880 confocal microscope equipped with a 63×/1.4 NA Plan Apochromat objective. For colocalization analysis, images were converted to 8-bit format, subjected to default autothresholding, and analyzed using the Coloc2 plugin in Fiji to calculate Manders' colocalization coefficients (60, 61).

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Transmission electron microscopy

Transmission electron microscopy was performed by the Microscopy Core Facility at Weill Cornell Medicine. Cell pellets were fixed with modified Karnovsky's fixative, followed by secondary fixation with reduced osmium tetroxide $(62)$ . After graded ethanol dehydration, samples were embedded in an Epon analog resin and sectioned at 65 nm using a DiATOME diamond knife on a Leica Ultracut S ultramicrotome. Ultrathin sections were contrasted with lead citrate as described previously $(63)$ and imaged using a JEM-1400 transmission electron microscope (JEOL) operated at 100 kV. Digital images were acquired with a Veleta 2K × 2K CCD camera (EMSIS GmbH).

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Live-cell imaging

Cells were seeded in 4-well chamber slides (Nunc Lab-Tek II) at $4.5 \times 10^{4}$ cells per well and treated the next day with doxycycline (1 $\mu$ g/ml)

or left untreated. Phase-contrast live-cell imaging was performed using a Zeiss microscope controlled by ZEN software and equipped with a 40×/0.6 NA air objective (LD Achroplan 40×/0.6 Ph2; Zeiss). Time-lapse images were acquired 1 to 5 hours after doxycycline treatment for WT MEFs and 36 to 41 hours after treatment for $Apaf1^{-/-}$ MEFs to assess cellular morphology and behavior.

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TUNEL staining

WT and $Apaf1^{-/-}$ MEFs were untreated or treated with doxycycline (1 $\mu$ g/ml) for 3 and 40 hours, respectively, to induce tBID. Cells were harvested, fixed overnight in 4% paraformaldehyde at room temperature, washed with PBS, and pelleted at 1700 rpm for 5 min at 4°C. Fixed pellets were paraffin embedded and processed for TUNEL staining by the Molecular Cytology Core Facility at MSKCC. Sections (5 $\mu$ m) were mounted on glass slides, dried overnight at room temperature, and incubated at 60°C for 1 hour. Slides were deparaffinized in xylene, rehydrated through graded ethanol to water, and processed on a Discovery Ultra autostainer (Ventana Medical Systems, Roche). After heat retrieval at 37°C, slides were treated with Endogenous Biotin Blocking Kit (Ventana Medical Systems) for 20 min and incubated for 2 hours with TdT (1000 U/ml; Roche) and biotin-dUTP (4.5 nmol/ml; Roche). Signals were detected with streptavidin-HRP (Ventana Medical Systems) for 32 min and amplified using the Alexa Fluor 488 Tyramide SuperBoost Kit (1:150; Thermo Fisher Scientific) for 16 min. Slides were counterstained with DAPI (5 $\mu$ g/ml; Sigma) for 5 min, mounted with Mowiol 4-88 (Sigma), and imaged using an LSM 880 confocal microscope (Zeiss) equipped with a 40×/1.3 NA oil-immersion objective.

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Quantification of cytosolic cathepsin B activity

Cells were harvested before or after cell death induction, pelleted at 2000 rpm for 4 min, and permeabilized for 5 min on ice in digitonin buffer containing 0.025% digitonin, 10 mM KCl, 5 mM MgCl₂, 1 mM EDTA, 1 mM EGTA, 250 mM sucrose, and 20 mM HEPES (pH 7.2). Lysates were centrifuged at 15,000g for 10 min at 4°C to remove nuclei, mitochondria, and membrane-bound organelles. Supernatants were centrifuged at 100,000g for 60 min at 4°C using an Optima MAX-XP ultracentrifuge (Beckman Coulter). The resulting supernatants were collected as the cytosolic fraction, and cathepsin B activity was measured using the Cathepsin B Activity Assay Kit (Abcam). Fluorescence was measured using a SpectraMax M5 multimode microplate reader (Molecular Devices) and normalized to untreated controls.

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Quantification of cellular ATP levels

Cells were seeded in 6-well plates at $2.5 \times 10^{5}$ cells per well and treated the next day with the indicated agents or left untreated. Cells were harvested, counted, and $1 \times 10^{4}$ cells were used per assay. Cellular ATP was measured using the ATP Bioluminescence Assay Kit HS II (Roche). Luciferase reagent (50 $\mu$ l) was mixed with 50 $\mu$ l of diluted sample, and luminescence was measured using a GloMax Navigator microplate luminometer (Promega). A standard curve was generated for each experiment using serial dilutions of the ATP standard provided in the kit, and signals were normalized to untreated controls.

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Statistics

Statistical significance was assessed using two-tailed unpaired Student's t tests in GraphPad Prism 9 or 10. Data are presented as mean ± SD, with P < 0.05 considered statistically significant unless otherwise stated. Significance is denoted in the figures as follows: \*P < 0.05; \*\*P < 0.01; \*\*\*P < 0.001; and \*\*\*\*P < 0.0001. For Fig. 5, A to D, Student's t tests were used to determine whether the mean relative fluorescence intensity of one sample exceeded 150% of that of the other. In Fig. 5A, n = 87, 105, 131, and 110 for sgCtrl control, sgCtrl doxycycline, sgBax-sgBak control, and sgBax-sgBak doxycycline, respectively. In Fig. 5B, n = 117, 139, 117, 127, 76, 56, 98, and 80 for Apaf1 $^{-/-}$ #1 control, Apaf1 $^{-/-}$ #1 doxycycline, Apaf1 $^{-/-}$ #2 control, Apaf1 $^{-/-}$ #2 doxycycline, Apaf1 $^{-/-}$ Vdac1 $^{-/-}$

$Vdac2^{-/-}$ #1 control, $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ #1 doxycycline, $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ #2 control, and $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ #2 doxycycline, respectively. In Fig. 5C, n = 101, 111, 124, 213, 195, 182, 137, and 107 for $Apaf1^{-/-}$ #1 control, $Apaf1^{-/-}$ #1 AS, $Apaf1^{-/-}$ #2 control, $Apaf1^{-/-}$ #2 AS, $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ #1 control, $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ #1 AS, $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ #2 control, and $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ #2 AS, respectively. In Fig. 5D, n = 157, 130, 135, 137, 130, and 124 for $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ control, $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ doxycycline, $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ expressing VDAC1/2 $^{WT}$ control, $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ expressing VDAC1/2 $^{WT}$ doxycycline, $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ expressing VDAC1/2 $^{MT}$ control, and $Apaf1^{-/-}Vdac1^{-/-}Vdac2^{-/-}$ expressing VDAC1/2 $^{MT}$ doxycycline, respectively. The numbers of independent experiments, samples, or events and the statistical tests used are indicated in the figure legends. All data are from at least two independent experiments with consistent results. No exclusion criteria were preestablished, and no data were excluded. Sample sizes were not predetermined statistically. Cell death assays were not blinded because administration of specific treatments required knowledge of treatment groups.

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ACKNOWLEDGMENTS

We apologize to investigators whose work could not be cited due to space limitations. We thank the MSKCC Molecular Cytology Core Facility, especially Y. Romin and E. Chan, and the Weill Cornell Medicine Microscopy & Image Analysis Core, especially L. Cohen-Gould and J. Jimenez. Funding: This work was supported by the National Institutes of Health (NIH) National Cancer Institute (NCI) (grant R01 CA252658 to E.H.C. and grant P30 CA008748 to C.M.R.) and the Geoffrey Beene Cancer Research Center (MSKCC) (E.H.C.). Author contributions: S.Y. and H.K. designed and conducted experiments and analyzed data. E.H.C. conceived and designed the study, analyzed and interpreted data, and supervised the project. G.L., N.T., H.T., S.R., C.C., Z.L., and N.T. conducted some experiments. J.J.H. analyzed and interpreted data. Competing interests: J.J.H. is a cofounder of ICEN Therapeutics. E.H.C. is a consultant for ICEN Therapeutics. These relationships are unrelated to the present work. The authors declare no other competing interests. Data, code, and materials availability: All data are available in the main text or the supplementary materials. License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.aea2181

Figs. S1 to S11; Tables S1 to S3; Movies S1 and S2; MDAR Reproducibility Checklist Submitted 30 June 2025; resubmitted 10 April 2026; accepted 2 September 2026

10.1126/science.aea2181

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RESEARCH ARTICLES

MOLECULAR BIOLOGY

Noncoding transcription controls the developmental dynamics of long-range gene regulation

Philippe J. Batut $^{1,2*}$ and Michael S. Levine $^{1*}$

The genomic regions regulating gene expression are often themselves transcribed into a variety of noncoding RNAs (ncRNAs). However, the regulatory roles of this noncoding transcription remain largely unknown. By using live imaging, we reveal that the sequential transcription of ncRNAs emanating from distinct regulatory elements underlies gene activation in Drosophila embryos. Single-allele covisualization uncovers that optimal gene activation is achieved by only moderate levels of enhancer activity. Disrupting enhancer-associated ncRNAs causes precocious gene activation, providing evidence that ncRNAs control the timing of gene expression in development. We further show that enhancer transcription can regulate long-range interactions within complex regulatory landscapes. We propose that ncRNAs locally modulate regulatory element activity in cis to shape genome organization and orchestrate the temporal control of gene expression in development.

In animal genomes, many genes are under the control of vast regulatory landscapes that can span megabases and are often disrupted in disease (1–3). These regions harbor constellations of regulatory elements, including enhancers, that drive transcription in specific spatiotemporal patterns during development (1–5). We and others have shown that the spatial organization of the genome can play an instructive role in specifying regulatory interactions (6, 7), enabling enhancers to control transcription at gene promoters over large genomic distances (1–11). These regulatory regions are themselves pervasively transcribed, producing myriad noncoding RNAs (ncRNAs) (12–18). In particular, ncRNAs have emerged as a hallmark of active enhancers in both vertebrates (19) and invertebrates (20, 21). Although prior studies have established cis-regulatory roles for a number of individual ncRNAs (15, 22–25), including both long and short enhancer-associated RNAs (eRNAs) (16, 17), it remains unclear how much of this noncoding transcription is functionally relevant, rather than merely spurious or opportunistic (15, 23, 26). How it is deployed to regulate gene expression during development also remains largely unexplored. Lastly, we have a limited understanding of how ncRNAs operate in the context of long-range regulation and how they might exploit—or even control—aspects of genome organization. Using the Drosophila embryo as a model system, we combined genome-wide and live-imaging approaches to determine the roles of noncoding transcription at regulatory elements in the developmental control of gene expression.

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Developmentally regulated ncRNA transcription at regulatory elements

We analyzed transcription genome-wide in early embryos, at the stage when the blueprint of the body plan is being established, using previously published PRO-cap data (20). This method maps transcriptional initiation sites at single-nucleotide resolution by identifying the 5' ends of nascent RNAs and is well suited for the detection of rare or unstable transcripts. We excluded the promoters of protein-coding genes and focused our analysis solely on ncRNAs. We detected noncoding transcription initiating within 40% of active enhancers [see supplementary materials (SM), materials and methods], in agreement with previous reports (20, 21) (Fig. 1, A and B, and fig. S1, A to C). This represents a strong enrichment over random expectation (fig. S1C). In addition to enhancers, we also analyzed transcription at tethering elements. This class of regulatory sequences influences three-dimensional (3D) genome organization (6, 7) and is functionally distinct from enhancers (fig. S1, A and B). We showed in a prior study that tethering elements foster specific long-range enhancer-promoter interactions and gene activation (6) (Fig. 1A). PRO-cap analysis revealed that 33% of tethering elements also produce ncRNAs (Fig. 1B and fig. S1, A to C).

Although the prevalence of noncoding transcription across regulatory regions is well established, its functional relevance is not. To gain insights into this question, we measured sequence conservation at the transcription start sites (TSSs) of ncRNAs. By leveraging the single-nucleotide resolution of PRO-cap, we were able to detect strong patterns of sequence conservation precisely centered on the TSSs of enhancer- and tether-associated ncRNAs (Fig. 1C and fig. S1, D and E). This shows that noncoding transcription at regulatory elements is under strong selective pressure—suggesting that it serves important biological functions across the genome.

This is illustrated by the Hox gene Sex combs reduced (Scr), one of the master regulators of animal body plans (27) and the ortholog of human Hox5 genes (28). We have previously shown that Scr is regulated in embryos by a distal enhancer located \~35 kb upstream of its promoter and that a distal tethering element (DTE) facilitates this long-range enhancer-promoter interaction (6). Both the Scr enhancer and the DTE are transcribed in embryos to produce distinct, well-defined long ncRNAs (Fig. 1D). To evaluate their biological relevance, we reanalyzed developmental transcriptomic time series in multiple Drosophila species from our previous study of ncRNA conservation (29). These datasets, generated with a TSS profiling method named RAMPAGE (30), show that both ncRNAs have been functionally conserved for >35 million years. They are transcribed from recognizable core promoters displaying clear sequence conservation (fig. S2, A and B). In addition, the developmental transcription dynamics of enhancer- and tether-associated ncRNAs across the genome, including the two ncRNAs at the Scr locus, are also highly conserved (Fig. 1, E and F, and figs. S1, F and G, and S2, A and B). Notably, the temporal transcription profile for the Scr eRNA is among the top 1% most conserved in the entire genome—more conserved than that of the Scr gene itself (Fig. 1F). These observations suggest that the transcriptional dynamics of both Scr ncRNAs are critical for development.

To characterize these dynamics at high resolution, we engineered the Scr locus to visualize the transcription of endogenous ncRNAs in single cells of developing embryos (Fig. 1G and movies S1 to S3). Our live imaging data reveal a precisely ordered “launch sequence,” in which the enhancer, tethering element, and gene are activated in robustly timed succession (Fig. 1H and fig. S3). These observations suggest that the sequential activation of distinct regulatory elements may underlie the temporal control of gene expression. Contrary to the expectation that enhancer activity should instructively determine gene activity, our quantitative analysis reveals that the Scr gene shows no detectable transcription for a 45-min period during which the enhancer displays its strongest activity, suggesting additional layers of regulation.

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Single-cell transcriptional dynamics of an enhancer-gene pair in vivo

We sought to better understand the quantitative relationship between the enhancer and its target gene by measuring their transcription dynamics in live embryos in cis, on a single allele (Fig. 2A and movie S4).

A Tethering elements foster long-range enhancer-promoter interactions

B

c

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D Organization of the Scr HOX locus

E Developmental dynamics in 5 species

F Conservation of developmental dynamics

G Single-cell imaging of transcription

H Live imaging of ncRNA transcription

Fig. 1. Noncoding transcription at regulatory elements is widespread, conserved, and highly dynamic. (A) Enhancers can activate transcription at target promoters over large genomic distances. Tethering elements are devoid of intrinsic enhancer activity but foster specific long-range enhancer-promoter interactions (6). (B) Genome-wide analysis of PRO-cap data from 3- to 4-hour-old embryos identifies active TSSs within 40% of active intergenic enhancers and 33% of tethering elements. Heatmaps show the distribution of PRO-cap signal over 800-bp windows centered on the identified TSSs, on the same genomic strand (see SM, materials and methods). (C) Mean sequence conservation (phastCons score) at each position across an 800-bp window centered on each TSS, for the classes defined in (B). Shaded envelope: SEM; gray bars: aggregate PRO-cap signal. (D) Micro-C contact map and annotation of the HOX gene Scr (part of the Antennapedia complex, ANT-C). The Scr distal regulatory region includes an early embryonic (EE) enhancer, as well as a distal tethering element (DTE) engaging in a focal contact (arrow in Micro-C panel) with a promoter-proximal tethering element (TE) (6). The EE enhancer harbors the TSS for the enhancer-associated ncRNA [eRNA, CR44931, \~7.4 kb (thick boxes represent exons)], and the DTE harbors the TSS for the distal tether-associated ncRNA (dtRNA, CR45559, \~0.6 kb). ftz and Antp are other protein-coding genes at the locus. (E) Transcriptional dynamics over embryonic development for four well-known developmental genes and the Scr eRNA, in five Drosophila species (spanning \~35 million years of divergence). Transcriptome analysis was carried out at 1-hour resolution throughout embryogenesis for each species (29); for every gene, the five curves correspond to the five species. All time series were computationally aligned to the D. melanogaster reference, which defines the time axis (hours after egg laying). The four conserved developmental genes show the accuracy of temporal alignment between time series. (F) Distribution of conservation scores for the transcriptional dynamics of all active promoters across the genome (N = 10,229 promoters). Arrows show transcriptional dynamics conservation scores for the two alternative promoters of the Scr gene, the eRNA promoter, and the dtRNA promoter. (G) Live imaging of active transcription foci for the endogenous Scr gene and its eRNA, in a trans configuration. The images are maximum intensity projections of individual confocal z-stacks from a 4D live microscopy dataset of a late blastoderm-stage embryo [nuclear cycle 14 (NC14)]; Gray: cell nuclei (histone H2A); magenta: eRNA (PP7); green: Scr gene (MS2). The images were optimized for display purposes only (2x upsampling and Gaussian smoothing); quantitative analysis was conducted on the raw 4D data (see SM, materials and methods). (H) Quantification of the mean transcriptional output per nucleus over the NC14 interphase for the endogenous Scr gene and its two associated ncRNAs (envelope: SEM across biological replicates). Each transcript was endogenously tagged individually with MS2 and visualized in different embryos.

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A Co-visualization of eRNA & mRNA transcription in vivo

Temporal dynamics of transcription at enhancer-gene pair

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C Quantitative relationship between enhancer & gene transcription

Fig. 2. Single-cell transcriptional dynamics of a developmentally regulated enhancer-gene pair. (A) (Top) Covisualization of active transcription foci (arrowheads) for the endogenous Scr gene and its enhancer-associated RNA (eRNA), on the same allele (cis configuration). Gray: nuclei; purple: Scr gene (PP7); cyan: eRNA (MS2). Scale bar, 2 $\mu$ m (2x upsampling and Gaussian smoothing, for display only). (Bottom) Transcription signal for a single representative nucleus. The two channels are normalized to their respective maxima; the arrow designates an individual gene activation event. (B) (Top) Single-cell transcription signal for the Scr gene and its enhancer (eRNA) over all gene activation events observed, aligned to the onset of gene transcription (N = 12 embryos, n = 118 events; envelope: SEM across all events). Because the detection of gene transcription necessitates transcriptional elongation through the detection cassette, the dashed lines indicate the temporal window of gene activation, based on in vivo estimates of elongation speed (see SM, materials and methods). (Bottom) Time-lagged cross-correlation between the enhancer and gene transcription signals (Arrow: cross-correlation minimum; envelope: 90% confidence interval estimated from 1000 bootstraps). (C) (Top) Individual enhancer activation events (n = 267) aligned to the onset of enhancer transcription. Single-cell traces are color-coded according to the minimum signal reached during the 3-min period after transcriptional onset (dashed lines). (Bottom) Relationship between enhancer transcription (minimum signal reached during the 3-min period after enhancer activation) and subsequent gene transcription (maximum increase in gene transcription in the 4-min period after enhancer activation). Timing for gene transcription is offset according to estimates of elongation speed (see SM, materials and methods). Single-cell events are sorted into eight quantiles of enhancer transcription signal; the dots show the mean enhancer and gene transcription signals for each quantile (error bars: SEM along both axes).

This revealed that gene activation events do not appear to coincide with discrete enhancer activation events. Rather, the enhancer appears to be strongly transcribed for an extended period of time preceding gene activation. The onset of Scr expression actually coincides with a decrease in enhancer transcription, as evidenced by a sharply negative cross-correlation between the two signals around the time of gene activation (Fig. 2B).

We further quantified the relationship between the strength of individual enhancer activation events and the magnitude of subsequent increases in gene transcription. This analysis uncovered a strongly nonmonotonic relationship between enhancer and gene transcription: Enhancer activity is positively correlated with gene activity at low levels but anticorrelated at higher levels (Fig. 2C). A negative control in which the eRNA and gene were measured in a trans configuration on homologous chromosomes showed no such correlation (fig. S4). Together, these observations suggest that enhancer transcription may, counterintuitively, inhibit gene activation.

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Noncoding transcription controls the timing of gene activation

We tested the possibility that eRNA transcription inhibits Scr expression by generating a precise 45-bp deletion of the eRNA TSS within the endogenous locus and measuring the impact on gene transcription using live imaging. This deletion leads to augmented levels of Scr transcription, suggesting that transcription of the enhancer attenuates gene expression (Fig. 3, A and B, and fig. S5, A to C). This loss of eRNA transcription also leads to markedly precocious activation of the gene. The spatial pattern of gene activity, by contrast, is only slightly altered, showing that the eRNA specifically controls the timing of Scr activation (Fig. 3B and fig. S5, A to C). Deletion of the eRNA TSS in trans has a negligible effect on gene activity and dynamics, showing that the eRNA controls the timing of gene activation strictly in cis (fig. S6).

To rule out the possibility that deletion of the eRNA TSS results in the removal of an Scr silencer element located within the eRNA core promoter, we replaced it with the well-characterized heterologous core promoter from the segmentation gene even-skipped (eve). This not only restored eRNA transcription but also increased it several-fold over wild type, as quantified by live transcription measurements (Fig. 3, A and B). The eve-driven eRNA fully rescues Scr repression, resulting in both diminished levels and delayed onset of Scr expression (Fig. 3B and fig. S7, A and B). Moreover, augmented eRNA transcription by the eve promoter causes an even more marked reduction in Scr expression levels and pronounced delay in the timing of activation as compared with wild type.

Further evidence supporting the model that eRNA transcription controls the levels and timing of Scr expression was obtained by creating nucleotide substitutions within the eve promoter. Five nucleotides were substituted in the eve Initiator (INR) element, which has been shown to strongly impair promoter activity (31). This subtle substitution results in precocious activation and increased levels of Scr expression, with an effect size similar to that observed with the original

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A Enhancer-associated RNA (eRNA) TSS deletion (Endogenous locus)

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B Enhancer ncRNA transcription

Scr gene transcription

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C Gene repression depends on eRNA transcript length

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D DTE-associated RNA (dtRNA) TSS deletion

Fig. 3. Transcription from a HOX locus enhancer and DTE controls the dynamics of gene expression. (A) Schematic of CRISPR-mediated deletion of the Scr eRNA TSS (45 bp), and Scr eRNA TSS replacement with the eve core promoter, at the endogenous locus. (B) Live single-cell measurements of transcription for the Scr enhancer (left) and gene (right) upon deletion of the eRNA TSS and replacement with the eve core promoter. (C) Live transcription measurements for the Scr gene upon replacement of the body of the eRNA transcription unit (\~7.3 kb, from 37 bp downstream of the TSS to 39 bp upstream of the first PAS, including the intron and part of both terminal exons) by a sequence derived from the phage $\lambda$ genome, with and without added insertion of a premature SV40 PAS. (D) Live transcription measurements for the Scr gene upon deletion of the dtRNA TSS.

deletion of the endogenous eRNA TSS (fig. S8). Together, these results argue that loss of eRNA transcription is responsible for the changes in the timing and levels of Scr expression observed upon deletion of the eRNA promoter.

We next sought to gain insights into the underlying mechanism by investigating the dependency of Scr repression on the sequence and length of the eRNA. We replaced the body of the eRNA transcript [from 37 base pairs (bp) downstream of the TSS to 39 bp upstream of the polyadenylation signal (PAS)] with an unrelated sequence derived from the genome of bacteriophage $\lambda$ . This 7.3-kb sequence substitution maintains overall transcript length and was designed to only alter sequences situated downstream of the Scr enhancer (fig. S9A). This ncRNA substitution resulted in an even stronger repression of Scr as compared with wild-type (Fig. 3C and fig. S9), ruling out the possibility that transcription of the eRNA exposes cryptic silencer elements (32) impinging on Scr expression, because $\lambda$ replacement completely removes the native eRNA transcription unit.

It is possible that Scr repression involves competition between the Scr and eRNA promoters for factors recruited in rate-limiting amounts by the enhancer, rather than the synthesis of full-length eRNAs. To examine these potential mechanisms, we tested both synthetic reporter genes and edits of the endogenous Scr locus. Transgenic reporter assays indicate that although promoter competition can slightly reduce gene activity, it is not sufficient to account for the long delay in the timing of Scr activation seen in wild-type embryos (fig. S5D). To directly test whether synthesis of full-length transcripts is required, we inserted a simian virus 40 polyadenylation signal (SV40 PAS) within the 5' region of the eRNA transcription unit, 280 bp downstream of the eRNA TSS. To exclude any possible contributions from unknown DNA silencer elements exposed during eRNA transcription, the PAS was inserted in the context of $\lambda$ replacement. Premature termination of the $\lambda$ ncRNA caused a marked increase in the levels of Scr transcription relative to $\lambda$ replacement alone (Fig. 3C), and gene activation occurs even earlier than in wild-type embryos (fig. S9). Taken together, these observations suggest that the process of eRNA transcription alone is not sufficient for the repression and temporal control of gene activity. Instead, normal Scr transcriptional dynamics require the production of full-length ncRNAs, regardless of their primary sequence.

To explore whether different ncRNAs at the Scr locus may be endowed with distinct regulatory functions, we deleted the TSS of the ncRNA transcribed from the DTE (dtRNA). In contrast to the eRNA, loss of dtRNAs does not affect the temporal dynamics of Scr activation but instead leads to a failure to reach the maximum rate of transcription (Fig. 3D and fig. S5, B and C). Together, these results show that the ncRNAs encoded by the enhancer and DTE have opposing regulatory functions—one repressive, one activating—and that the eRNA specifically determines the timing of gene activation. Deletion of either the dtRNA or eRNA TSS is consequential. Each results in classical Scr homeotic phenotypes—changes in the number of sex combs on the forelegs of adult males (fig. S10). This suggests that cis-regulatory ncRNAs influence organismal fitness.

To determine the generality of the Scr model, we also investigated the potential regulatory roles of an ncRNA located \~34 kb upstream of the second promoter of the Antennapedia gene (Antp P2), which we identified on the basis of RAMPAGE and PRO-cap data. This ncRNA is transcribed from a putative tethering element that forms a weak regulatory loop with the P2 promoter (fig. S11A). Transcription of this ncRNA is observed in five species spanning 35 million years of evolutionary divergence, and its temporal activity profile during embryonic development is highly conserved (fig. S11B). A focal deletion of its TSS (45 bp; fig. S11A) leads to a subtle yet significant increase in the transcription rate of the Antp gene (fig. S11C). This ncRNA appears to modulate the spatial pattern of Antp expression by quantitatively repressing gene activity exclusively in the anterior half of its normal expression domain (fig. S11, C and D).

We also identified several additional ncRNAs in the regulatory regions of other developmental control genes that exhibit distinct spatiotemporal expression patterns as compared with their associated genes. Once again, we found that these ncRNAs exhibit high conservation throughout the Drosophila clade (fig. S12). These observations raise the possibility that ncRNAs might be used as a widespread strategy for the precise control of transcriptional dynamics of developmental control genes.

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Enhancer transcripts control tethering element activity and genome organization

The ability of ncRNAs to regulate transcription of the Scr gene over long distances prompted us to investigate their relationship to the tethering elements that promote long-range interactions. An attractive hypothesis is that the distal enhancer and its associated eRNA may regulate the activity of the DTE. We tested this model by measuring the transcription of the dtRNA in live embryos upon targeted edits of the enhancer. Deletion of the entire enhancer, which we have previously shown to diminish Scr activity (6), also leads to a sharp decrease in dtRNA transcription—establishing that transcription of the DTE is primarily under the control of the Scr enhancer (Fig. 4A). By contrast, a focal deletion of the eRNA TSS causes a substantial increase in dtRNA transcription (Fig. 4A). This result demonstrates that transcription of the eRNA strongly inhibits the transcriptional activity of the DTE, in addition to repressing Scr.

To investigate whether the DTE is required for the eRNA to regulate Scr expression, we simultaneously deleted the DTE and the eRNA TSS on the same allele and measured the regulatory impact on gene transcription. This revealed complete epistasis with respect to the timing of Scr activation. The double mutant exhibits the same delay in activation as that seen with the loss of the DTE alone, indicating that the eRNA exerts its regulatory influence on Scr only when the DTE is present (Fig. 4B and fig. S13, A and B). A plausible explanation for this could be that the DTE is simply required for eRNA transcription, but we excluded this possibility by showing that deletion of the DTE does not abolish, but rather slightly increases, eRNA transcription (fig. S13, C and D). Instead, this interaction suggests an interplay between non-coding transcription and genome organization. The biological relevance of this cross-talk is underscored by the synthetic lethality observed at late embryonic stages in $\Delta eRNA,\Delta DTE$ double mutants.

To determine whether eRNAs influence the DTE's ability to form a regulatory loop with the Scr promoter, we carried out Micro-C analysis $(33)$ in edited embryos lacking the eRNA TSS. Although the general organization of the locus is largely unaffected, disruption of the eRNA leads to increased DTE-promoter interactions (Fig. 4C and fig. S14). This is the only significant change detected among the 100 strongest loops across the genome, including a DTE-promoter loop at the neighboring Antp locus (fig. S14). Taken together, these results suggest that eRNA transcription regulates the activity of the DTE and its ability to engage in long-range activation of Scr.

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Discussion

Complex regulatory regions harboring multiple cis-elements and ncRNAs are a hallmark of developmental and disease-associated loci, yet they remain poorly understood. This study uncovers the regulatory dynamics of such a region through real-time visualization of ncRNA transcription in living embryos. Single-cell quantification of transcriptional dynamics revealed unexpected insights into the mechanisms of gene regulation by ncRNAs.

We showed that the timing of Scr expression does not coincide with the activation of its distal enhancer and tethering element, but instead, their transcription exhibits a well-defined temporal launch sequence. This challenges the notion that enhancer activity directly determines gene activity. Rather, it appears that regulatory elements constitute a cis-network governing a multistep activation process. Transcriptomic studies of cellular differentiation have shown that enhancer transcription globally precedes transcription at gene promoters in mammalian cells (34).

A DTE transcription is under the control of the Early Enhancer & eRNA

B eRNA regulatory activity requires the DTE

C Micro-C analysis of eRNA TSS deletion

D Summary model

Fig. 4. Enhancer transcription controls tethering element transcription and long-range interactions. (A) Regulation of DTE transcription by the EE enhancer and eRNA. (Left) Deletions of the enhancer and the eRNA TSS. (Right) Live transcription measurements for the DTE-associated RNA (dtRNA), upon deletions of the enhancer and eRNA TSS. (B) Genetic interaction between the Scr eRNA and DTE. (Left) Deletions of the DTE and the eRNA TSS. (Right) Live transcription measurements for both deletions, separately and in combination. Disrupting both elements simultaneously causes embryonic lethality. (C) Micro-C analysis of the Scr locus upon deletion of the eRNA TSS. (Top) Micro-C contact map of eRNA TSS deletion mutant in early embryos (NC14). (Inset) Micro-C contact map for stage-matched wild-type embryos (see Fig. 1D). (Bottom) Virtual 4C (circular chromosomal conformation capture) quantification of the spectrum of interactions of the Scr promoter (anchor) across the Scr TAD, in wild-type and eRNA TSS deletion mutant embryos. (D) Proposed model. At early developmental stages, high enhancer activity drives intense eRNA production. eRNAs in turn (i) inhibit the formation of long-range regulatory loops and (ii) inhibit enhancer activity, potentially through disruption of transcription condensates. As enhancer activity progressively diminishes, eRNA-mediated repression is relieved—leading to precise timing of gene activation.

Our work demonstrates that enhancer transcription can delay gene expression to achieve precise timing of activation. Taken together, these observations provide evidence for a role of ncRNAs in the temporal control of gene activity and suggest that enhancer transcription may be broadly deployed to control the dynamics of gene activity during development. Our study also suggests that cis-regulatory ncRNAs influence a range of regulatory outcomes, including the timing of activation (Scr eRNA), levels of expression (Scr dtRNA), and spatial patterning (Antp P2).

The precise control of Scr temporal dynamics does not solely depend on the process of transcriptional initiation or elongation at the enhancer but also requires full-length eRNA products that function strictly in cis. These eRNAs have two regulatory effects (Fig. 4D): inhibition of enhancer activity (fig. S5) and disruption of long-range regulatory loops (Fig. 4C). Although this process is highly dependent on transcript length, it does not hinge on specific RNA sequences (Fig. 3C). At the molecular level, different mechanisms can be envisioned, but we consider mainly two nonexclusive possibilities. One is that high eRNA concentrations disrupt transcription condensates (25, 35–40), which may account for the nonmonotonic relationship between enhancer and gene activities observed at the single-cell level (40) (Fig. 2). Another possibility is that eRNAs interact with transcriptional coactivators (and DNA looping factors) to disrupt their association with chromatin or tune their regulatory activities (15, 23). Additionally, sequestration of Pol II or other rate-limiting factors to the eRNA promoter may also dampen gene activation. We propose that cis-regulatory ncRNAs, through these or other mechanisms, co-transcriptionally modulate the activity of underlying DNA elements to quantitatively control the timing of gene expression.

Our findings resonate with a recent study describing gene repression by synthetic transcripts with strong dependencies on transcription rate and transcript length in mouse embryonic stem cells (41). That study likewise supports an RNA-dependent mechanism, as opposed to a simple promoter competition model, and highlights the relevance of our work to gene regulation in vertebrates. Notably, the Scr eRNA is a highly directional \~7.4-kb spliced long noncoding RNA (lncRNA). Splicing has been suggested to modulate lncRNA chromatin release and enhancer activity (42), raising the possibility that the absence of introns in the $\lambda$ ncRNA might increase retention of nascent transcripts and further delay the onset of Scr expression.

We also provided evidence for a crucial interplay between cis-regulatory ncRNAs and genome organization. Although previous studies have shown that ncRNAs can influence genome organization (43–45), our work reveals how this may be deployed to regulate the temporal dynamics of gene activity in development. The strong genetic interaction observed between a ncRNA and a neighboring architectural element—and associated embryonic lethality—demonstrates that even ncRNAs with no overt knockout phenotypes (26) may in fact serve critical biological functions, with major implications for our understanding of the genetic architecture of complex diseases. In light of the prevalence of ncRNAs in the human genome (15), these insights suggest that noncoding transcription may be central to long-range gene regulation and to the quantitative control of gene activity in space and time.

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ACKNOWLEDGMENTS

The authors thank M. Levo for countless discussions and insights throughout this project; X. Bing, X. Li, N. Treen, all members of the Levine lab, and J. Batut for many helpful discussions and suggestions; W. Ke and P. Schedl for their precious help with micro-C analysis; L. Mahal, E. Meagher, and other members of the Batut lab for help testing and validating fly lines, as well as discussions and suggestions; the Levo lab for the use of its microscope; and E. Gatzogiannis for technical advice regarding microscopy. We also thank the Princeton Genomics Core Facility for high-throughput sequencing services, as well as the Lewis-Sigler Institute's genomics computing group and the Columbia Systems Biology C2B2 computing group for help with high-performance computing resources. Funding: This work was supported by NIH grant R35 GM118147 (M.S.L.) and NIH grant R35 GM162470 (P.J.B.). Author contributions: Conceptualization: P.J.B., M.L.; Formal analysis: P.J.B., M.L.; Funding acquisition: M.L.; Investigation: P.J.B.; Methodology: P.J.B.; Project administration: M.L.; Resources: P.J.B., M.L.; Software: P.J.B.; Supervision: M.L.; Validation: P.J.B., M.L.; Visualization: P.J.B., M.L.; Writing – original draft: P.J.B., M.L.; Writing – review & editing: P.J.B., M.L. Competing interests: The authors declare that they have no competing interests. Data, code, and materials availability: Source data for MS2/PP7 transcription imaging analyses are available through Zenodo (46). Raw and processed Micro-C data are available through Gene Expression Omnibus (GEO) with accession nos. GSE343884 (Scr-MS2 and Scr-MS2,eRNAΔTSS embryos) and GSE171396 (yw embryos; data published previously). Raw sex comb counts are available through Zenodo (47). Custom data analysis code for the primary processing and integrative analysis of MS2/PP7 data was published previously and is available through Zenodo (47). All DNA constructs and fly lines included in this study are available upon request from P.J.B. License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.aek5696

Materials and Methods; Figs. S1 to S14; Tables S1 and S2; References (48–58);

Movies S1 to S4; MDAR Reproducibility Checklist

Submitted 14 July 2026; accepted 25 August 2026; published online 10 September 2026

CONSERVATION BIOLOGY

Safeguarding global terrestrial vertebrate species from future sea level rise

Zhong-Wen Jiang $^{1\dagger}$ , Heng-Bin Xiao $^{1\dagger}$ , Jeffrey O. Hanson $^{2}$ , Yiwen Zeng $^{3}$ , David S. Wilcove $^{4}$ , Mark Schuerch $^{5,6}$ , Matthew L. Kirwan $^{7}$ , Qin-Fang Yan $^{1}$ , Yaping Chen $^{1*}$ , Liang Ma $^{1*}$

Sea level rise (SLR) threatens terrestrial biodiversity, yet its spatiotemporal and species-specific impacts remain unclear. Integrating relative SLR projections across five shared socioeconomic pathways (SSPs) with area of habitat (AOH) maps for 34,120 terrestrial vertebrate species, we project that species exposed to SLR will increase from up to 13,680 in 2050 to 15,324 by 2100, including 57 to 63% of birds, 47 to 52% of mammals, 28 to 36% of reptiles, and 20 to 24% of amphibians. In Southeast Asia, inland inundation areas support high richness. Under SSP5-8.5, species facing >10% habitat inundation surge from 18 in 2050 to 109 by 2100, with reptiles and already threatened species overrepresented. Safeguarding SLR refugia—the noninundated habitats for exposed species—is critical, yet more than 96% lie outside protected areas, which means that early international action is required.

Terrestrial vertebrate species face multifaceted threats from climate change, including rising temperatures (1, 2), extreme heat events (3, 4), and prolonged droughts (5, 6). Among these threats, sea level rise (SLR) represents an underappreciated hazard that can cause irreversible habitat loss (7, 8). SLR has already led to population collapses and extinctions by inundating or degrading critical habitats (9–11). The Bramble Cay melomys (Melomys rubicola) was declared extinct, with SLR identified as the root cause (11). SLR has also driven population declines through tidal nest flooding, as documented for shorebird species and the saltmarsh sparrow (Ammospiza caudacuta) (10, 12). With global SLR rates at record-high levels (>4 mm year $^{-1}$ ) and likely increasing beyond 10 mm year $^{-1}$ in coming decades (7), rising seas may soon force more species declines and extinctions. Therefore, a systematic assessment of SLR impacts to guide conservation action is urgently needed.

Understanding SLR impacts on biodiversity requires timely and spatially explicit information (13–15). Because SLR exhibits substantial spatial and temporal variability (16, 17), nuanced projections of when and where inundation may occur are critical for assessments. This is challenging because the inundation at a specific location is influenced by local-scale factors, such as vertical land movements (land subsidence or uplift) (18) and dynamic variations in regional sea levels (e.g., owing to uneven thermal expansion and contraction) (19). Species-level habitat data, including elevational ranges and habitat preferences, can refine broad geographic distributions into more precise estimates of habitat exposure (20), enabling conservation actions that are tailored to species-specific risks. Finally, identification of SLR refugia—defined as noninundated habitats capable of supporting affected species—may offer an underused strategy to buffer biodiversity loss (21, 22).

In this work, we provide a global, species-specific assessment of SLR impacts on terrestrial vertebrate species and explore conservation avenues. We leverage the area of habitat (AOH) approach to characterize the distribution of 34,120 terrestrial vertebrates ( $\sim90\%$ of all known terrestrial vertebrates) by integrating their ecological requirements with topographic constraints (20). Species recognized by the International Union for Conservation of Nature (IUCN) Red List of Threatened Species as Critically Endangered, Endangered, and Vulnerable were classified as threatened. We exclude species that are Extinct, Extinct in the Wild, or whose habitats are entirely artificial or marine according to the IUCN Habitats Classification Scheme (version 3.1; habitat types 9 to 15) (23). For species inhabiting both terrestrial and nonterrestrial habitats, only terrestrial portions were considered. Although all AOH maps were initially generated at 100-m-by-100-m resolution, we aggregated maps for 32,919 species with $AOH > 2 km^{2}$ to 1-km-by-1-km resolution for computational feasibility, following recommended practices (24–26). By overlapping AOH maps with inundation areas derived from high-precision relative SLR projections—harmonized to each species' spatial resolution and accounting for region-specific vertical land movements—we identified regions and species at greatest risk by 2050 and 2100 under five shared socioeconomic pathways (SSPs). These scenarios range from low to high warming: SSP1-1.9 (+1.4°C by 2100 relative to preindustrial levels), SSP1-2.6 (+1.8°C), SSP2-4.5 (+2.7°C), SSP3-7.0 (+3.6°C), and SSP5-8.5 (+4.4°C) (26, 27). Species-specific vulnerability was quantified using the proportion of habitat inundated at each species' native resolution, whereas richness-based analyses were conducted on 1-km-by-1-km grids (26). Finally, we map SLR refugia within species' noninundated habitats. Although previous works have examined how shifting climatic conditions alter species' habitat availability (3, 6, 28), our study highlights direct SLR inundation as another pathway through which climate change threatens terrestrial vertebrates.

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Geographic patterns in terrestrial vertebrate diversity affected by SLR

Integrating sea level projections from the Intergovernmental Panel on Climate Change Sixth Assessment Report (16, 29) with observation-based, spatially explicit vertical land motion (uplift or subsidence) data (30, 31), our analyses indicate that relative sea levels along global coasts may rise by up to 0.57 m by 2050 and 1.33 m by 2100 under SSP2-4.5. Using tidal regimes for 12,148 global coastline segments (17), we translated the magnitude of relative SLR into inundation area. The Amazon River delta is expected to undergo the greatest habitat loss for terrestrial vertebrates, with $>1000 \, km^2$ of inland area inundated by 2050 (fig. S1). As SLR accelerates, area-loss hotspots spread from the Amazon River delta to parts of Asia, Europe, and North America.

To map geographic patterns of SLR impacts on terrestrial vertebrates, we used three metrics: total species richness, threatened species richness, and rarity-weighted richness. The first two metrics, respectively, capture the number of species and the number of threatened species in each inundated pixel, whereas rarity-weighted richness—calculated by summing the inverse of each species' AOH—quantifies each pixel's relative importance to species. The Amazon River delta emerges as the region with the highest affected species richness across all SSPs and times (Fig. 1, A and B). This pattern reflects extensive SLR-induced area loss in the Amazon basin, a global biodiversity hub (32). The coasts of Southeast Asia, Central America, and Southeastern Africa also score high in affected species richness, reflecting their status as global biodiversity hotspots (33, 34).

SLR disproportionately affects terrestrial vertebrates in island-rich regions (Fig. 1, C and D), where species generally have small geographic ranges (35). Islands host many endemic species (13, 33), and their coastline-to-interior ratio exposes a greater share of inland areas to rising tides. Consequently, even minor habitat loss from modest SLR can increase the extinction risk of island-dwelling species. Inundation areas with the highest rarity-weighted richness are concentrated in Southeast Asia, the Ryukyu Islands, and the Caribbean Islands (Fig. 1, C and D), which supports predictions that island species will be among the first to bear the brunt of SLR (7, 13, 15, 36). Contrary to previous work (14), although the Amazon River delta supports extremely high species richness and is predicted to lose vast inland areas to SLR, it does not rank among the most affected regions for range-restricted endemics, as indicated by its modest rarity-weighted richness (Fig. 1, C and D).

Fig. 1. Spatial patterns of SLR impacts on terrestrial vertebrate species under SSP2-4.5. (A and B) Species richness (defined as the number of species present in a given area) exposed to SLR by 2050 (A) and by 2100 (B). (C and D) Rarity-weighted richness exposed to SLR by 2050 (C) and by 2100 (D). This metric represents the cumulative importance of an area to all species that it supports, calculated as the sum of the reciprocals of total habitat of all species found in the area. (E and F) Threatened species richness by 2050 (E) and by 2100 (F) under predicted SLR. This metric indicates the number of species in a given area of inundation that are currently classified as threatened according to the IUCN threat status. Species exposed to SLR are defined as those with at least $1\mathrm{km}^2$ of habitat inundated or $\geq 0.01\mathrm{km}^2$ for species with total $\mathrm{AOH} \leq 2\mathrm{km}^2$ . This figure displays results for the medium SLR scenario (SSP2-4.5). The results for other SSPs and taxon-specific patterns are presented in figs. S10 to S33. Results retain their original 1-km-by-1-km resolution, although plotted points are enlarged for global visibility without altering geographic coordinates.

Southeast Asia and surrounding islands emerge as a region of concern across all three metrics (Fig. 1), with inundated areas harboring high numbers of threatened species (Fig. 1, E and F). Under SSP2-4.5, inundated pixels in the Malay Peninsula, Borneo, and Sumatra support, on average, nearly three times as many threatened species as those in the rest of the world, with the ratio increasing from 2.82 in 2050 to 2.87 by 2100 ( $W = 583,049,309$ , $P < 0.001$ ; see taxon-specific patterns in supplementary text 1.1). Therefore, although projected inundation in Southeast Asia is smaller than that in the Amazon River delta and southern North America (fig. S1), its exceptional biodiversity, including many range-restricted and threatened species, makes it highly vulnerable to SLR (Fig. 1, C to F). Some regions identified in this work as highly vulnerable to SLR, such as Borneo and the Philippine archipelago, were underestimated by using species-area relationships (15).

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Species-specific exposure and vulnerability to SLR

We assessed species-specific exposure and vulnerability to SLR across four terrestrial vertebrate groups and six IUCN threat statuses: Critically Endangered, Endangered, Vulnerable, Near Threatened, Least Concern, and Data Deficient. We first used absolute habitat loss thresholds to identify species exposed to SLR: $\geq1~km^{2}$ of AOH inundated or $\geq0.01~km^{2}$ for species with total AOH of $\leq2~km^{2}$ . We did so because small habitat fragments often contribute disproportionately to species and genetic diversity (37), and many species depend on small habitats vulnerable to SLR (10) during key life stages (38). Species-specific vulnerability was then quantified as the proportion of each species' AOH inundated. Absolute thresholds prevent large range sizes from mathematically diluting habitat loss in widespread species (39), and proportional inundation standardizes vulnerability (40).

Under the intermediate SSP2-4.5 scenario, 13,511 terrestrial vertebrate species are exposed to SLR by 2050 and 14,831 by 2100 (Fig. 2). Across all SSPs, exposed species range from 13,308 to 13,680 by 2050 and from 14,325 to 15,324 by 2100. These include 20 to 24% of amphibians (1540 to 1587 by 2050; 1683 to 1844 by 2100), 28 to 36% of reptiles (2779 to 2900 by 2050; 3129 to 3551 by 2100), 57 to 63% of birds (6225 to 6356 by 2050; 6559 to 6835 by 2100), and 47 to 52% of mammals (2764 to 2837 by 2050; 2954 to 3094 by 2100). Although SLR is predicted to affect a greater proportion of birds and mammals than of amphibians or reptiles, species affected in the latter two groups, particularly reptiles, will experience nearly twice the average proportional habitat loss compared with birds and mammals (Fig. 2 and fig. S2).

Species losing a substantial proportion of their habitat to SLR may require conservation intervention. To identify such species, we applied a 10% habitat loss threshold because such habitat losses may be associated with reductions in genetic diversity that can take thousands of years to recover (41). Under SSP5-8.5, 18 species

are projected to lose $>10\%$ of their AOH by 2050, increasing to 109 by 2100, including 13 amphibians, 58 reptiles, 27 birds, and 11 mammals. Of these, 32 species are predicted to lose $>20\%$ of their AOH (fig. S2 and table S1). The worm lizard (Amphisbaena littoralis), Catalina chuckwalla (Sauromalus klauberi), and Restinga toadlet (Melanophryniscus setiba) are projected to lose $\sim50\%$ of their habitats by 2100 under SSP5-8.5 (table S1). Although birds show lower total habitat loss to SLR, key vulnerability emerges for migratory species when breeding, nonbreeding, and resident habitats are analyzed separately. For example, although total habitat inundation for the ferruginous duck (Aythya nyroca) remains $<1\%$ under SSP5-8.5, the proportion of its resident habitat inundated increases from 17% in 2050 to 38% by 2100 under SSP2-4.5 (table S1).

Terrestrial vertebrate species recognized as threatened by IUCN are likely to be disproportionately affected by SLR, with their average proportion of habitat loss estimated to be five times as great as that of Least Concern species, ranging from 2 to 10 times as great across SLR scenarios (W = 534,132,782, P < 0.001). This is consistent with losses predicted for island-restricted species (15), which suggests that the disproportionate vulnerability of threatened species to SLR is not confined to island ecosystems but occurs globally across terrestrial vertebrates.

Fig. 2. Species-specific vulnerability to SLR impacts under SSP2-4.5. (A and B) The distributions of the proportion ( $P_{\text{inundated}}$ ) of each species' AOH inundated by SLR are shown for the four terrestrial vertebrate groups (A) and six IUCN threat statuses (B) according to SLR by 2050 (left column) and by 2100 (right column). The four groups of terrestrial vertebrate species presented from top to bottom in (A) correspond to amphibian, reptile, bird, and mammal. Similarly, the six IUCN threat statuses shown from top to bottom in (B) refer to Critically Endangered (CR), Endangered (EN), Vulnerable (VU), Near Threatened (NT), Least Concern (LC), and Data Deficient (DD). The dashed red line marks where 1% of the habitat is inundated, the mean represents the estimated mean proportion of habitat inundated ( $P_{\text{inundated}}$ ) of the group, and $n$ denotes the number of species in the group. Species with $P_{\text{inundated}} > 1\%$ were included in the refugia analysis. The results for other SSPs are presented in figs. S34 to S37. Note that the $x$ axis is $\log_{10}$ -transformed to accommodate the highly skewed data distribution, and the axis tick labels display untransformed proportion values to aid interpretation. Animal silhouette images were sourced from PhyloPic (https://www.phylopic.org/).

Habitat inundation was negatively correlated with total AOH, indicating greater proportional loss in narrow-ranged species. This relationship is particularly strong for reptiles and species classified as Data Deficient, Endangered, or Critically Endangered (figs. S3 and S4).

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SLR refugia

As sea level rises, species affected by inundation are expected to retreat to their remaining noninundated habitats (42, 43). We identified SLR refugia within the noninundated AOH of species projected to lose $>1\%$ of their AOH to SLR (hereafter referred to as affected species), a threshold widely adopted in conservation frameworks (26, 44, 45). SLR refugia were defined as the top 10% of noninundated pixels, consistent with the 10% threshold commonly used to define refugia (45, 46), ranked using three complementary metrics (26): the total number of affected species supported, the number of affected threatened species supported, and the summed proportion of habitat inundated across supported species (fig. S5). The third metric highlights noninundated pixels supporting species with greater habitat loss from SLR.

Only 0.5% of SLR refugia that we identified for 2050 fall within existing protected areas (table S2). Although countries have pledged to protect 30% of land areas by 2030 under target 3 of the Kunming-Montreal Global Biodiversity Framework (GBF) (47), substantial progress is needed (48). Protected area coverage of refugia is also low across most countries. Under SSP2-4.5, Myanmar, Fiji, Madagascar, and Brazil each have <1% coverage of SLR refugia. Conversely, New Zealand, Cuba,

Japan, and Spain have $>30\%$ coverage across almost all SLR scenarios. Comparing current national protected area coverage with the proportion of unprotected refugia at the country level (fig. S6) (26), our analysis reveals that countries such as Myanmar, Vietnam, and Indonesia could simultaneously protect biodiversity from SLR and move toward 30% protected area coverage by increasing protection of SLR refugia (fig. S6).

Projected SLR refugia exhibit dynamic spatial patterns over time. Because SLR refugia are defined on the basis of species' remaining noninundated habitats, initially identified refugia may expand and new refugia may emerge as SLR affects more species. Under SSP2-4.5, only Myanmar and Australia host SLR refugia by 2050, with this number increasing to 26 countries by 2100 (Fig. 3A, dark red, and fig. S7). Geographic patterns of refugia vary across the four taxonomic groups, with detailed analyses provided in supplementary text 1.2. Country rankings based on total SLR refugia area are relatively consistent across low to moderate SLR scenarios (SSP1-1.9 and SSP1-2.6) but differ under more severe scenarios (SSP2-4.5 to SSP5-8.5). For instance, China is projected to contain a relatively small area of SLR refugia by 2100 under low to moderate scenarios, yet it ranks among countries with the greatest refugia areas under worst-case scenarios (SSP3-7.0 and SSP5-8.5; fig. S7). These time- and scenario-specific projections can guide protected area expansion and land use planning through a staged refugia strategy—preferentially protecting refugia emerging by 2050 while developing plans and allocating resources to areas that progressively gain importance as SLR intensifies.

Fig. 3. Spatial patterns of global SLR refugia under SSP2-4.5. (A and B) The dark red color indicates the location of SLR refugia identified around the globe by predicted SLR by 2050 (A) and by 2100 (B). SLR refugia refer to the noninundated areas, which rank simultaneously among the top 10% in three metrics: the summed proportion of habitat inundated across supported species (denoted as P), the number of affected threatened species supported (T), and the total number of affected species supported (R). The analysis is performed for all species with at least 1% of AOH lost to SLR. The results for other SSPs and taxon-specific patterns are presented in figs. S37 to S61.

Many SLR refugia, including those in Southeast Asia and central-western South America, are spatially congruent with recognized global biodiversity hotspots (34, 49) and terrestrial conservation priority areas (50), but many occur outside these areas. For instance, eastern coastal China and Russia's northern coastlines have largely been overlooked as conservation priorities, yet they are predicted to harbor SLR refugia that expand under severe SLR scenarios (Fig. 3 and fig. S7). Similarly, although Thailand is projected to host extensive SLR refugia (Fig. 3) that overlap biodiversity hotspots (34, 49), its designated conservation priority remains low (50). Together, these findings highlight the potential of safeguarding SLR refugia to achieve GBF targets while revealing mismatches between conventional conservation prioritization and emerging climate-driven vulnerability.

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Implications

Our findings offer insights into the multidimensional impacts of climate change on global biodiversity and highlight locations for targeted conservation. By 2100, $\sim 45\%$ of all species studied may be affected by SLR, yet only $5.9\%$ of affected species are flagged for climate-relevant threats in the IUCN Red List (supplementary text 1.3). These findings have implications for helping countries meet the Kunming-Montreal GBF targets. First, SLR refugia have low protected area coverage in most countries, which suggests that protected area expansion under target 3 should improve coverage of SLR refugia. Second, integrated planning under target 1 should account for SLR impacts to avoid losing areas that will become increasingly important for biodiversity. Third, for species projected to lose most of their habitat to SLR, strategic habitat restoration and ex situ conservation will likely be necessary to prevent extinctions under target 4, as demonstrated by previous recovery efforts (51-54). Overall, minimizing impacts and building resilience to SLR under target 8—alongside other climate change impacts—will be crucial for achieving multiple policy targets under the GBF (47).

SLR impacts are highly heterogeneous across space and among species. Terrestrial vertebrates in regions threatened by SLR—such as the Amazon, where frogs also face increasing dryness (6); island systems such as the Caribbean; and the southern United States—are also expected to experience increased exposure to overheating (3, 28). Among taxa, reptiles may be especially vulnerable to changing climates, as shown by the SLR-induced habitat loss identified in this and in previous island-focused work (13), and their high exposure to extreme heat events (3). Compared with prior estimates (15), our assessment suggests that fewer species may lose their entire habitat to SLR by 2100. For example, under SSP5-8.5, only three species are projected to lose about half of their habitats, whereas 37 species were predicted to lose all their habitats under a global uniform 1-m SLR scenario, with extinctions inferred from a generalized area loss-species loss proportionality assumption (15). This difference arises partly because our study accounts for spatially dynamic variation of SLR. Even under SSP5-8.5, the projected global mean relative SLR by 2100 is $0.80 \pm 0.22$ m, although local values may reach $1.54$ m. Additionally, we directly estimate species-specific habitat exposure by intersecting projected inundation areas with individual AOH maps. Although few species are likely to lose all their habitats to SLR, many species may lose enough habitat to affect their long-term persistence.

Integrating high-precision relative SLR projections with species-specific AOH data provides finer-grained insights into biodiversity risk assessment and conservation planning. However, fine-scale species-level analyses remain limited by uncertainties in underlying data products. For instance, the digital elevation model used to assess inundation area was produced a decade ago (55). Although it offers reliable, globally consistent topography with low vertical uncertainty, a single terrain snapshot cannot reflect the ever-changing nature of coastal landscapes. Another limitation is that we assess range-wide species-level impacts, whereas much conservation planning occurs at national scales or focuses on subspecies and populations (56–58). For example, although the tiger (Panthera tigris) appears minimally affected by SLR at the species level, with $<0.05\%$ of its habitat inundated, the Bengal subspecies (P. t. tigris) is projected to lose nearly half of its habitat within a few decades (59). We excluded fully marine species and considered only terrestrial habitat components captured by AOH maps for coastal-dependent species. Yet many, including migratory shorebirds in the families Scolopacidae and Charadriidae, rely on intertidal zones for foraging and breeding (10, 60, 61); therefore, their full SLR exposure is not captured in this work. Additionally, our study focuses only on progressive SLR and does not account for increasing salt spray (62), amplified storm surges (63, 64), and intensifying hurricanes (64), which can carry salt water further inland and degrade terrestrial vertebrate habitats before regular tidal inundation. Thus, our study represents a conservative estimate of SLR impact on terrestrial vertebrates.

Early, coordinated international action is needed to reduce SLR impacts on biodiversity. This is especially pertinent for low- and middle-income countries, where limited financial capacity and pressing development needs make delayed conservation increasingly costly (21, 22, 52, 65–68). Because many countries may have limited financial capacity to conserve SLR refugia (supplementary text 1.4), international policies providing funding and technical assistance could aid in conserving SLR refugia. Such efforts should account for disparities in national wealth and local sociocultural contexts (69). Although coastal flood-defense barriers are important for protecting human development (70), they are unlikely to fully mitigate

Biodiversity Framework" (United Nations Environment Programme, Report CBD/COP/DEC/15/4, 2022); https://www.cbd.int/doc/decisions/cop-15/cop-15-dec-04-en.pdf.

SLR impacts on terrestrial vertebrates. Our sensitivity analysis suggests that these barriers can reduce projected exposure for some inland species, but their effects vary spatially, diminish over time (supplementary text 1.5 and figs. S8 and S9), and may exacerbate coastal squeeze or disrupt ecological connectivity (17, 71, 72). Consequently, SLR refugia will likely play an important role in supporting SLR-affected species throughout the 21st century. Because many refugia fall outside biodiversity hotspots (34) or conservation priorities (50, 73), they may be overlooked in conservation planning. Systematic conservation planning can build on our findings to identify priority areas for protecting SLR refugia while accounting for habitat dynamics and uncertainty across SLR scenarios (74). Our findings underscore the importance of protecting SLR refugia to build resilience under GBF target 8 while safeguarding biodiversity, thereby helping achieve broader biodiversity targets.

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ACKNOWLEDGMENTS

We thank C. Mi for his comments and R. Liu for her assistance with data preparation. Funding: This study was supported by Fundamental and Interdisciplinary Disciplines Breakthrough Plan of the Ministry of Education of China JYB2025XDXM902 (Z.-W.J., L.M., Y.C., and H.-B.X.); National Natural Science Foundation of China 32330067 (Z.-W.J. and L.M.); National Natural Science Foundation of China 32501390 (Z.-W.J.); National Natural Science Foundation of China 32570593 (L.M.); Fundamental Research Funds for the Central Universities, Sun Yat-sen University 24hytd014 (L.M.); National Natural Science Foundation of China 42501094 (Y.C.); Fundamental Research Funds for the Central Universities, Sun Yat-sen University 24hytd012-2 (Y.C.); Natural Sciences and Engineering Research Council (NSERC) (J.O.H.); and Environment and Climate Change Canada (ECCC) (J.O.H.). Author contributions: Conceptualization: Z.-W.J., L.M., H.-B.X., Y.C.; Data curation: Z.-W.J., J.O.H., M.S.; Funding acquisition: L.M., Y.C., Z.-W.J., H.-B.X.; Investigation: Z.-W.J., L.M., H.-B.X., Y.C., Q.-F.Y.; Methodology: Z.-W.J., L.M., H.-B.X., Y.C., J.O.H., Y.Z.; Project administration: Z.-W.J., L.M., Y.C.; Supervision: L.M., Y.C.; Visualization: Z.-W.J., H.-B.X.; Writing – original draft: Z.-W.J., L.M., H.-B.X., Y.C.; Writing – review & editing: Z.-W.J., L.M., H.-B.X., Y.C., J.O.H., Y.Z., D.S.W., M.S., M.L.K., Q.-F.Y. Competing interests: The authors declare no competing interests. Data, code, and materials availability: Global sea level projections to 2100 were obtained from Zenodo (https://zenodo.org/records/6382554) (29). The digital elevation model was derived from the NASA Shuttle Radar Topographic Mission (SRTM) dataset (https://srtm.csi.cgiar.org) (55). AOH maps for mammals and birds are available on Dryad (https://datadryad.org/dataset/doi:10.5061/dryad.02v6wwq48) (75), and those for amphibians and reptiles were generated using the "aoh" R package (76) based on distribution range data from the IUCN Red List (https://www.iucnredlist.org/resources/spatial-data-download) (23). All data and code generated in this paper are available on Dryad (77). No new materials were created in this study. License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.aed5772

Materials and Methods; Supplementary Text; Figs. S1 to S62; Tables S1 and S2;

References (78–111); MDAR Reproducibility Checklist

Submitted 2 November 2025; resubmitted 21 March 2026; accepted 26 August 2026; published online 8 October 2026

NATURAL PRODUCTS

Natural product biosynthesis by guanidine prenyltransferases in plants and bacteria

Dominik Kolling $^{1,2}$ , Katharina Konzok $^{3}$ , Daghan Taser $^{4}$ , Tom Jentsch $^{4}$ , Svenja Schwoerer $^{4}$ , Henry Struwe $^{4}$ , Arne Bültemeier $^{5,6}$ , Jonas Freiberg $^{7}$ , Claus-Peter Witte $^{7}$ , Jakob Franke $^{5,6}$ , Andriy Luzhetskyy $^{2,8}$ , Andreas Kirschning $^{4,9}$ , Sophia Rudorf $^{3*}$ , Jesko Koehnke $^{1*}$

Guanidine exists almost exclusively as a resonance-stabilized cation, making its direct enzymatic functionalization challenging. We identified the cyanobacterial enzyme NosH, which catalyzes direct prenyl transfer to free guanidine. Structural and mechanistic analyses revealed guanidine activation by a two-aspartate clamp coupled to prenyl-donor binding through a distinct catalytic architecture. Guided by these features, we identified a large family of guanidine prenyltransferases across bacteria and plants. Plant enzymes produced guanidine alkaloids such as galegine in vitro and heterologous expression of a plant ortholog in Nicotiana benthamiana produced galegine in planta, providing a direct enzymatic link to plant-specialized metabolism.

Under physiological conditions, guanidine (Gua, 1) is one of the strongest naturally occurring bases, existing almost exclusively as a mesomerically stabilized cation. Guanidine is a biologically important metabolite across diverse branches of life (1). Organic guanidine derivatives are central to drugs for cardiovascular disease, infections, and type II diabetes (2–7). Guanidine occurs in mammalian urine, and bacteria—including cyanobacteria—use free guanidine as a nitrogen source (8–11).

In specialized metabolism, primary metabolites are repurposed to construct complex natural products. Plants, in particular, produce guanidine-containing alkaloids such as galegine (2) (12–14), which inspired the development of metformin (3), the most prescribed antidiabetic drug worldwide (Fig. 1A) (15, 16). However, despite more than a century of pharmacological relevance, the biosynthetic origin of guanidine incorporation in galegine and the plant metabolites pterogynine (4) and nitensidine (5) has remained enigmatic.

Guanidine-derived natural products are also found in bacteria, including gromomycin (6), cybastacine (7), and zillamycin (8) (Fig. 1A and fig. S1) (17–20). In the biosynthesis of well-studied toxins such as saxitoxin (S48) and stylissadine (S49), amidinotransferases degrade arginine and transfer only a fragment of its guanidino group (21–24). In natural products such as autumnalamide A (S63) or argicyclamide A (S64), ABBA-fold prenyltransferases append isoprenoid chains to the guanidino groups of arginine or agmatine, tuning solubility, stability, and bioactivity (fig. S1) (25–27). However, these known guanidine prenyltransferases act on guanidino groups embedded within larger natural-product scaffolds. Direct prenyl transfer to free guanidine has not been demonstrated, and no mechanism has been established for the enzymatic functionalization of free guanidine beyond its degradation.

Here, we identify and characterize NosH, a cyanobacterial guanidine prenyltransferase that catalyzes the direct prenylation of free guanidine. Structural analysis reveals a distinct active-site architecture that activates guanidine and accommodates diverse prenyl donors through a hydrophobic trench. Guided by these structural features rather than sequence identity alone, we uncover a large family of guanidine prenyltransferases across plants and bacteria and demonstrate the ability of selected plant enzymes to produce galegine in vitro and in planta.

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NosH catalyzes direct prenylation of free guanidine

The recent discovery of a family of guanidine-containing secondary metabolites called gromomycins revealed biosynthetic machineries that operate independently of amidinotransferases (fig. S2 and table S1) (17). Analysis of the corresponding biosynthetic gene cluster (BGC) suggested that the encoded enzyme GroH catalyzes the formation of the gromomycin intermediate hexaprenyl/C $_{30}$ -guanidine (zillamycin; 8) from arginine and the prenyl-donor hexaprenyl diphosphate (HePP; S6) through an unusual reaction mechanism involving arginine modification and subsequent cyclization. However, GroH activity was inferred from metabolomics data and has not been demonstrated by in vitro biochemical reconstitution, in part because biochemical characterization was limited by poor enzyme solubility.

To overcome these limitations, we identified a cyanobacterial ortholog, NosH, encoded in a related putative terpene BCG from Nostoc flagelliforme CCNUN1 (Fig. 1B, fig. S3, and tables S2 and S3). Recombinantly expressed NosH showed only trace conversion of FPP (9) with L-arginine (Arg, 10) or agmatine (Agm, 11) into C $_{15}$ -prenylated derivatives (12 and 13), prompting us to consider whether free guanidine might serve as a substrate (fig. S4). This hypothesis was supported by the presence of genes associated with guanidine metabolism in the vicinity of the NosH-associated BGC and by the recent demonstration of a guanidine-specific riboswitch-controlled catabolic pathway in N. flagelliforme CCNUN1 (fig. S5 and table S4) (11).

NosH catalyzed a $Mg^{2+}$ -dependent reaction between free guanidine and FPP (9), yielding farnesyl guanidine (14, $[M+H]^{+}_{obs.}=264.2427$ Da, $[M+H]^{+}_{calc.}=264.2434$ Da, $\Delta ppm-2.65$ ), which was further confirmed by nuclear magnetic resonance (NMR) analysis (Fig. 1C, figs. S6 to S10, and table S5). Time-course experiments under initial-rate conditions, using purified 14 as an external standard for quantification yielded a $K_{M}$ for guanidine of $1.00\pm0.39$ mM and a $k_{cat}$ of $2.59\pm0.18$ min $^{-1}$ (Fig. 1D and fig. S11).

We next examined the prenyl-donor scope of NosH using isoprenoid diphosphates of increasing chain length: isopentenyl diphosphate (IPP; S1), dimethylallyl diphosphate (DMAPP; S2), geranyl diphosphate (GPP; S3), geranylgeranyl diphosphate (GGPP; S4), pentaprenyl diphosphate (PePP; S5), and HePP (S6). NosH required a minimum donor chain length of $C_{10}$ and accepted donors up to at least $C_{30}$ , yielding the corresponding guanidinylated polyprenyls 15-17 and zillamycin (8) (Fig. 1E and figs. S12 to S15). This broad donor tolerance distinguishes NosH from canonical ABBA-fold prenyltransferases, which are limited to short-chain donors ( $C_{5}$ to $C_{10}$ ) (28). NosH-like proteins have been proposed in silico to participate in guanidino-group modification pathways (20), and the cyanobacterial ortholog ScAer3 transfers DMAPP to the guanidino-group of agmatine (11), but activity on free guanidine was not reported (29).

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Structural basis of free guanidine prenylation by NosH

To define the structural basis of guanidine prenylation, we determined apo and ligand-bound NosH structures (figs. S16 to S22 and table S6). NosH forms a homodimeric $\alpha4-\alpha4$ barrel that is structurally related to class I terpene synthases and distinct from ABBA-fold prenyltransferases (30, 31). Unlike canonical class I enzymes, NosH contains an inverted DDxxD motif (residues 176 to 183, NDFIDYADD) that coordinates $Mg^{2+}$ and the prenyl diphosphate in a distinct geometry. The active site combines a two-aspartate guanidine-binding clamp (Asp140 and Asp172) with a hydrophobic tunnel that opens into a trench upon prenyl-donor binding, consistent with the broad $C_{10}$ to $C_{30}$ donor range observed biochemically.

A

B

C

D

E

Fig. 1. NosH catalyzes prenylation of free guanidine. (A) Representative bacterial and plant natural products containing prenylated guanidino groups and the natural-product-inspired synthetic drug metformin (3). (B) Biosynthetic gene clusters (BGCs) for gromomycin from Streptomyces sp. Je 1-332 and a related cluster from Nostoc flagelliforme CCNUN1 containing NosH. (C) Invitro reactions of NosH with farnesyl diphosphate (FPP; 9) and guanidine (1), L-arginine (Arg; 10), or agmatine (Agm; 11). Extracted ion chromatograms (EICs) show formation of farnesyl guanidine (14) and trace amounts of farnesyl L-Arg (12) and Agm (13). (D) Time course of guanidine prenylation with $1\mu \mathrm{M}$ or $0.1\mu \mathrm{M}$ NosH and Michaelis-Menten analysis with FPP and varying guanidine substrate concentrations. The data represent mean $\pm$ SD from independent biochemical reactions ( $n = 3$ ). (E) Prenyl-donor scope of NosH using isoprenoid diphosphates of different chain lengths. Donors from $\mathrm{C}_{10}$ to $\mathrm{C}_{30}$ were accepted, enabling in vitro reconstruction of zillamycin (8) biosynthesis. Parts of the figure were created using BioRender.

The 2.10-Å resolution ternary structure with guanidine, $Mg^{2+}$ , and the nonhydrolysable FPP analog farnesyl S-thiolodiphosphate [(FSPP)18] captures the reaction partners in the active site (Fig. 2, A and B, and figs. S23 and S24). Guanidine is anchored by Asp140 and Asp172, whereas the FSPP diphosphate is coordinated through $Mg^{2+}$ interactions with the inverted DDxxD motif, and its prenyl chain occupies the hydrophobic trench. Comparison with the apo and FSPP-bound structures shows that guanidine binding disrupts the Arg137-Asp176 salt bridge and repositions Arg137 toward the guanidine-binding site. In the ternary complex, Arg137 lies between guanidine and the FSPP C-1 carbon, which are separated by 4.7 Å. These structures define the substrate-binding geometry and identify the Asp140/Asp172 clamp and

Arg137 conformational switch as key features linking guanidine recognition to prenyl-donor positioning.

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NosH mechanism and substrate recognition

Guided by the structural data, we performed targeted mutagenesis to probe the catalytic mechanism of NosH (figs. S25 and S26). We first examined the guanidine-binding residues Asp140 and Asp172. The conservative Asp140Asn mutation reduced turnover by \~15% (all values in this section compare mutant activity with wild-type NosH), whereas Asp140Ala abolished activity. Since guanidine is a monovalent cation bound by two Asp residues, one Asp residue is expected to participate predominantly in hydrogen bonding, while the other forms a salt bridge; our data implicate Asp140 in the former role. Asp140 forms a hydrogen bond with Glu52, an interaction retained in the Asp140Asn variant that may contribute to its residual activity. Glu52 itself is dispensable, as Glu52Gln and Glu52Ala retained near-full activity (88% and 99%, respectively). By contrast, the negative charge on Asp172 proved indispensable: Asp172Asn and Asp172Ala were inactive, whereas the conservative Asp172Glu variant retained 93% activity, consistent with sequence variation among orthologs.

A

Fig. 2. Ternary complex defines substrate binding in NosH. (A) Ternary complex of NosH with non-hydrolysable FPP analog farnesyl S-thiolodiphosphate (FSPP; 18), guanidine (1), and $Mg^{2+}$ . The FSPP diphosphate is stabilized by $Mg^{2+}$ , while the prenyl chain is bound in the hydrophobic trench and engaged through hydrophobic interactions. The $F_{O}-F_{C}$ electron density map for 18 is shown as grey isomesh contoured at $3\sigma$ . (B) Close-up of the active site. Guanidine is coordinated by Asp140 and Asp172, and Arg137 is repositioned between guanidine and the C-1 atom of FSPP. Dashed lines represent salt bridges and hydrogen bonds; distances given in Å.

Arg137 emerged as a key residue (fig. S27). In the guanidine-bound structure, its guanidino group lies close to the substrate, whereas in the FSPP-bound complex, Arg137 forms a salt bridge with Asp176, enabling alignment of the isoprenoid donor for prenyl transfer. In the ternary complex, Arg137 reorients toward guanidine, displacing the isoprenoid C-1 carbon. We therefore propose that Arg137 toggles between two states: one positioned near guanidine and one bound to Asp176. The positively charged side chain of Arg137 may lower the $pK_{a}$ of the guanidine substrate and facilitate guanidine activation by Asp172. The salt bridge with Asp176 may prevent steric interference with FPP binding. Mutants still able to lower the $pK_{a}$ of the guanidine substrate (Arg137Lys and Arg137Met) retained activity whereas mutants harboring short (Arg137Ala) or bulky (Arg137Leu) side chains were impaired. The importance of the Arg137-Asp176 interaction was further supported by Asp176Asn, which showed virtually no activity, and Asp176Glu, which retained 67% activity. We therefore propose that Arg137 and Asp172 facilitate guanidine deprotonation and its conversion into a nucleophile for prenyl transfer (Fig. 3A and fig. S28). Whether the proton is relayed directly to the diphosphate or through Asp176 remains unresolved.

NosH orthologs AgdT and AgdS had previously been annotated as components of cyanobacterial aeruginoside (S15) and microguanidine (S16 and S17) BGCs in silico, though their functions remained unverified (20). The recently characterized ScAer3, which transfers DMAPP to agmatine but was not reported to use free guanidine, can now be considered part of the broader NosH-like guanidine prenyltransferase lineage (29). A principal difference between NosH and these agmatine/arginine-using enzymes is residue Asn175, which corresponds to Asp in the latter (fig. S29). Mutation of this residue in NosH (Asn175Asp, hereafter $\mathrm{NosH}^{\mathrm{RP}}$ ) expanded substrate specificity, enabling acceptance of agmatine and arginine in addition to guanidine (Fig. 3B and figs. S30 and S31).

To rationalize this change, we determined the 1.85-Å crystal structure of NosH $^{RP}$ in complex with Arg (10) (Fig. 3C and fig. S32). The guanidino group occupies the same position as free guanidine in the NosH active site, whereas the remainder of Arg adopts two alternative conformations: In one conformation, the Arg carboxyl group coordinates a Ca $^{2+}$ ion from the crystallization condition and would clash with the prenyl donor, suggesting that this state is a crystallization artifact. In the second, the $\alpha$ -amino group forms a salt bridge with Asp175 and is compatible with FPP binding. This structure therefore provides a rationale for how Asn175Asp enables recognition of extended guanidine-containing substrates without altering the position of the reactive guanidino group.

NosH $^{RP}$ also accommodated longer isoprenoid chains without apparent length limitation, producing derivatives 12, 13, 19, 20, and S65 to S70 with excellent conversion (figs. S33 to S37). Its enhanced efficiency allowed us to assay additional arginine analogs (Fig. 3D and fig. S38 to S41). Guanidinoacetic acid (21) and guanidinobutyric acid (S73) were converted to their farnesylated products (22 and S74) with yields exceeding those of arginine. L-Homoarginine (23) and L-arginine O-methyl ester (25) were also accepted (yielding 24 and 26), whereas modifications of the guanidino group itself, such as in L-canavanine (27, S77, S78), were detrimental, likely owing to altered electrostatics or steric hindrance. NosH $^{RP}$ prenylated both L- and D-arginine (10 and 28), although the L-form was preferred (fig. S41).

Finally, the architecture of the NosH isoprenoid-binding trench suggested compatibility with non-natural FPP analogs (32–35). NosH and $NosH^{RP}$ accepted three of five tested synthetic FPP derivatives (30 to 32, S7, and S8), yielding prenylated products 33 to 35 and corresponding L-arginine and agmatine derivatives S83 to S86 (Fig. 3E and figs. S42 to S46). Substrates bearing altered double-bond positions or bulky substituents were not accepted, consistent with steric and geometric constraints of the active site. One accepted analog features a terminal allyl group that provides a chemically addressable handle, highlighting the potential of NosH-derived enzymes for selective guanidine functionalization.

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Structure-guided discovery of NosH homologs in plants

The occurrence of guanidine-containing natural products, such as galegine (2), in plants raised the question of whether nature employs NosH-like guanidine prenyltransferases beyond bacteria (fig. S47). A standard BLAST search against plant enzyme databases identified proteins that we classify as putative guanidine prenyltransferases among the top hits; however, their sequence identity to NosH was typically below 30%, making confident functional assignment difficult by sequence similarity alone. We therefore leveraged our structural insights to define the three-dimensional architecture of the NosH active site as a higher-level descriptor for enzyme discovery and performed a structure-guided, motif-based search supported by Chai-1-generated structural models (36). Specifically, careful analysis of the NosH crystal structures identified a diagnostic R/KxxD motif together with a second acidic residue at a fixed spacing (R/KxxD/Ex $_{31}$ D/E) as a signature for guanidine coordination. This intentionally stringent composite motif served as the primary sequence-level filter for candidate identification and enabled us to exclude enzymes with related folds, such as class I terpene cyclases, which lack the NosH-guanidine recognition architecture.

A

B

C

D

E

Fig. 3. Mechanism and substrate reprogramming of NosH. (A) Proposed catalytic mechanism. The Asp140/Asp172 clamp positions and activates guanidine for nucleophilic attack on the C-1 of FPP (9), coupled to diphosphate departure and protonation. The precise proton-transfer route remains unresolved. (B) Substitution of Asn175 with Asp $(\mathrm{NosH}^{\mathrm{RP}})$ broadens acceptor specificity, enabling utilization of arginine and agmatine in addition to free guanidine. (C) Superposition of the $\mathrm{NosH}^{\mathrm{RP}}$ -L-arginine complex (blue surface) and the NosH-guanidine complex (green sticks). The L-arginine conformation compatible with FPP binding is shown in orange; the alternative, $\mathrm{Ca^{2+}}$ -coordinated conformation is shown as black sticks. Conformational differences in active-site residues are indicated by arrows, with distances shown in Å. (D) Acceptor scope of $\mathrm{NosH}^{\mathrm{RP}}$ toward arginine derivatives. Both L- and D-arginine (10 and 28) are accepted, with preference for the L-enantiomer, whereas modification of the guanidino group impairs conversion. (E) NosH and $\mathrm{NosH}^{\mathrm{RP}}$ tested with FPP derivatives 30–32, S7 and S8. Substrates 30–32 were accepted, while S7 and S8 were not.

Comprehensive bioinformatic analyses revealed NosH-like orthologs not only in plants but also across several bacterial and algal lineages, including Actinomycetota, Gammaproteobacteria, Cyanobacteriota, Chlorophyta, and Alveolata (fig. S48). Integrating structural similarity searches with motif-based filtering recovered more than 1000 putative guanidine prenyltransferases across diverse taxa, demonstrating that structural features can recover evolutionarily remote enzymes that evade confident annotation by conventional sequence searches.

Phylogenetic analyses revealed distinct bacterial and plant clades, each associated with characteristic genomic contexts consistent with roles in specialized metabolism (fig. S48). In Cyanobacteriota and Actinomycetota, NosH orthologs were embedded in putative BCGs for terpenes, aeruginoguanidines, microguanidines, and microcystine (S47), as well as in cryptic or hybrid clusters containing genes encoding nonribosomal peptidesynthetases (NRPS), polyketide synthases (PKS), and ribosomally synthesized and posttranslationally modified peptides (RiPPs) (figs. S49 to S61 and tables S7 to S12) (20, 37, 38). These data imply that NosH-like proteins could also act on guanidino groups in more complex settings, such as peptides, although additional experiments will be required to investigate this hypothesis. In plants, we discovered a NosH ortholog in every genome analyzed, and identified more than 600 candidate proteins across more than 100 families, with Fabaceae (82 proteins), Poaceae (70), and Brassicaceae (49) most represented (fig. S62). Sequence alignments revealed high conservation of residues critical for NosH catalysis (Glu52, Asp59, Leu106, Arg/Lys137, Asp140, Asp/Glu172; NosH numbering) and variable spacing between the guanidine-coordinating Asp140 and Asp/Glu172 residues (14 to 85 aa; median 32 aa) (Fig. 4A and fig. S63). Plant orthologs most often carried Lys in place of Arg137 and occasionally Glu in place of Asp172 (fig. S64). All plant orthologs carry Asp at the position equivalent to NosH

A

Fig. 4. Structure-guided discovery and validation of plant guanidine prenyltransferases. (A) Conservation of catalytic and magnesium-binding residues in bacteria and plant orthologs. (B) Selected plant and algal orthologs chosen for heterologous expression and biochemical characterization. (C) LC-MS analysis of representative reactions of the four NosH orthologs using guanidine (i and ii), agmatine (iii), or L-arginine (iv) as substrates. EICs show formation of the indicated prenylated products. (D) Proposed and experimentally supported routes to the guanidine alkaloids galegine (2) and pterogynine (4). The left panel summarizes proposed biosynthetic relationships; the right panel shows transformations supported experimentally in this study, including heterologous galegine production following expression of CofH-Iso1 in Nicotiana benthamiana. Parts of the figure were created using BioRender.

Asn175, suggesting that this residue may tune substrate preference across the phylogenetic tree (fig. S65).

Compared with bacterial orthologs, plant enzymes exhibited greater structural diversity and were represented by multiple splice forms, with up to 14 predicted variants per gene. Some consisted of the NosH-like core and additional $\alpha$ -helical domains, whereas others appeared to be embedded in larger proteins (fig. S62 and S66). A highly conserved $\alpha$ -helical part of plant NosH orthologs corresponds to a fold class frequently associated with ubiquitin-binding proteins (fig. S67). To test catalytic activity, we selected eight orthologs for heterologous expression in $E.$ coli and biochemical characterization (tables S13 and S14). Six proteins were expressed and purified successfully: orthologs from Cannabis sativa (CanH), Chlamydomonas reinhardtii (CamH), Edaphochlamys debaryana (EdaH), Physcomitrium patens (PhyH), and Coffea arabica (CofH-Iso1 and CofH-Iso2, two splice isoforms) (Fig. 4B). All six displayed guanidine prenyltransferase activity in the presence of $\mathrm{Mg}^{2+}$ (Fig. 4C and figs. S68 to S77). They accepted free guanidine (1), L-Arg (10) and Agm (11) as substrates, but preferentially utilized DMAPP (S2) as prenyl donor; longer-chain polyprenyl diphosphates were not accepted. This restriction is consistent with predicted structural differences, as plant orthologs possess a binding pocket rather than the hydrophobic tunnel found in NosH (fig. S78).

The biochemical relevance of these enzymes is underscored by their capacity to produce several guanidine alkaloids in vitro, including dimethylallylguanidine (galegine; 2), pterogynine (4), and pterogynidine (36). We further observed differences in product profiles between plant and algal NosH orthologs: The algal enzymes CamH and EdaH used doubly prenylated derivatives as substrates for an additional prenylation step, yielding an additional triply prenylated metabolite (37) (figs. S68 and S69). The characterized orthologs further accepted both L-arginine and agmatine as substrates for dimethylallyl-prenylation, yielding the plant metabolite sphaerophysin (38) and compound 39 in vitro. The biosynthesis of galegine (2) has long remained speculative as a result of limited genomic data and ambiguous isotopic labeling studies (12, 39). The heterologous expression of the NosH ortholog CofH-Iso1 in Nicotiana benthamiana led to the production of galegine (2) in planta (fig. S79). The identification and biochemical validation of NosH-like enzymes now provide a direct enzymatic link to pharmacologically relevant guanidine alkaloids and establish prenylation of free guanidine as a conserved biochemical strategy in plant-specialized metabolism (Fig. 4D, fig. S80, and table S15).

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Discussion

Our work establishes direct prenylation of free guanidine as a conserved feature of plant and bacterial metabolism. Combining structural analysis with motif-based annotation revealed an active-site architecture comprising the two-aspartate guanidine clamp, R/KxxD... D/E spacing, and hydrophobic prenyl-binding trench, enabling detection of evolutionarily remote orthologs not confidently assigned by sequence similarity alone. This illustrates how conserved catalytic architecture can guide discovery across evolutionarily distant lineages, whose shared catalytic logic is preserved at the structural rather than sequence level.

Guanidine prenyltransferases are widespread in bacteria and plants, frequently appearing as multidomain proteins that include ubiquitin-binding folds or other regulatory architectures. Although the functions of these additional domains remain unknown, their recurrent association with guanidine prenyltransferase cores suggests roles in broader biosynthetic, regulatory, or recognition processes. A possible example is tetrodotoxin biosynthesis, for which a polyprenylated guanidine has been proposed as a precursor and NosH produces the corresponding compound in vitro (40). Plant NosH-like enzymes produce guanidine alkaloids such as galegine (2), pterogynine (4), and sphaerophysine (38) in vitro, whereas heterologous expression in N. benthamiana yields galegine. These observations extend the relevance of guanidine prenylation beyond bacterial metabolism and support a broader role for NosH-like enzymes in plant guanidine-alkaloid biosynthesis. (Fig. 4D and figs. S79 and S80).

Mechanistically, NosH is a guanidine prenyltransferase with a class I terpene cyclase-related fold but catalytic logic distinct from amidinotransferases or ABBA-type prenyltransferases. A two-aspartate clamp and an Arg137-based conformational switch enable guanidine activation and substrate positioning. This architecture supports broad substrate tolerance, whereas the NosH $^{RP}$ -Arg structure explains how the Asn175Asp substitution expands substrate scope by providing an additional interaction for extended guanidino substrates without altering the position of the reactive guanidino group.

Beyond its biological importance, NosH offers opportunities for biocatalysis. NosH and $NosH^{RP}$ catalyze the selective formation of alkylated guanidines under mild, aqueous conditions and accept non-natural prenyl donors carrying chemically addressable handles. This provides an enzymatic route to guanidinium-functionalized building blocks relevant to chemical biology and materials chemistry, where guanidinium-functionalized surfaces, coatings, and membranes show antimicrobial, antifouling, and membrane-interactive properties (41–44). More broadly, NosH illustrates how structurally defined active-site motifs can uncover distant enzyme orthologs and the biosynthetic logic of cryptic metabolites beyond the reach of sequence annotation.

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ACKNOWLEDGMENTS

We acknowledge the use of the ESRF beamline ID-30B and the local contacts for their support. We want to especially thank J. Hakanpää and S. Chatziefthymiou from P11 beamline at DESY for their excellent help during data collection. The authors want to further thank A. Palusczak for her help performing LC-MS measurements and J. Zapp for NMR structure elucidation. We want to express our gratitude for helpful discussions and proofreading of the manuscript to P. Stallforth, S. E. O'Connor, J. Hartig, and R. G. da Silva. Funding: This work was supported by the following: European Research Council (ERC CoG 101002326); zukunft.niedersachsen (funding program of the Lower Saxony Ministry of Science and Culture); Volkswagen Foundation. K.K. was supported by the Dissertation Plus scholarship from the Claussen-Simon-Stiftung. Author contributions: D.K. and J.K. conceived the idea for the study. D.K. and J.K. developed the hypothesis and designed the experiments. D.K. performed protein purification, in vitro biochemical reactions, kinetic experiments, protein crystallization, and protein structure elucidation. K.K. and S.R. designed and performed bioinformatic analyses. D.K. performed genome mining and biosynthetic gene cluster identification. D.T., T.J., and S.S. performed organic synthesis for NosH substrates, reference compounds, and FSPP. H.S. provided FPP derivatives for biochemical transformations. A.B. and Jo.F. performed Nicotiana benthamiana experiments. D.K., J.K., K.K., S.R., A.L., Ja.F., C-P.W., and A.K. analyzed and discussed the results. D.K., J.K., K.K., and S.R. prepared the manuscript. Competing interests: Authors declare that they have no competing interests. Data, code, and materials availability: Coordinates for the crystal structures determined within this study were deposited to the Protein Database under the following entry ID: NosH-apo (pdb\_00009tgv), NosH-gua (pdb\_00009tgx), NosH-FSPP-Mg $^{2+}$ (pdb\_00009tgz), NosH-Gua-FSPP-Mg $^{2+}$ (pdb\_00009th3), NosH $^{RP}$ -Arg (pdb\_000031ka). No new code was generated during the course of this study. Methods and characterization for all chemical materials can be reproduced according to the methods. Requests for biological materials such as plasmids, and raw data should be directed to J. Koehnke. Materials are available without material transfer agreements (MTAs). Tabular data from figures and text can be found in data S57. License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse. This research was funded in whole or in part by the European Research Council (ERC CoG 101002326); as required, the author will make the Author Accepted Manuscript (AAM) version available under a CC BY public copyright license.

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.aeg1821

Materials and Methods; Figs. S1 to S84; Tables S1 to S19; Data S1 to S57;

MDAR Reproducibility Checklist; References (45–92)

Submitted 5 February 2026; accepted 26 August 2026

SOLID-STATE PHYSICS

Thermodynamic origin of the phonon Hall effect in a honeycomb antiferromagnet

Qingkai Meng $^{1,2\dagger}$ , Xiaokang Li $^{1*}\dagger$ , Jie Liu $^{1}$ , Lingxiao Zhao $^{3}$ , Chao Dong $^{1}$ , Zengwei Zhu $^{1*}$ , Liang Li $^{1*}$ , Kamran Behnia $^{4*}$

The underlying mechanism of the thermal Hall effect generated by phonons in a variety of insulators is yet to be identified. In this work, we report on a sizable thermal Hall conductivity in nickel phosphorus trisulfide (NiPS $_3$ ), a van der Waals stack of honeycomb layers with a zigzag antiferromagnetic order. The longitudinal ( $\kappa_{aa}$ ) and the transverse ( $\kappa_{ab}$ ) thermal conductivities peak at the same temperature, and the thermal Hall angle, at this peak, respects a previously identified bound. The amplitude of $\kappa_{ab}$ is extremely sensitive to the amplitude of magnetization along the $b$ axis but is not correlated with the phonon mean free path, which points to an intrinsic origin.

The thermal analog of the electrical Hall effect is dubbed the thermal Hall effect (THE). It refers to a transverse temperature difference generated by a longitudinal heat current in the presence of a perpendicular magnetic field. For a long time, phonons, lacking charge and spin, were thought incapable of contributing to the THE (1). However, this assumption was proven wrong by the discovery of a THE in a paramagnetic insulator $\left(\mathrm{Tb}_{3}\mathrm{Ga}_{3}\mathrm{O}_{12}\right)$ in 2005 (2). Numerous experiments (3–20) have reported a detectable THE in a wide variety of insulators, including three nonmagnetic solids (10, 18, 20). These experimental observations motivated many theoretical studies on how the lattice vibrations (phonons) can couple to the magnetic field (1, 21–31).

$\mathrm{NiPS}_3$ is a layered antiferromagnet, in which Ni atoms form honeycomb layers that are stacked along the $c$ axis with a lateral shift and are coupled by van der Waals interactions (Fig. 1A) (32, 33). Its zigzag antiferromagnetic order can be described by a Hamiltonian with ferromagnetic exchange between the first and the third neighbors and a much weaker antiferromagnetic exchange between the second neighbors (34, 35). It has an energy gap of $1.8\mathrm{eV}$ (33) and belongs to the family of $MPX_3$ (where $M = \mathrm{Fe}$ , Mn, or Ni and $X = \mathrm{S}$ or Se) van der Waals magnets. Exfoliation of the bulk has shown that the magnetic order of $\mathrm{NiPS}_3$ is fully and abruptly suppressed in the monolayer limit. This implies the importance of the interlayer coupling for the magnetic order (36). The discovery of spin orbit-entangled excitons associated with a Zhang-Rice singlet-triplet transition (37) has amplified the interest in this family as a platform for studying many-body coherence and coupling (38-41). Recently, infrared and Raman spectroscopy detected hybridization between magnon and optical phonon bands in $\mathrm{FePSe}_3$ (38, 40, 41).

In this work, we report on the observation of the THE in $NiPS_{3}$ , a van der Waals honeycomb antiferromagnet. The longitudinal and transverse thermal conductivities peak at the same temperature, and the maximum thermal Hall angle is comparable to what was found in other insulators. Notably, we find a strong correlation between transverse thermal response and in-plane magnetic anisotropy. Combined with the presence of magnon-phonon band crossings in this magnetic solid, the observation supports an intrinsic phonon THE that may be driven by magnon-phonon hybridization.

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Measuring thermal transport

The NiPS $_3$ single crystals used in this work were grown by the chemical vapor transport method using I $_2$ as the transport agent [see the supplementary materials for more details (42)]. The temperature dependence of the magnetization can be seen in Fig. 1B. The Néel temperature is 155 K and the easy axis along the $a$ , consistent with previous studies (32, 35, 37). As seen in Fig. 1C, the field dependence of magnetization up to 55 T (at 4.2 K) does not show any transition. Given the magnetic moment of Ni atoms (1.05 $\mu_B$ ) (32), at this field, the Zeeman energy is 3.2 meV. The persistence of the magnetic order is consistent with the largest exchange parameter quantified by inelastic neutron scattering ( $J_3 = 6.9$ meV) (34, 35).

We simultaneously measured longitudinal and transverse thermal transport using the one-heater-three-thermocouples method, shown in Fig. 1D (42). Figure 2A displays the temperature dependence of $\kappa_{aa}$ at $0\mathrm{T}$ and $14\mathrm{T}$ , which superpose on top of each other. No strong anomaly is detectable at the Néel temperature, which indicates that phonons are the exclusive carriers of heat. $\kappa_{aa}(T)$ peaks at $274\mathrm{W K}^{-1}\mathrm{m}^{-1}$ , which is larger than in most magnetic insulators, slightly lower than in $\mathrm{Cu_3TeO_6}$ (14), and well below what is observed for phonons in nonmagnetic insulators such as black phosphorus (18) [or diamond, where the peak exceeds $10^{4}\mathrm{W K}^{-1}\mathrm{m}^{-1}$ (43)], confirming the marginal role of magnons in carrying heat.

Figure 2B shows the field dependence of the thermal Hall conductivity $\kappa_{ab}$ at three typical temperatures and up to 14 T. The field dependence is always linear, but the absolute magnitude increases substantially from 2.6 mW K $^{-1}$ m $^{-1}$ at 305 K to 910 mW K $^{-1}$ m $^{-1}$ at 33 K (the sign remains negative). This is much larger than the enhancement of $\kappa_{aa}$ , which implies that the thermal Hall angle, defined as the ratio of the two, also increases when cooling.

Figure 2C displays the temperature dependence of $\kappa_{aa}$ (divided by a factor of $-160$ ) and $\kappa_{ab}$ at $14\mathrm{T}$ . $\kappa_{ab}$ does not show any jump at $T_N$ and peaks, at $25\mathrm{K}$ and $14\mathrm{T}$ , to attain a markedly large value of $-1636\mathrm{mW}$ $\mathrm{K}^{-1}\mathrm{m}^{-1}$ . As observed in prior works (10, 18), $\kappa_{aa}(T)$ and $\kappa_{ab}(T)$ peak at the same temperature. Moreover, the thermal Hall angle, defined as the ratio of $\kappa_{ab}$ to $\kappa_{aa}$ divided by the magnetic field, peaks to $4\times 10^{-4}\mathrm{T}^{-1}$ at this temperature. This value remains within a narrow range of $10^{-4}$ to $10^{-3}\mathrm{T}^{-1}$ , where most reported maximal thermal Hall angles lie (fig. S9) (18).

The phonon mean free path at peak temperature in these materials varies from 10 nm to 100 $\mu$ m (18). By contrast, the thermal length ( $\lambda_{tha}$ ) scale extracted from the experimentally measured maximum Hall angle, $\lambda_{tha} = \sqrt{\frac{\hbar}{eB} \times \kappa_{ab} / \kappa_{aa}}$ , shows little variation (18); therefore, it may be linked to two other relevant length scales—the interatomic distance and the phonon wavelength at the peak temperature—which, unlike the phonon mean free path, do not vary substantially across these insulating solids (18).

Proposed theoretical mechanisms of the phonon THE (1, 2I–3I) can be broadly divided into extrinsic and intrinsic. Most extrinsic scenarios invoke the phonon mean free path. For example, according to a recent theoretical proposal (28), longitudinal and transverse thermal conductivities can be simply expressed as $\kappa_{aa} \sim Cv^{2}\tau \propto \ell$ and $\kappa_{ab} \sim Cv^{2}\tau^{2}\tau_{0}^{-1} \propto \ell^{2}$ . Here, C, v, $\tau$ , $\ell (=v\tau)$ , and $\tau_{0}^{-1}$ are the phonon specific heat, the speed of sound, the average scattering time, the mean free path, and the time-reversal odd skew scattering rate, respectively. The two equations imply $\kappa_{aa} \propto \ell$ , $\kappa_{ab} \propto \ell^{2}$ , and $\kappa_{ab}/\kappa_{aa} \propto \ell$ , in contrast to experiment, which finds that $\kappa_{ab}/\kappa_{aa}$ does not depend on $\ell$ .

A

B

C

D

Fig. 1. Lattice structure, magnetization, and thermal transport setup. (A) Lattice structure of NiPS $_3$ (with space group $C2/m$ ). The side view (top) shows the layered structure. Each layer consists of a honeycomb lattice of NiS $_6$ octahedra. Below the Néel temperature, the magnetic moments along the $a$ axis form ferromagnetically zigzag chains and order antiferromagnetically between the chains (with magnetic space group $P_{C}2_1/m$ ) (35,37). (B) Temperature dependence of magnetization at 7 T with three different orientations. The curves deviate from each other at 155 K, suggesting an antiferromagnetic phase transition, consistent with the previous literature (32). (C) High-field magnetization up to 55 T at 4.2 K. Absence of transition indicates a robust antiferromagnetic exchange interaction. (D) Setup for simultaneous measurements of longitudinal $[\nabla T_a = -(T_3 - T_2)/I]$ and transverse $[\nabla T_b = -(T_2 - T_1)/w]$ thermal gradients. The magnetic field is along the $c^*$ axis.

A

B

C

Fig. 2. Longitudinal and transverse thermal conductivities of NiPS $_{3}$ . (A) Temperature dependence of longitudinal thermal conductivity ( $\kappa_{aa}$ ) under magnetic fields of 0 T and 14 T. The two curves coincide with each other in the whole temperature region, with a peak around 25 K. (B) Field dependence of transverse thermal conductivity ( $\kappa_{ab}$ ) at three different temperatures with the field sweeping to 14 T. In thermal Hall measurements, the heat current is along the a (x) axis, and the transverse temperature gradient is along the b (y) axis. (C) Comparison of the temperature-dependent $\kappa_{aa}$ (divided by -160) and $\kappa_{ab}$ .

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Sample dependence of the THE in NiPS $_{3}$

Studying five crystals of NiPS $_3$ , we found very similar values of longitudinal thermal conductivity and a sample-dependent thermal Hall response correlating with the anisotropy of magnetization and the presence of twinning. The results are shown in Fig. 3. The temperature dependence of magnetization $M$ at 7 T in five different samples is shown in Fig. 3, A and B. Whereas $M_a$ is almost unchanged across the samples, $M_b$ displays a sample variation of $\approx$ 30\% between the most and the least anisotropic samples. Our data are consistent with what has been reported by two other groups (fig. S12). The sample dependence of magnetization can be understood based on the presence of twins (44, 45). The difference between the magnetization along the $a$ axis and that along the $b$ axis is attenuated by the presence of minority domains. A reasonable conjecture is that weaker magnetic anisotropy reflects a higher density of twins in the sample [see the “Twins” section for details (42)]. Sample 1, with the highest magnetic anisotropy, is the closest to a perfect untwinned sample; sample 3 is characterized by almost equal populations of the three possible crystalline domains. Torque magnetometry, which is particularly sensitive to magnetic anisotropy, further supports this interpretation in two representative samples (Fig. 3C). The angle dependence of the magnetic free energy shows a twofold oscillation vanishing at the two high-symmetry axes. Its amplitude is larger in the sample with the larger $\frac{M_b}{M_a}$ (sample 4). Figure 3, D and E, shows the temperature dependence of $\kappa_{aa}$ and $\kappa_{ab}$ in five different samples. $\kappa_{aa}$ curves all fall on top of each other. This is also the case for the $\kappa_{bb}$ and the specific heat (figs. S5 and S7). Despite the identical phonon mean free path, the transverse response $\kappa_{ab}$ is very sample dependent. The peak amplitude is $\sim$ 10 times as large in sample 1 as in sample 3.

The correlation between the amplitude of the thermal Hall conductivity and a component of magnetization (Fig. 3E, inset) is reminiscent of the Streda formula linking a Hall response to a thermodynamic property (46, 47). In sharp contrast to this correlation, the longitudinal thermal conductivity and phonon mean free path are isotropic and do not correlate with $\kappa_{ab}$ or with $M_{b}/M_{a}$ .

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Discussion and outlook

$\mathrm{NiPS}_3$ is not the first case of a THE with variable amplitude. Replacing a tiny fraction of Sr atoms with Ca strongly damps $\kappa_{xy}$ in $\mathrm{SrTiO_3}$ (16). In $\mathrm{Sr}_2\mathrm{IrO}_4$ (48), replacing Ir with Rh first amplifies $\kappa_{xy}$ before suppressing it when the magnetic order is destroyed. In both these cases, however, the large change in the amplitude of the thermal Hall angle is accompanied by a change in the longitudinal thermal conductivity and a modification of the ground state. In the present case, we observed a 10-fold variation of the thermal Hall response with no change in the longitudinal transport. The accompanying change in the magnetic response implies that the variation of the thermal Hall response is driven by the realignment between the spin and the crystal lattices.

Comparing $NiPS_{3}$ with $\alpha-RuCl_{3}$ is also instructive. Both are van der Waals layers of a honeycomb lattice with a zigzag antiferromagnetic order at zero temperature. However, in the latter, in contrast to the former, one suspects the presence of a sizable Kitaev term. In this context, it is notable that the longitudinal and the transverse thermal conductivity are both a hundred times as large in $NiPS_{3}$ as in $\alpha-RuCl_{3}$ (fig. S10). This observation indicates that the replacement of well-defined magnons in $NiPS_{3}$ by a continuum of incoherent magnetic excitations in $\alpha-RuCl_{3}$ (4.9) leads to a severe damping of the phonon mean free path. Nevertheless, the thermal Hall angle of the two solids is roughly equal. What sets this angle neither scales with the phonon mean free path nor depends much on the magnetic excitations coupling with phonons.

Theoretically, degenerate chiral phonons are known to reside at the center of the Brillouin zone in a honeycomb lattice (50). The magnetic order in $NiPS_{3}$ , which breaks inversion center symmetry, lifts this degeneracy. Recently, Raman scattering and infrared conductivity have reported on the hybridization between magnons and optical phonons in a sister compound of $NiPS_{3}$ , $FePSe_{3}$ (38, 40, 41). However, heat is carried by acoustic phonons. Coupling between the latter and magnons has been suggested previously (51–53). Suppose that magnon and phonon modes cross each other at a point (Fig. 4A). In this case, even an infinitesimal coupling will lift the degeneracy, open a gap, and generate two hybrid modes. The lower mode has the capacity to carry heat and generate an odd response to a finite magnetic field. We note that in the study by Petit et al. (54), inelastic neutron scattering revealed spectroscopic evidence for mixing between phononic and magnetic modes in $Tb_{3}Ga_{5}O_{12}$ , the first THE insulator (2).

Motivated by these considerations, we compared the computed phonon spectrum of $NiPS_{3}$ (55) with the magnon spectrum extracted from inelastic neutron scattering measurements (45). The magnetic ordering generates a new Brillouin zone on top of the nuclear one (35, 45). The magnetic Brillouin projects rectangles over the hexagons of the honeycomb lattice (Fig. 4B). As a result of this zone folding, a boundary point of the nuclear Brillouin zone is located at the center of a magnetic Brillouin zone. This crucial feature allows magnons to mix up with acoustic phonons. Figure 4C is a representation of band dispersion of magnons and acoustic phonons along $\Gamma-M$ . One can see that magnon and phonon bands intersect at multiple points near the $\Gamma$ and M points of the Brillouin zone. These crossings, in the momentum space, occur along $b^{*}$ , and in real space, the amplitude of magnetization along the b axis was found to set the amplitude of $\kappa_{ab}$ . Near the M point, the three acoustic phonon branches cross the magnon bands, and the lowest crossing occurs at an energy of 3.7 meV. Finite coupling at this energy would open a gap. Yang et al. (27) have argued that, independent of the microscopic details, an intrinsic THE displays a simple behavior, $\kappa_{xy}/T \propto \exp(-T/T^{*})$ . $T^{*}$ represents the width of the energy window in which the Berry phase is finite and constant (8, 9, 19, 27). Figure 4D shows that our data for the least twinned sample (sample 1) display such a behavior. The fit yields $T^{*} = 12$ K. This 1-meV energy scale is markedly close to the distance between the magnon-phonon crossing points (Fig. 4C).

This picture is compatible with the extreme sensitivity of $\kappa_{ab}$ to twinning. Single-layer $NiPS_{3}$ is a honeycomb network of $NiS_{6}$ octahedra with a $C_{3}$ symmetry axis (the $c^{*}$ axis) normal to the ab plane. The zigzag magnetic order breaks the threefold symmetry (Fig. 4E) of these honeycomb layers. In the bulk crystal, these layers are stacked along one of the possible c axes, which are all tilted off the $c^{*}$ axis (Fig. 4F). Thus, crystallographic stacking and magnetic order each break the threefold symmetry in their own way. The zigzag order favors one of the three a axes. Stacking favors one of the three c axes. As a consequence, the relative orientation of the two $b^{*}$ axes, the one favored by crystalline stacking and the one favored by the magnetic order, rotates by $120^{\circ}$ in the three domains (Fig. 4F). This may account for the large attenuation of $\kappa_{ab}$ with the increasing presence of minority domains (42).

We found that NiPS $_{3}$ , a honeycomb lattice with a zigzag magnetic order, hosts a phonon THE with an amplitude set by magnetic anisotropy. Combined with magnon–acoustic phonon band crossing, the observation points to an intrinsic origin and a potential role played by magnon-phonon hybridization. Our results have implications for the intense debate on the origin of the THE in $\alpha$ -RuCl $_{3}$ , another honeycomb lattice with zigzag magnetic order. They raise the open question of the importance of magnon-phonon hybridization in generating phonon Berry curvature in other magnetic quantum materials.

A

B

T (K)

$\theta (^{\circ})$

Fig. 3. Sample dependence of thermal transport, in-plane magnetization, and torque in NiPS $_{3}$ . (A and B) In-plane magnetization for B//a (A) and B//b (B) in five different samples (1 to 5). There is no detectable change in $M_{a}$ , but $M_{b}$ changes by about 30%. (C) The angle dependence of torque at 30 K and 5 T in two samples (4 and 5). The sample with a higher $M_{b}$ (sample 4) has a larger torque response. (D) Temperature dependence of longitudinal thermal conductivity, $\kappa_{aa}$ , in different samples. The curves overlap. (Inset) Peak $\kappa_{aa}$ is plotted as a function of the in-plane magnetic anisotropy ( $M_{b}/M_{a}$ ) in the five samples. (E) Temperature dependence of the thermal Hall conductivity, $\kappa_{ab}$ in the five samples. Contrary to the $\kappa_{aa}$ , the $\kappa_{ab}$ is strongly sample dependent. (Inset) Correlation between the peak of $\kappa_{ab}$ and $M_{b}/M_{a}$ .

C

E

F

D

Fig. 4. Magnon-phonon hybridization and stacking twins. (A) Schematic diagram of the magnon-phonon band hybridization (51). (B) Brillouin zone boundaries for magnetic (red) and crystallographic (black) Brillouin zones (56). $\Gamma - Z - M$ is along the $b^{*}$ orientation. (C) Calculated phonon spectrum (in green) (55) together with experimentally derived magnon spectrum (35, 45) of NiPS $_{3}$ . There is a magnon-phonon crossing near the M point occurring near 4 meV. (D) A semi-log plot of $\kappa_{ab} / TB$ as a function of temperature in sample 1. $\kappa_{ab} / TB$ peaks at $\approx 30$ K. Above this temperature, it follows $\exp(-T / T^{*})$ , with $T^{*} = 12$ K. (E) Magnetic structure of NiPS $_{3}$ , viewed along the $c^{*}$ axis (top) and the $b$ axis (bottom) (32, 35). The black lines represent the boundaries of the unit cell. (F) Main (orange block) and secondary (blue and red blocks) domains with different stacking directions. Each domain is stacked along one of the three possible ( $c_{1}, c_{2}$ , or $c_{3}$ ) axes. Red arrows ( $b_{\mathrm{mag}}^{*}$ ) represent the $b^{*}$ axis perpendicular to the $a$ axis favored by the magnetic order. Orange arrows ( $b_{\mathrm{lattice}}^{*}$ ) represent the $b^{*}$ axis perpendicular to the $c$ axis favored by stacking. The angle between these two axes rotates by $120^{\circ}$ in the three domains.

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ACKNOWLEDGMENTS

We thank B. Fauqué, G. Grissonnanche, R. Valenti, and particularly A. Wildes for helpful discussions. Funding: This work was supported by the National Key Research and Development Program of China (grant nos. 2022YFA1403500, 2023YFA1609600, and 2024YFA1611200), the National Natural Science Foundation of China (grant nos. 12304065, 12674058, 12474043, 52588101, 51821005, 12004123, 51861135104, and 11574097), the Fundamental Research Funds for the Central Universities, the Hubei Provincial Natural Science Foundation (no. 2025AFA072), and the Cai Yuanpei Franco-Chinese program (no. 51258NK). Author contributions: X.L., Z.Z., and K.B. conceived and designed the study. L.Z. provided the samples used in this study. Q.M. and X.L. performed the thermal transport and magnetization measurements. L.L. developed the pulsed high-magnetic field facility and the magnetization measurement station. C.D. measured high-field magnetization under pulsed magnetic field. J.L. performed the magnetic torque measurements. Q.M., X.L., Z.Z., L.L., and K.B. analyzed the data. Q.M., X.L., Z.Z., and K.B. wrote the manuscript with assistance from all the authors. Competing interests: The authors declare no competing interests. Data, code, and materials availability: All data are available in the main text, the supplementary materials, and Zenodo (57). Details for the synthesis and characterization of all compounds and materials are provided in the materials and methods section. License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.adt1992

Materials and Methods; Supplementary Text; Figs. S1 to S13; References (58–64)

Submitted 16 September 2024; accepted 19 August 2026

MACHINE LEARNING

Sequential diagnosis with language models

Harsha Nori\*†, Mayank Daswani†, Christopher Kelly†, Scott Lundberg†, Marco Tulio Ribeiro†, Marc Wilson†, Xiaoxuan Liu, Viknesh Sounderajah, Jonathan M. Carlson, Matthew P. Lungren, Bay Gross, Peter Hames, Mustafa Suleyman, Dominic King, Eric Horvitz\*

We explored the capabilities of frontier language models in sequential diagnosis, a diagnostic paradigm that captures the iterative nature of clinical reasoning. Given a brief clinical presentation, clinicians selectively acquired information to reach a diagnosis, enabling assessment of diagnostic accuracy and workup cost. We developed an interactive benchmark and an artificial intelligence (AI) system that simulates a panel of physicians, continually revising the differential diagnosis and selecting cost-effective tests. Using this benchmark, the system achieved 83.2% accuracy on New England Journal of Medicine clinicopathological conference cases and 80.3% on MIMIC-IV-ED emergency department admissions, outperforming generalist physicians (36.1 and 46.8%, respectively). Although these findings were obtained in a controlled benchmark setting, they highlight the promise of language models for supporting more accurate, lower-cost diagnoses.

Clinical diagnosis is a sequential process of information gathering and reasoning rather than a one-shot analysis of a complete case. Physicians begin with limited information, formulate an initial differential diagnosis, and then choose questions to ask and tests to order, weighing the expected diagnostic yield of each against its cost, patient burden, and delay. As findings return, they continually revise the differential diagnosis and judge whether the evidence is sufficient to commit to a diagnosis or therapeutic action, or whether further workup is needed. Such interleaving of hypothesis refinement with strategic information gathering is the core of clinical diagnosis.

Language models (LMs) have promising medical reasoning capabilities, achieving top-tier scores on licensing examinations and structured diagnostic vignettes $(1-7)$ . Current evaluations of LMs have not tested diagnosis as an active, sequential information-gathering process that jointly considers diagnostic accuracy and diagnostic workup costs. Instead, benchmarks typically evaluate LMs on fully specified cases that bundle the chief complaint, history of present illness, physical examination findings, and diagnostic test results into a single prompt. By compressing diagnosis into one inference step, static benchmarks cannot measure whether a system asks the right questions, refrains from indiscriminate testing, updates the differential diagnosis as evidence accrues, or recognizes when sufficient certainty has been achieved to conclude the workup. Thus, they may overstate diagnostic competence while masking failure modes such as inappropriate testing or premature closure.

We introduce the Sequential Diagnosis Benchmark (SDBench), which transforms 304 clinicopathological conference cases from the New England Journal of Medicine (CPC cases) (8) and 325 emergency department-to-admission encounters from MIMIC-IV-ED (ED cases) (9) into interactive, stepwise encounters. Together, the CPC and ED cases span a broad spectrum of clinical presentations and documentation styles, with final diagnoses ranging from common conditions to rare disorders. Each case begins with a brief clinical vignette, from which a diagnostician [either an artificial intelligence (AI) agent or a physician] may ask questions, order diagnostic tests, or commit to a final diagnosis (Fig. 1). Performance was evaluated along two dimensions: diagnostic accuracy (measured against the reference diagnosis) and the cumulative estimated cost of the tests ordered. This framework evaluates not only diagnostic accuracy but also the ability to identify and acquire informative evidence efficiently and determine when sufficient diagnostic certainty has been achieved to conclude the encounter.

We used SDBench to evaluate Diagnostic Orchestrator (DxO), a model-agnostic orchestrator that performs sequential diagnosis by simulating a panel of clinical experts with complementary roles, incorporating cost-conscious test stewardship at each step and aggregating diagnoses across independent runs. Within SDBench, DxO operated at higher regions of the estimated cost-accuracy Pareto frontier (the operating points for which no evaluated method is simultaneously more accurate and less costly) when compared with that of participating individual generalist physicians under controlled, text-only conditions. These comparisons do not establish superiority over specialists, multidisciplinary teams, or real-world clinical practice. However, they show that LM orchestration of an iterative workflow can improve measured cost-accuracy trade-offs in a benchmark designed to evaluate sequential diagnosis and provide evidence that the methods can be harnessed to support clinicians.

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Results

SDBench presents each CPC and ED case as a text-based sequential encounter beginning with a short clinical vignette. At each step, a physician or AI system, serving in the role of a Diagnostic agent, can ask for history or examination findings, order diagnostic tests, or commit to a final diagnosis (Fig. 1). The key components and flow of SDBench are illustrated in Fig. 2. A Gatekeeper agent mediates all information requests drawing from the underlying case record, returning only information that is clinically obtainable from the specified question or test. When a requested finding is absent from the source record, the Gatekeeper generates diagnostically neutral synthetic results to avoid signaling the absence of data, which could provide clues about the final diagnosis. Final diagnoses are adjudicated by a Judge agent that uses a five-level physician-authored clinical rubric and the reference diagnosis, in which scores of 4 or 5 (diagnoses for which management would be unchanged) were considered correct (supplementary materials, materials and methods).

Testing costs were estimated from requested investigations by using Current Procedural Terminology (CPT)-based pricing derived from the chargemaster of a major health system (10), with history and examination questions treated as part of a fixed physician-visit cost. This framework allowed direct comparison of participating physicians, baseline LMs, and DxO variants across both diagnostic accuracy and cumulative testing cost (supplementary materials, materials and methods).

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Clinicopathological conference studies

We found that DxO with GPT-5 established a new Pareto frontier that outperformed the participating physicians at every cost or accuracy level (Fig. 3). The DxO configuration without budget constraints demonstrated particular effectiveness, achieving 83.2% accuracy at an average cost of \$5431. The structured reasoning of DxO responds to specified budgetary constraints with a slight lowering of accuracy with progressive reduction in testing costs, achieving 80.9% accuracy at an average cost of \$2241 and 79.6% at \$1303. At the other end of the spectrum, with a configuration aimed at achieving diagnostic excellence, accuracy jumped to 84.5% at a cost of \$8945. This trade-off was achieved by balancing how many questions versus tests were requested (supplementary text).

We recruited active primary-care and hospital and acute-care physicians (inclusive of internal medicine specialists, acute-care, and

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Diagnostic agent

detail when the sore throat, peritonsillar swelling, and bleeding began, how they have progressed, and any associated symptoms such as fever, difficulty swallowing, voice changes, ear pain, or breathing problems?

Seven weeks before admission: onset of sore throat. Over the first week, pain persisted. Four days later the soreness worsened, prevented sleep. Thirty-one days before admission, noted right-sided throat pain and swelling with sensation of food "stuck," accompanied by fatigue; no fevers, headaches, respiratory, gastrointestinal symptoms, or rash...

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Let's gather some history.

Series of questions covering past medical history, medication history, signs of malignancy, HIV/HPV history, dental issues, history of bleeding, pregnancy, initial labs (e.g. FBC, clotting, and imaging including MRI neck...

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Nasopharyngeal carcinoma?

Test request: Ultrasound-guided core biopsy of the right peritonsillar mass (large-bore), send for routine H&E, immunohistochemistry (CD31, D2-40, CD34, ERG, GLUT-1, pan-cytokeratin, CD45, CD20, CD3, Ki-67)

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Not it. Alveolar rhabdomyosarcoma?

neoplasm with high nuclear-to-cytoplasmic ratio and frequent mitotic figures.

Immunohistochemistry: CD31: negative D2-40: negative CD34: negative ERG: negative GLUT-1: negative Pan-cytokeratin: negative CD45: negative CD20: negative CD3: negative Ki-67: 60% nuclear positivity

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Histology (H&E): Infiltrative round-cell

Test request: Immunohistochemistry: Desmin, Myogenin, MyoD1 (to assess rhabdomyogenic differentiation)

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Let's rule out embryonal rhabdomyosarcoma

Immunohistochemical analysis of the peritonsillar biopsy specimen demonstrated tumor cells diffusely positive for desmin and MyoD1 and multifocally positive for myogenin.

Test request: FOXO1 (13q14) break-apart FISH on tumor tissue

Fluorescence in situ hybridization with break-apart probes to the FOXO1 (13q14) locus did not detect any FOXO1 rearrangements

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Diagnostician's final diagnosis

"Embryonal rhabdomyosarcoma of the right peritonsillar region"

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NEJM ground truth diagnosis

"Embryonal rhabdomyosarcoma of the pharynx"

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Comparison by judge

5/5 - Same disease; candidate adds correct specific location.

Fig. 1. Example of DxO solving a sequential-diagnosis reasoning problem. Initial case information: A 29-year-old woman was admitted to the hospital because of sore throat and peritonsillar swelling and bleeding. Symptoms did not abate with antimicrobial therapy.

Fig. 2. Orchestration in SDBench. A corpus of CPC or ED cases was transformed into a set of sequential-diagnosis challenges through coordination among the Gatekeeper, Diagnostic, and Judge agents. At run time, the Gatekeeper mediates requests for information from the Diagnostic agent, deciding whether and how to respond to the Diagnostic agent's questions about patient history, examination findings, and test results. The Judge evaluates whether the Diagnostic agent's final diagnosis matches the ground truth reported in the original case.

emergency-care physicians) to assess human performance on the benchmark. For the physician study with CPC cases (56 cases held out from engineering efforts during development), participants completed an average of 36.4 (closed book) and 34.8 (open book) cases, providing a total of 764 (closed book) and 662 (open book) human diagnoses over the 56 cases. On average, physicians spent 11.9 (closed book) and 18.1 (open book) minutes per case, asking 6.1 (closed book) and 8.4 (open book) questions and requesting 7.1 (closed book) and 12.1 (open book) tests, resulting in average costs of \$3049 (closed book) and \$4725 (open book). Their average diagnostic accuracies were 22.3% (closed book) and 36.1% (open book). Compared with closed-book testing, providing search and reference tools for the open-book CPC studies increased the number of questions asked and the number of tests ordered and boosted the overall time spent by the physicians per case, as well as the average cost of testing per case. Nevertheless, even the physician performing at the highest diagnostic accuracy (51.8%) was outperformed in both accuracy and cost. We found that physicians interleaved questions and tests compactly, asking a mean of 5.6 questions before ordering their first test. By contrast, DxO with GPT-5 asked a mean of 25.5 questions before ordering the first test on the same cases, indicating a different strategy of extensive structured history-taking before initiating diagnostic testing.

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Emergency medicine studies

CPC cases are curated by academic clinicians, whereas the ED cases consist of contemporaneous electronic health record (EHR) notes that reflect routine workflow and a more representative case mix. DxO without budget constraints achieved an average diagnostic accuracy of 80.3% at a mean cost of \$4979 per ED case (Fig. 4). With budget constraints, DxO achieved 73.2% at a cost of \$2634, and 69.5% at a cost of \$2037. As expected, generalist physicians showed greater proficiency on ED cases than on CPC cases, with 46.8% (versus 36.1%) average accuracy. The average cost of testing by physicians on ED cases was \$3400. The individual physician with the best diagnostic performance achieved 62.5% average accuracy at an average cost of \$3332 (40 cases).

As on CPC cases, DxO tended to ask more questions and order fewer tests than did participating physicians, especially under budget constraints. Whereas physician performance differed substantially on ED versus CPC cases, DxO accuracy was comparable on both datasets.

Fig. 3. Performance and Pareto frontiers for CPC cases. Points indicate average diagnostic accuracy and average cumulative medical cost for DxO with GPT-5, baseline LMs, and participating physicians (test set only; legend) on New England Journal of Medicine clinicopathological conference cases. Performances of participating physicians are displayed for closed-book (red +) and open-book (gray x) challenges, with the average performance for each setting (the boldface + and x).

Modern LMs, and DxO harnessing them, appear to handle long-tail, atypical patterns more consistently than did the participating clinicians. In contrast to the overall maintenance of LM performance across ED cases and CPC cases, the diagnostic accuracy of clinicians dropped precipitously on the rare complexities characterizing CPC cases.

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Studies of model capabilities and errors

We show the performance of DxO using GPT-5 in Fig. 3 (CPC cases) and Fig. 4 (ED cases). We compared the performance of DxO on CPC and ED cases with commercial LMs used with a minimal prompt (supplementary text), testing multiple families and sizes of models from a variety of providers. Across all of the models tested, DxO orchestration boosted the diagnostic accuracy on the ED cases and CPC cases by an average of 4.4 and 7.9 percentage points, respectively (supplementary text).

We studied and compared the diagnostic errors of DxO, baseline models, and participating physicians (supplementary text). We used two independent frontier LMs to categorize failures, followed by manual verification. DxO errors typically involved selecting a clinically adjacent answer at the wrong level of specificity rather than an unrelated disease. DxO's advantage over baseline models was concentrated in diagnoses that depend on better history-taking, such as rare exposures and travel-related infections. For such cases, deeper questioning surfaced discriminating clues that would not be easily found in broad test batteries. When physicians erred, their diagnoses tended to be more distant from the reference diagnosis than the AI errors were.

DxO was initially developed when GPT-4.1 was the strongest model available. We subsequently evaluated the approach with GPT-5 and, before publication, repeated the full evaluation suite using GPT-5.5 without modifying prompts or orchestration (supplementary text).

DxO continued to define the Pareto frontier, and its accuracy advantage over the baseline prompt increased with GPT-5.5, suggesting that improvements in model capability do not necessarily diminish the benefits of careful orchestration.

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Discussion

SDBench is a benchmark that transforms 304 New England Journal of Medicine CPC cases and 325 MIMIC-IV-ED cases into interactive, multiturn diagnostic challenges. Unlike static medical benchmarks, SDBench requires deciding what to ask, what to test, and when to commit, with each decision incurring cost. In the context of the benchmark, we presented DxO, an approach that executes a sequential diagnosis workflow with a simulated panel of clinical experts to decide which questions or tests to request. We showed that DxO improves diagnostic accuracy over baseline-prompted models while simultaneously reducing cumulative test costs, establishing a new Pareto frontier for accuracy and cost. Although DxO was initially developed by using CPC cases, it maintained Pareto dominance on the independent ED cases and across newly released LMs.

We found that DxO substantially outperformed practicing generalist physicians in diagnostic accuracy while often incurring lower cumulative testing costs. Such findings are perhaps unsurprising because CPC cases are selected for their instructional value and often include reflections and conclusions from specialists. We would expect the performance gap to narrow when comparing DxO with expert specialists or multidisciplinary specialist teams selected to match the content of each case. We had expected to see a smaller advantage for DxO on the ED challenges, which were drawn from routine emergency-department cases and therefore fall squarely within the everyday practice of generalist and emergency clinicians.

Fig. 4. Performance and Pareto frontiers for ED cases. Points indicate average diagnostic accuracy and average cumulative medical cost for DxO with GPT-5, baseline LMs, and participating physicians (legend) on patients admitted to the hospital after emergency department evaluation. Depicted are the open-book performances of individual physicians (gray x) and the mean performance (boldface x).

We hypothesize that part of the advantage derives from the scale of training exposure: Frontier LMs are trained on vast corpora that span rare diseases, atypical presentations, and cross-specialty reasoning, yielding a breadth of medical knowledge that no individual physician could master, while allowing LMs to apply that knowledge consistently across cases. Unlike human clinicians—whose diagnostic reasoning may be influenced by recent cases, time pressure, cognitive fatigue, or generalist and specialty-specific biases and blind spots—these systems maintain uniform recall and systematic evaluation. The orchestrated reasoning process implemented by DxO, in which simulated clinical experts pursue distinct reasoning goals, helps enforce consistent information gathering and cost evaluation, behaviors that physicians strive for but may not always sustain under cognitive load and constraints on time and resources.

Moreover, routine clinical practice appropriately prioritizes avoiding missed diagnoses and ensuring patient safety over explicit optimization of cumulative testing costs. Although clinicians may routinely consider resource utilization, they rarely have formal decision-support tools that continuously quantify the marginal diagnostic value and cost-effectiveness of each additional test. By maintaining an explicit differential diagnosis, challenging leading hypotheses through adversarial critique, and quantifying the marginal value of each test, the system is designed to mitigate common reasoning failures such as anchoring and premature closure. By contrast, most physicians do not have the luxury of a continuously available team that systematically audits their reasoning, challenges assumptions, and helps maintain diagnostic rigor throughout the workup.

These advantages are amplified within a controlled simulation. The benchmark environment abstracts away many details of medical practice, including uncertainty in patient histories and reporting, incomplete documentation, rapport building, and longitudinal follow-up. Clinicians also contend with time constraints, administrative requirements, and emotional and ethical considerations that shape care delivery but remain outside the scope of this study. Thus, the performance advantage refers specifically to information gathering and diagnostic accuracy under idealized conditions, not to the full scope of clinical reasoning, patient care, or medical judgment required in practice.

The results suggest that the structured reasoning processes underlying DxO's performance (explicit hypothesis tracking, adversarial critique, and cost-aware test selection) could augment human clinical judgment. Physicians already perform many of these cognitive tasks implicitly, but rarely with the same degree of systematization, economic accountability, or safeguards against cognitive bias. By codifying these processes, such systems could improve diagnostic consistency and make reasoning more transparent while complementing the clinical expertise and contextual judgment that remain essential to medical care. An important direction for future work is the design of clinician-AI workflows that incorporate the core capabilities of automated sequential diagnosis (11). Beyond supporting physicians in the diagnosis and cost-effective management of individual patients, the methods described here could also enable educational applications, including interactive diagnostic challenges and insight-building case simulations designed to refine clinical reasoning during medical training and continuing professional education.

Although SDBench moves us toward a more realistic evaluation of diagnostic reasoning of AI systems, limitations remain. The benchmark currently includes only pathological cases drawn from CPC cases and ED encounters. CPC cases may overrepresent diagnostically challenging presentations, and both exclude healthy or benign encounters, so the overall case mix and disease prevalence do not mirror those of routine clinical practice. Moreover, both physicians and AI agents interact with a text-based “oracle” gatekeeper, rather than EHRs or the full richness of patient encounters in the open world. The test sessions did not exhibit the noise, uncertainty, and ambiguity that can come with incomplete documentation and communication nuances, such as patients omitting or forgetting information, or temporal dynamics, including physiologic responses to preliminary interventions. Nor did the test sessions capture multimodal data such as imaging, waveforms, or pathology slides that are central to real diagnostic workflows. As a result, SDBench measures diagnostic reasoning under idealized information conditions rather than bedside performance or patient outcomes.

A limitation of our evaluation is the comparison of DxO performance with individual physicians. Real-world diagnosis often involves multispecialty collaboration situated in a rich health care ecosystem with processes for appropriate referral to different teams of specialists. In terms of metrics, the cost estimates used in SDBench rely on standardized US pricing data that approximate, but cannot fully capture, real-world variability and practical dimensions such as time-to-result, invasiveness, patient discomfort, and logistical availability. Similarly, the Judge rubric evaluates diagnostic correctness at the disease level but does not assess therapeutic appropriateness, safety, or longitudinal management quality. In practice, physicians diagnose, prescribe, and adjust iteratively over time, whereas SDBench and DxO focus solely on the diagnostic phase of reasoning.

More broadly, modeling diagnosis as a sequential, cost-aware process—rather than as a one-shot prediction problem—provides a framework for developing AI systems that more closely align with the iterative nature of clinical reasoning while supporting more transparent, economical, and collaborative medical decision-making. As models become increasingly capable, methods that integrate structured sequential inference with clinician expertise may reshape how AI supports diagnostic reasoning, with the potential to improve the quality and accessibility of health care worldwide.

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REFERENCES AND NOTES

1. H. Nori et al., arXiv:2311.16452 [cs.CL] (2023).

2. H. Nori, N. King, S. M. McKinney, D. Carignan, E. Horvitz, arXiv:2303.13375 [cs.CL] (2023).

3. H. Nori et al., arXiv:2411.03590 [cs.CL] (2024).

4. D. McDuff et al., Nature 642, 451–457 (2025).

5. S. Cabral et al., JAMA Intern. Med. 184, 581–583 (2024).

6. E. Goh et al., JAMA Netw. Open 7, e2440969 (2024).

7. P. G. Brodeur et al., Science 392, 524–527 (2026).

8. New England Journal of Medicine, Case Records of the Massachusetts General Hospital (2026); https://www.nejm.org/medical-articles/case-records-of-the-massachusetts-general-hospital.

9. A. Johnson et al., MIMIC-IV-ED (version 2.2). PhysioNet (2023); https://doi.org/10.13026/5ntk-km72.

10. Kaiser Permanente Washington, “Central Hospital standard charges” (2023); https://healthy.kaiserpermanente.org/content/dam/kporg/final/documents/health-plan-documents/coverage-information/910511770-central-hospital-standard-charges-wa-en.xlsx.

11. S. S. Everett et al., NPJ Digit. Med. 9, 409 (2026).

12. H. Nori et al., SDBench code and data. Zenodo (2026); https://doi.org/10.5281/zenodo.21286121.

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ACKNOWLEDGMENTS

We are grateful to NEJM Group for permission to use narratives and data from the New England Journal of Medicine clinicopathological conference cases in the research presented in this paper. This work has benefited from contributions of many teams at Microsoft. We extend our sincere thanks to colleagues both within and outside of Microsoft for their valuable insights, including B. Bunning (Stanford University), N. Ding (Microsoft), N. de Freitas (Microsoft), K. Mandl (Microsoft), A. Milicevic (Microsoft), V. Patel (Columbia University), J. Petro (Microsoft), H. Poon (Microsoft), D. Rhew (Microsoft), A. Rodman (Beth Israel Deaconess), N. Shah (Stanford University), C. Sherstan (Microsoft), C. Cooper Simpson (Microsoft), E. Shortliffe (Columbia University), K. Simonyan (Microsoft), P. Szolovits (MIT), E. Topol (Scripps Research), R. Wachter (UCSF), and J. Weinstein (Microsoft). We also thank G. Fontana (Prova Health) and K. Hawkins (Prova Health) for their support on health economics and outcomes. Funding: No funds external to Microsoft were acquired for these studies. Author contributions: Conceptualization: C.K., E.H., H.N., M.D., M.T.R., M.W., S.L. Methodology: C.K., E.H., H.N., M.D., M.T.R., M.W., S.L., X.L. Investigation: C.K., E.H., H.N., M.D., M.T.R., M.W., S.L., V.S., X.L. Visualization: C.K., E.H., H.N., M.D., M.T.R., M.W., S.L. Project administration: E.H., D.K., H.N., M.S. Supervision: E.H., H.N., D.K. Writing – original draft: C.K., E.H., H.N., M.D., M.T.R., M.W., S.L., X.L. Writing – review & editing: B.G., C.K., E.H., H.N., J.M.C., M.D., M.P.L., M.T.R., M.W., P.H., S.L., V.S., X.L. Competing interests: All authors are employees at Microsoft and hold equity in the company, which provides commercial services in AI and health care. C.K., E.H., H.N., M.D., M.T.R., M.W., S.L., and X.L. are inventors on US patent application 19/722,651 submitted by Microsoft that relates to an automated evaluation framework for sequential diagnosis. Data, code, and materials availability: No new materials were generated in this study. Code and data are available at Zenodo (12). The source code implementing SDBench—including the Gatekeeper, Judge, Cost Estimator, and baseline orchestration—is also available under the MIT License at https://github.com/microsoft/sdbench. Three datasets were used in the reported studies: (i) NEJM case records: SDBench was developed by using the case records of the Massachusetts General Hospital published in the New England Journal of Medicine (8). The SDBench dataset derived from these cases is available from NEJM Group for noncommercial research use under license; requests should be directed to elicensing@nejm.org. (ii) MIMIC-IV-ED: Emergency department encounters were drawn from MIMIC-IV-ED, a module of MIMIC-IV (9). The curated subset of cases used in this study will be released on PhysioNet alongside publication, subject to completion of PhysioNet credentialing and the MIMIC-IV Data Use Agreement. (iii) Test costs: Costing data used in this study were obtained from the Kaiser Permanente Washington Central Hospital Standard Charges file (chargemaster) (10), which is publicly available at https://healthy.kaiserpermanente.org/content/dam/kporg/final/documents/health-plan-documents/coverage-information/910511770-central-hospital-standard-charges-wa-en.xlsx (accessed April 2026). This file is published by Kaiser Permanente in compliance with the Centers for Medicare & Medicaid Services (CMS) Hospital Price Transparency rule (45 CFR Part 180), which requires hospitals to make standard charge information publicly available in a machine-readable format free of charge and without restrictions on reuse. SDBench natively ingests this file, but the framework can be adapted to accept any alternative chargemaster or costing sheet. License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.aeh7930

Materials and Methods; Supplementary Text; Figs. S1 to S9; Tables S1 to S13; References (13–29); MDAR Reproducibility Checklist

Submitted 4 April 2026; accepted 10 August 2026

Electronic bound states in the continuum in a two-dimensional metal

Morgan Thinel $^{1,2}$ , Xiong Huang $^{1}$ , Daniel G. Chica $^{2}$ , Simon Turkel $^{1,3}$ , Sebastian E. Rossi $^{1}$ , Christie S. Koay $^{2}$ , Hong Li $^{3}$ , Willa Mihalyi-Koch $^{2}$ , Bipasa Samanta $^{4}$ , Madisen Holbrook $^{1}$ , Aravind Devarakonda $^{5}$ , Luca M. Nashabeh $^{1}$ , Alexandru B. Georgescu $^{4*}$ , Xavier Roy $^{2*}$ , Xiaoyang Zhu $^{2*}$ , Abhay N. Pasupathy $^{1,3*}$ , Raquel Queiroz $^{1*}$

Bound states in the continuum (BICs) are quantum states that remain localized despite lying within a continuum of extended, delocalized states. Whereas optical BICs have been realized in photonic systems, achieving electronic bound states embedded in a metallic background remains an ongoing challenge. In this study, we used scanning tunneling microscopy to identify two defect-induced electronic states that remain localized within the metallic continuum of $Pd_{5}AlI_{2}$ , a two-dimensional van der Waals metal. Our calculations suggest that electron-hopping interference on the decorated checkerboard lattice of $Pd_{5}AlI_{2}$ gives rise to a (quasi) flat band built from spatially localized eigenstates that are orthogonal to the dispersive continuum. Atomic defects within this frustrated lattice shift the associated flat-band localized states into the metallic continuum, forming robust, symmetry-protected BICs.

Solutions to wave equations usually feature a spectral separation between extended continuum states and spatially localized discrete frequencies. In the early days of quantum mechanics, however, von Neumann and Wigner showed that specific potentials in the Schrödinger equation could result in spatially localized wave functions with energies within the continuous spectrum of extended states (1). These bound states in the continuum (BICs) have been shown to emerge from diffractive interference, making them a generic property of wave equations, including the Maxwell equations in acoustics and photonics (2). BICs have been experimentally realized in photonic systems, where nanofabrication tools enable customization of the energies and symmetries of photonic modes (3–5). Applications such as chiral lasing (6–9), enhanced nonlinear frequency conversion (10–12), and the mitigation of radiation losses in waveguide devices have emerged from this research (13–15). In general, BICs are designed with fine parameter tuning, which enforces localized destructive interference of extended waves (16, 17). Although topological BICs have been realized at corners and edges of acoustic and photonic lattices (18–21), point defects in photonic lattices that give rise to optical BICs protected by lattice symmetries offer a more controllable platform than topological edges (22, 23). These advancements motivate the search for analogous electronic bound states within a metallic continuum in condensed matter systems.

Bound states around defects are ubiquitous in insulators and semiconductors such as $MoS_{2}$ (24, 25), where they exist in a spectral gap between bands. The localization of these states is directly tied to the presence of the bandgap, allowing the defect states to avoid hybridization with continuum states. In metals, however, dilute point defects behave as scattering centers for extended states, which only weakly perturbs them (26, 27). Localized defect states can also emerge in topological insulators, where scattering of the topologically protected surface states occurs, and the defect state lies within the spectral gap of the bulk (28, 29). Many-body interactions such as the Kondo effect (30) can give rise to localized resonances (31–34), but they are typically found near the Fermi level rather than deep within the metallic band. A few studies have reported electronic BICs confined by artificially designed periodic potentials or potential wells in two-dimensional (2D) electron gas systems, such as GaAs (35–37). However, the lack of spatially resolved measurements in these works leaves the claims of spatially localized bound states ambiguous (38). The experimental realization of unambiguously exponentially localized electronic BICs therefore remains an open pursuit.

By analogy to optical BICs, modulating lattice-hopping parameters may be a promising avenue to realize electronic BICs (39). In this work, we report a general mechanism that produces robust BICs in lattices exhibiting flat bands due to frustrated electron hopping between adjacent lattice sites. This frustration occurs in bipartite lattices with an unequal number of sublattice sites, such as the Lieb lattice (40), as well as in line graph lattices, such as the kagome (41) and dice (42) lattices. Frustrated hopping can also result from the interplay of lattice symmetry and orbital composition, such as in the decorated checkerboard lattice (43, 44). In all these lattices, dispersive bands coexist with highly degenerate flat bands, in which the extended Bloch states can be combined into spatially localized eigenstates known as compact localized states (CLSs) (45–47). The formation of electronic BICs can be understood within the following framework (Fig. 1A): A lattice defect shifts the chemical potential of a CLS into the continuum of dispersive bands. Owing to the localized nature of the eigenstates, the more distant CLSs remain largely unaffected, whereas the continuum states are only slightly perturbed. Notably, the orthogonality between the CLS and the dispersive states can be preserved during this shift, which makes the CLS remain perfectly spatially localized without hybridizing with the continuum, forming a BIC. This mechanism is intrinsic to materials hosting nontrivial flat bands (48, 49), enabling the formation of electronic BICs through local vacancies or impurities without requiring fine-tuning model parameters.

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Experimental system

We use scanning tunneling microscopy and spectroscopy (STM and STS) to directly characterize the local density of states (LDOS) of electronic BICs in $Pd_{5}AlI_{2}$ , a van der Waals (vdW) metal with a decorated checkerboard lattice that gives rise to frustrated electron hopping (50). The tetragonal crystal structure of $Pd_{5}AlI_{2}$ (space group I4/mmm) consists of a stack of vdW slabs, each five atoms thick. These slabs can be peeled off the crystal and isolated as air-stable flakes through mechanical exfoliation. Each intermetallic slab is composed of a PdAl checkerboard lattice sandwiched between two square planes of $Pd_{2}$ , capped with iodine atoms (Fig. 1B). Tight-binding modeling of the PdAl layer reveals that it forms a bipartite lattice with frustrated hopping between orthogonal Pd $d_{xz}$ and $d_{yz}$ orbitals, mediated by Al $p_{z}$ orbitals (Fig. 1C) (50). The electronic structure of this Lieb-like lattice, termed decorated checkerboard, has been measured in photoemission experiments and features linearly dispersing bands at high symmetry points (M and $\Gamma$ ), which are intersected by a flat band (50). Figure 1C shows a CLS of this flat band mapped onto the PdAl inner layer of $Pd_{5}AlI_{2}$ . Figure 1D shows atomic resolution STM topography of the surface iodine atoms of a cleaved $Pd_{5}AlI_{2}$ crystal, measured at negative sample bias. The image features a square lattice with an in-plane lattice constant a = 4.05 Å (fig. S1), which is in agreement with single crystal x-ray diffraction (51, 52). Three types of point defects, labeled as i, ii, and iii in Fig. 1D, are observed in relatively high density ( $\sim2.3\times10^{12}~cm^{-2}$ ) across the surface (fig. S2). The tunneling spectrum of $Pd_{5}AlI_{2}$ shows a nonzero density of state (DOS) at all voltages (purple spectrum, Fig. 1E), which is consistent with the metallicity of the material. This spectrum features peaks at +150 mV and +400 mV. We compared quasiparticle interference (QPI) patterns with density functional theory (DFT)-calculated joint density of states (JDOS) to identify the band structure origin of these peaks (fig. S3 and supplementary text). The band structure (fig. S4) shows that the features arise from two distinct phenomena: peak 1 from a change in band curvature near the closing of the $\Gamma$ hole pocket ( $\sim150~meV$ ), and peak 2 from a Lifshitz transition of the band near 400 meV. Notably, STS on type ii defects reveals two additional LDOS peaks at +475 and +620 mV within the continuous metallic bands (green spectrum, Fig. 1E), whereas all other features of the $Pd_{5}AlI_{2}$ spectrum remain unchanged. These additional peaks are absent in tunneling spectra from other defect types (fig. S5).

B

C

Fig. 1. Bound states on defects in $Pd_{5}AlI_{2}$ . (A) Schematic of extended states in a metallic continuum and compact localized states of a flat band. A flat band eigenstate that is pushed into the continuum from the local potential of a defect remains localized because it is orthogonal to the continuum states. (B) Crystal structure of a $Pd_{5}AlI_{2}$ vdW slab, viewed along the ab plane. (C) Top view of the central PdAl checkerboard plane with an overlay showing an atomic orbital representation of the CLS (gray square). Frustrated hopping occurs between orthogonal $Pd\ d_{xz}$ and $d_{yz}$ orbitals, mediated by the Al $p_{z}$ orbital. Blue and red arrows indicate the in-phase and out-of-phase hopping, respectively. (D) Constant current STM topography image of a $16-nm^{2}-by-16-nm^{2}$ area of $Pd_{5}AlI_{2}$ (setpoint: -300 mV, 50 pA), showing surface iodine atoms and three types of point defects. (E) Average tunneling spectrum (setpoint: 150 mV, 30 pA; modulation: 25 mV, 927 Hz) measured on a defect-free region (purple dashed line) and on the type ii defect circled in (D) (green). Two bound states in the continuum emerge on defect ii. Data acquired at a sample temperature of T = 6.7K. dI/dV, differential conductance.

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Spectroscopy of bound states

We identified the defects of interest as Pd vacancies in the central decorated checkerboard PdAl plane by comparing experimental STM topography and DFT simulations at different sample biases (Fig. 2, A and B, and fig. S6). Spectroscopic imaging over the region shown in Fig. 2C reveals a four-lobed pattern around the Pd vacancy at +470 mV, which resembles an atomic d orbital (Fig. 2D). The state at +620 mV appears as a circular pattern that resembles an atomic s orbital (Fig. 2E). By measuring point spectra along the blue line in Fig. 2C, we demonstrate that the states are confined to a subnanometer spatial range (Fig. 2F and DFT calculations in fig. S3), indicating a remarkable localization of both states. Furthermore, the linewidths of these peaks (35 to 47 mV) are exceptionally sharp when compared with tunneling spectra of bound states in semiconductors and even those of bound electrons in molecules and quantum dots (53). The Gaussian lineshapes, unlike lifetime-limited Lorentzians, indicate that extrinsic broadening (e.g., electron-phonon coupling) dominates the measured linewidths, implying a substantially longer intrinsic BIC lifetime (fig. S7) (54). Notably, we observed no defect-induced scattering patterns in large-area spectroscopic imaging at +470 mV, in contrast to the clear interference observed at other biases (fig. S8). This lack of detectable quasiparticle interference is consistent with a BIC that couples exceptionally weakly to continuum states. The combination of discrete energy levels within the metallic band, spatial localization, and lack of scattering suggest that these states are electronically isolated from the metallic continuum, analogous to optical BICs decoupled from the photonic continuum.

Fig. 2. Spectroscopic structure of bound states on Pd vacancies. (A and B) Experimental (purple) and DFT simulated (grayscale) STM topography of $Pd_{5}AlI_{2}$ areas containing a Pd vacancy at (A) negative (-300 mV, 50 pA) and (B) positive (+550 mV, 50 pA) sample bias. (C) 5-nm $^{2}$ -by-5-nm $^{2}$ STM topography of a region containing all three types of defects, where STS maps were acquired. (D and E) Real-space LDOS maps at bias voltages corresponding to the defect-induced peaks in LDOS [(D) = +470 mV; (E) = +620 mV]. Color scale indicates LDOS. Strong features in the DOS are apparent only around the type ii defect and have different orbital-like symmetries at the two quantized energy levels. (F) Line spectroscopy across the region delimited by the blue line shown in (C). The defect states decay within 1 nm from the center of the defect. Data in panels (C) to (F) were acquired with a feedback setpoint of -300 mV, 50 pA. Spectra were acquired with a lock-in modulation of 10 mV, 927 Hz at a sample temperature of 6.7 K. a.u., arbitrary units.

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Modeling the bound states

We turn to the frustrated hopping band structure of the PdAl layer containing this defect to explain the localization effect. The band structure for an idealized decorated checkerboard model with no next-nearest-neighbor hopping is shown in Fig. 3A. In Fig. 3B, we use the simplified three-band model describing Pd $d_{xz}$ and $d_{yz}$ orbitals and Al $p_{z}$ orbitals to compute the DOS spectrum for a 41-by-41 supercell of PdAl, with a single Pd atom removed. This model is inferred from the DFT-based Wannier model that we have previously developed for this material (50). The spectrum around the vacancy shows excellent agreement with experiment, in which two peaks emerge a few hundred milli-electron volts above the Fermi level ( $E_{F}$ ). In these simulations, the widths of these peaks are determined by an arbitrary broadening parameter. These eigenstates are formed by symmetric CLSs in a 3-by-3 grid surrounding the Pd defect (fig. S9). The relative phases of the neighboring orbitals forming the localized states are constrained by the $C_{4}$ symmetry of the system about the vacancy, resulting in four possible eigenstates that we label by their eigenvalue under the $C_{4}$ symmetry operator $\pm1$ or $\pm i$ . When examining the symmetry of the localized states (Fig. 3B), we found that the lower energy state at +400 meV corresponds to the -1 eigenstate, whereas the state at +700 meV corresponds to the +i eigenstate. An additional on-site potential is necessary for the +i state to emerge, which we attribute to p orbitals from the iodine atoms positioned above and below the PdAl checkerboard (fig. S10). These p orbitals are affected by the absence of the Pd orbitals in the plane. By mapping the nodal lines (Fig. 3, C and D), which are defined by $\pi$ -phase shifts of the wave functions, we found that the -1 state features angular nodal planes, forming a four-lobe structure, whereas the +i state has a radial node, resulting in a circular structure. Although individual CLSs are not typically observable in the LDOS, shifting a CLS into the continuum results in a LDOS enhancement confined at the defect site that retains the nodal structure of the CLS wave function. These theoretical results are consistent with experimental spectroscopic imaging (Fig. 3, E and F).

E

Fig. 3. Nodal structures in a frustrated hopping model. (A) Band structure of an idealized decorated checkerboard model where hopping interference leads to a flat band intersected by two linearly dispersing bands. (B) DOS spectra from a simulated 41-by-41 supercell of decorated checkerboard. The spectrum for the 3-by-3 supercell around a Pd vacancy (green) reveals two peaks that are absent in a 3-by-3 supercell without the vacancy (purple). Details of the calculations presented in (A) and (B) can be found in the supplementary text section “Details of tight-binding calculations of Pd vacancies.” (C and D) Schematic of two eigenstates of the 41-by-41 supercell containing a single Pd vacancy. Color wheel indicates the relative phase of Pd d orbitals. Nodal lines (orange dashed lines) emerge where there is a $\pi$ -phase shift of the wave function. The state shown in (D) emerges because of an additional $\sigma_{y}$ transformation from an on-site potential from iodine $p_{x} + ip_{y}$ orbitals (rainbow circle, fig. S10). These eigenstates are combinations of flat band CLSs and thus are also eigenstates of the flat band. They are orthogonal to high-energy dispersive states and remain localized. (E and F) Nodal lines from the tight-binding model overlaid on the experimental spectroscopic maps shown in Fig. 2, D and E, showing qualitative agreement.

To understand whether the perfectly flat band of the ideal decorated checkerboard lattice is a necessary condition to host point defect BICs in $Pd_{5}AlI_{2}$ , we artificially introduced next-nearest-neighbor hopping to our model, which adds dispersion to the flat band. This transformation makes the CLSs not exact eigenstates of the system, and therefore, the defect state can hybridize with the continuum of extended states. However, the exponential localization of the BICs is robust for a large parametric range of next-nearest-neighbor hopping and band dispersion, including realistic parameters that match the experimental band structure of $Pd_{5}AlI_{2}$ (fig. S11) (50). Furthermore, the absence of BICs at other defect types (fig. S5) indicates that perturbing the PdAl frustrated lattice is a necessary condition. To support this, we synthesized $Pd_{5}AlI_{2}$ single crystals doped with a trace amount of Fe, where STM topography reveals substitution at Pd sites within the PdAl checkerboard plane (tables S1 and S2 and figs. S12 to S14). Spectroscopic imaging at these Fe substitution sites identifies BICs, but at different energies than those associated with intrinsic vacancies. Spectroscopic imaging reveals that these states possess the same extent and four-lobed spatial symmetry as the vacancy-induced BIC, confirming that distinct impurity potentials can produce similar BICs on this lattice site (fig. S14). This demonstrates that localization is driven by the topologically nontrivial character of the flat band rather than by a conventional impurity state. These states result from the interference of neighboring orbitals and do not have an analog in isolated orbitals (55–57). Indeed, the atomic orbital-like LDOS patterns observed in Fig. 2, D and E, are noticeably larger than atomic orbitals.

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Dimers of bound states

The resulting electronic BICs resemble atomic orbitals of different symmetries at different energies. Like conventional atomic orbitals, they can bind when in proximity, forming molecular bound states. However, unlike atomic orbitals, their energy splitting into bonding and antibonding orbitals does not need to respect conventional rules. We performed spectroscopic imaging over an area containing two defects separated by a single atomic lattice constant (Fig. 4A). Spatially averaged spectroscopy over this dimer reveals four bound states,

Fig. 4. Dimers of electronic BICs. (A) STM topography of the region containing a divacancy where spectroscopic maps were acquired. (B) Spatially averaged tunneling spectrum over a defect dimer [dashed oval shown in (A)] overlaid with the single defect spectrum from Fig. 1E. (C to F) Real space LDOS maps at bias voltages corresponding to the dimer bound state peaks in (B). (G to J) Schematic of dimer eigenstates formed by combining two vacancy eigenstates. (G) and (I) are combinations where there is a $\pi$ -phase relationship between the two vacancy states. (H) and (J) are combinations of two in-phase defect states (fig. S17). There is qualitative agreement between nodal lines defined in (G) to (J) and the shape of the experimental data. Data were acquired with a feedback setpoint of -400 mV, 50 pA, and lock-in modulation of 5 mV, 1127 Hz at a sample temperature of 6.7K.

corresponding to the splitting of each of the two BICs associated with a single vacancy (Fig. 4B). This splitting is reminiscent of bonding and antibonding energy levels that form in homonuclear diatomic molecules. Consistent with the expectation for bonding in diatomic molecules, spectroscopic imaging of divacancy states of the four-lobed BIC shows a bonding orbital at +440 mV and an antibonding orbital at a higher energy of +510 mV (Fig. 4, C and D). By distinction, the hybridization of the circular states creates a node between the defects, similar to an antibonding molecular orbital, at +590 mV (Fig. 4E). The higher energy state at +650 mV exhibits a high density of states between the defects, resembling a bonding molecular orbital (Fig. 4F). Spectroscopic imaging over an area containing a dimer and an isolated vacancy confirms this energy distribution (fig. S15). When Pd vacancies are separated by two or more atomic lattice constants, interdefect hybridization is not observed, further supporting the strongly localized nature of the BICs (fig. S16). We can describe these dimerized states within the PdAl tight binding model as linear combinations of two single-defect eigenstates (Fig. 4, G to J). In diatomic molecules, bonding orbitals result from favorable phase interactions in the linear combination of atomic orbitals, which make up the molecular orbital with fewer nodes than the antibonding orbital. In this situation, the relative phase of the BIC with respect to its neighbor—i.e., the sign of the linear combination—is the only factor that determines the energy of the bonding and antibonding CLSs (fig. S17). In particular, when two defect states are out of phase with each other, the interaction is favorable and the divacancy state is lower in energy. The dimer states formed by combining two in-phase defect states are higher in energy, regardless of the number of nodes in the resulting structure.

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Discussion and outlook

Using STM and STS, we have demonstrated that electronic bound states form around vacancies within the metallic continuum of $Pd_{5}AlI_{2}$ . This phenomenon arises from electron-hopping interference on the decorated checkerboard of $Pd_{5}AlI_{2}$ , leading to spatially localized eigenstates that are orthogonal to the continuum and strongly resistant to hybridization. Our results show that point defects in $Pd_{5}AlI_{2}$ can host a condensed matter analog of optical BICs. More broadly, our results point to a general mechanism to create BICs in other experimentally realized 2D frustrated hopping lattices, such as the Lieb and kagome lattices (58, 59), where CLSs have been proposed to play a key role in exotic correlated electron phases, including superconductivity, density waves, and magnetism. Our imaging of defect-localized CLSs provides an experimental confirmation of topologically nontrivial localized states caused by orbital interference in frustrated lattices. Furthermore, we have demonstrated that defect dimerization controls the energy of these electronic states and proven that these CLSs are distinct from atomic orbitals. Motivated by recent advances in defect engineering demonstrating the assembly of atomically precise vacancy lattices in vdW materials, such as semimetallic $PtSe_{2}$ (60), we envision that $Pd_{5}AlI_{2}$ could provide a platform for the controllable synthesis of electronic BIC lattices that may host topological properties. Indeed, BICs on defects could enable lossless, defect-mediated transport channels when arranged in lines or lattices. Their coexistence with bulk states offers a rich platform for tuning electronic properties and exploring many-body interactions, including the simulation of Kondo physics (61). By analogy to the topological charges carried by photonic BICs, which are robust to perturbations, our defect BICs emerge from the nontrivial topology of the flat band. The multisite, phase-coherent structure of CLSs allows for precise engineering of lattices or arrays of BICs where the energetics are determined by the phase relationships between CLS wave functions. Such atomically precise topologically nontrivial lattices could enable functionalities in catalysis and energy storage (62). Lastly, the vdW structure of $Pd_{5}AlI_{2}$ provides a path for interfacing with other materials through mechanical exfoliation, stacking, and twisting. Overall, the thermodynamic and kinetic control of defect density and migration, in conjunction with conventional vdW material manipulation, make $Pd_{5}AlI_{2}$ a promising candidate for highly tunable localized states that may be useful for topological quantum chemistry and the study of many-body effects in topological systems.

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ACKNOWLEDGMENTS

The DFT calculations shown in this work have been performed on the Big Red 200 and Quartz supercomputer clusters at Indiana University. Funding: This research on localized states in novel frustrated hopping models is funded by a Brown Investigator Award, a program of the Brown Institute for Basic Sciences at the California Institute of Technology. Synthesis and structural characterization were in part supported by the NSF through the Columbia University Materials Research Science and Engineering Center (MRSEC) on Precision-Assembled Quantum Materials DMR-2011738. STM measurements were funded by the Air Force Office of Scientific Research under award nos. FA9550-22-1-0389 and FA9550-21-1-0378. Synthetic work was also partially supported as part of the Programmable Quantum Materials, an Energy Frontier Research Center, funded by the US Department of Energy (DOE). Office of Science, Basic Energy Sciences, under award DESC0019443. Theoretical efforts at Columbia University were supported by the NSF under award no. DMR-2340394. DFT calculations at Indiana University were supported in part by Lilly Endowment through its support for the Indiana University Pervasive Technology Institute, as well as by Indiana University startup funds. Author contributions: DFT calculations: B.S., A.B.G.; Resources (code): A.D.; STM experiments: M.T., X.H., S.T., H.L., M.H.; Supervision: R.Q., X.R., X.-Y.Z., A.N.P.; Synthesis: D.G.C., C.S.K., W.M.-K., X.R.; Tight-binding calculations: S.E.R., M.T., L.M.N., R.Q.; Writing – original draft: M.T.; Writing – review & editing: all authors. Competing interests: The authors declare that they have no competing interests. Data, code, and materials availability: The raw and processed data of this study are available for download at Zenodo (63). The synthesis of materials used in this study is described in the methods, and in greater detail in Devarakonda et al. (50). Other data needed to evaluate the conclusions in the paper are presented in the paper or the supplementary materials. License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.adt9825

Materials and Methods; Supplementary Text; Figs. S1 to S17; Tables S1 and S2;

References (64–76)

Submitted 18 October 2024; resubmitted 28 August 2025; accepted 14 August 2026

10.1126/science.adt9825

MEMBRANES

Dynamic functionality-enabled fast and selective transport in nanochannels

Hao Zhang $^{1}$ †‡, Yuan Kang $^{2,3*}$ †, Fan Feng $^{4}$ , Ting Hu $^{2}$ , Rongming Xu $^{5}$ , Hang Yu $^{5}$ , Kaiqiang He $^{2}$ , Zhe Yang $^{1}$ §, Zhuyuan Wang $^{1}$ , Cher Hon Lau $^{3}$ , Ze-Xian Low $^{6}$ , Qinfen Gu $^{7}$ , Jefferson Zhe Liu $^{4*}$ , Huanting Wang $^{2}$ , Xiwang Zhang $^{1,8*}$

Nanochannels capable of fast and selective mass transport are central to applications in energy, resources, biomedicine, and the environment. However, extreme nanoscale confinement, often coupled with rigid channel environments imposes substantial frictional and adhesive barriers, causing sluggish transport and constrained selectivity. We identified nanochannel dynamics as a key to addressing these challenges by harnessing the intrinsic mobility (e.g., self-rotation) of confined functionalities to enhance molecular transport. Through a combination of experiments and simulations, we demonstrated that such dynamics reshape transport by promoting kinetic energy transfer and enabling more efficient molecular relays, thereby improving separation performance beyond current benchmarks. Our findings highlight the role of nanochannel dynamics in regulating mass transport under confinement and provide a framework for designing advanced nanochannel systems.

Artificial channels with characteristic sizes down to 1-nm and sub-1-nm regimes are critical for understanding and exploiting mass transport at this scale (1, 2). Such dimensions are commensurate with those of most ions, gases, solvents, and solutes, providing a basis for controllable transport in diverse applications (3–5). Central to this capability are appropriately designed channel geometries (e.g., size) and built-in functionalities (e.g., embedded particles), which discriminate target species through differences in size and chemical affinity while providing directional relays through sequential adsorption-desorption events (hopping) to sustain rapid transport (6–9).

Efforts have therefore focused on refining channel size and functionality design (10–12). Despite being essential for fast and selective transport, these approaches often involve an inherent trade-off between permeability and selectivity (2, 12–14), largely arising from the rigid and spatially constrained nature of most nanochannels. Narrow channel walls and fixed functionalities impose steric hindrance (frictional barriers) to rapid transport (2, 15, 16), whereas strengthened channel-target affinity under nanoconfinement, although beneficial for selectivity, can hinder target migration by deepening local potential wells (adhesive barriers) (17).

In contrast, biological channels, such as membrane proteins, often display exceptional permselectivity. Besides precisely programmed channel geometry and functional motifs, their dynamic flexibility is also considered critical for superior transport properties (18–25). In representative ion (e.g., K channel of Streptomyces A for $K^{+}$ ), solvent (e.g., aquaporin-1 for $H_{2}O$ ), and gas (e.g., ammonium transporter B for $NH_{3}$ ) channels, protein backbones and functional side groups undergo conformational fluctuations, flipping, or rotation (18–23). Despite ultranarrow confinement, these dynamics modulate local energy landscapes and lower transport barriers, enabling ultrafast target permeation while maintaining exceptional selectivity.

Inspired by this principle, we identified nanochannel dynamics as a key to achieving fast and selective transport in artificial channels. We incorporated self-rotating ammonium ions $\left(\mathrm{NH}_{4}^{+}\right)$ into two-dimensional (2D) channels to introduce local dynamics that regulate molecular transport. In addition to repelling competing molecules, these rotatable functionalities accelerate target adsorption-desorption and promote successive hopping through enhanced kinetic energy transfer. In this manner, frictional and adhesive barriers under nanoconfinement can be largely overcome, uniting rapid transport with high selectivity and enabling superior solvent separation performance under practical conditions.

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Design and fabrication of 2D channels with dynamic functionality

Compared with biological channels, artificial nanochannels built from common materials usually lack periodic backbone flexibility. Therefore, we chose to introduce dynamics into nanochannels by incorporating functionalities with rapid self-motion, exemplified by grafting rotating $NH_{4}^{+}$ into 2D $Ti_{3}C_{2}T_{x}$ MXene channels (Fig. 1A and fig. S1). $Ti_{3}C_{2}T_{x}$ are negatively charged and functionalized (-OH, -O, and -F) nanosheets with a high Hamaker constant (figs. S2 and S3). These properties enable their easy stacking into a layered assembly, forming polar, sub-1-nm interlayer channels for stable $NH_{4}^{+}$ anchoring through enhanced hydrogen bonding and electrostatic attraction resulting from the nanoconfinement effect (11, 26). As supported by our density functional theory calculations and ab initio molecular dynamics (AIMD) simulations, $NH_{4}^{+}$ can stably reside within MXene channels through interactions with up to four surface functional groups, with limited positional fluctuations (figs. S4 and S5).

To incorporate $NH_{4}^{+}$ , the as-prepared pristine MXene membrane (untreated-M) in its wet state was exposed to an ammonium chloride ( $NH_{4}Cl$ ) solution to obtain the $NH_{4}^{+}$ -functionalized MXene membrane ( $NH_{4}^{+}-M$ ) (schematic illustration in fig. S6), which showed a defect-free surface and a lamellar cross section (Fig. 1B and fig. S7, A to D). Both high-resolution transmission electron microscopy (HRTEM) and x-ray diffraction revealed well-defined and undisturbed interlayer channels upon $NH_{4}^{+}$ incorporation (fig. S8). X-ray photoelectron spectroscopy (XPS) confirmed $NH_{4}^{+}$ incorporation through the characteristic N signal and showed its uniform distribution across the laminate by depth profiling, consistent with elemental mapping (Fig. 1B and figs. S7, E and F, and S9). Meanwhile, the incorporated $NH_{4}^{+}$ generated a new peak at $1450\ cm^{-1}$ in the Fourier transform infrared spectrum, assigned to the N-H bending vibration, along with a red shift of the O-H stretching vibration from 3470 to $3440\ cm^{-1}$ . These changes imply noncovalent MXene- $NH_{4}^{+}$ interactions through hydrogen bonds and electrostatic attractions (fig. S10), which also endow $NH_{4}^{+}-M$ with improved mechanical properties through versatile cross-linking (fig. S11).

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Fig. 1. Channel characterization and transport properties. (A) Schematic illustration of molecular transport through $NH_{4}^{+}-M$ channels (top) facilitated by self-rotating $NH_{4}^{+}$ (bottom). (B) Scanning electron microscopy (SEM) (top left; scale bar, 250 nm) and HRTEM (bottom left; scale bar, 5 nm) images of $NH_{4}^{+}-M$ , with depth-profiled N 1s XPS spectra (right) showing $NH_{4}^{+}$ distribution from the surface to a depth of 200 nm. Yellow dashed lines in the SEM image indicate the membrane thickness. The white dashed box in the HRTEM image indicates the region enlarged in the inset, where the yellow lines highlight the interlayer channels. (C) Solvent vapor permeance through untreated-M and $NH_{4}^{+}-M$ . (D) ${}^{1}H$ VT-NMR spectra of nanoconfined $NH_{4}^{+}$ within $NH_{4}^{+}-M$ and free $NH_{4}^{+}$ in the solution. a.u., arbitrary units; ppm, parts per million. (E) Water flux through untreated-M, $ND_{4}^{+}-M$ , $NH_{4}^{+}-M$ , and mix-M ( $NH_{4}^{+}/ND_{4}^{+}$ molar ratio = 1:1). (F) ${}^{1}H$ time-domain NMR spectra of untreated-M, $ND_{4}^{+}-M$ , and $NH_{4}^{+}-M$ . (G) PFG-NMR spectra of bulk water, untreated-M, $ND_{4}^{+}-M$ , and $NH_{4}^{+}-M$ . (H) Water self-diffusion coefficients in the bulk and confined states derived from PFG-NMR spectra.

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The role of functionality rotation

The impact of $NH_{4}^{+}$ functionalities on mass transport was assessed by measuring the permeance of representative solvents, including water, ethanol, isopropanol, and ethyl acetate, through the untreated-M and $NH_{4}^{+}-M$ channels (Fig. 1C and fig. S12). Both channels had similar solvent-accessible sizes under the same solvent environment (fig. S13). However, larger solvents, such as ethanol, permeated markedly more slowly through $NH_{4}^{+}-M$ than through untreated-M, consistent with the conventional view that introduced functionalities usually impose additional steric hindrance in nanochannels (13, 26). Unexpectedly, this substantial crowding by $NH_{4}^{+}$ (around 3 Å) accelerated water diffusion, increasing the permeation rate from 1.5 to 2.2 mol m $^{-2}$ h $^{-1}$ kPa $^{-1}$ , almost equaling open-air water evaporation rates (2.4 mol m $^{-2}$ h $^{-1}$ kPa $^{-1}$ ). This enhanced water permeation was also verified by single-component pervaporation tests of liquid water, in which the channel was in direct contact with the liquid (fig. S14). Likewise, $NH_{4}^{+}-M$ achieved a 70% increase in water flux, while differences in channel width and its distribution were excluded as contributing factors (figs. S15 and S16). This enhancement was also consistently observed across $NH_{4}^{+}-M$ membranes of different thicknesses (fig. S17).

We attributed this unusual transport acceleration to the rotational dynamics of $NH_{4}^{+}$ . Unlike static functional groups, $NH_{4}^{+}$ exhibits ultrafast rotation in a few polar solvents, such as water, rotating by an angle of $33^{\circ}$ within 1.1 ps (rotational correlation time, $\tau_{c}$ ), because of its tetrahedral N-H configuration (27, 28). It forms a mobile inner hydration shell comprising four hydrogen-bonded water molecules and a fifth that continuously exchanges with them (Fig. 1A) (29, 30). Such dynamics produce angular jumps that rotate the hydrated $NH_{4}^{+}$ and drive presumably adjacent water molecules forward. The dynamics of $NH_{4}^{+}$ within MXene channels were probed by ${}^{1}H$ variable-temperature nuclear magnetic resonance (VT-NMR) (Fig. 1D) (31). The absence of peak decoalescence across the tested temperature range indicates that $NH_{4}^{+}$ retains fast local averaging under nanoconfinement, whereas the weak temperature dependence of the linewidth is more consistent with rotational dynamics than proton exchange (32). Together with the restricted translational motion of $NH_{4}^{+}$ evidenced by AIMD simulations (fig. S5), these results support persistent $NH_{4}^{+}$ rotation within MXene channels.

On the basis of these results, we validated the transport-enhancing role of $NH_{4}^{+}$ rotation by correlating its rotational velocity with water permeation rates. We substituted hydrogen (H) in $NH_{4}^{+}$ with deuterium (D) to obtain MXene channels functionalized with $ND_{4}^{+}$ (referred to as $ND_{4}^{+}-M$ ) and an $ND_{4}^{+}-NH_{4}^{+}$ mixture (molar ratio 1:1, referred to as mix-M) (Fig. 1E). Unlike other ionic functionalizers (e.g., $K^{+}$ ; fig. S18 and table S1), $ND_{4}^{+}$ is an isotopic analog of $NH_{4}^{+}$ with similar physicochemical properties, thus resulting in nearly identical channel characteristics (fig. S19). However, the heavier deuterium gives $ND_{4}^{+}$ a higher moment of inertia and therefore a rotational angular velocity theoretically lower than that of $NH_{4}^{+}$ by a factor of $\sqrt{2}$ at the same temperature (supplementary text). Our results indeed revealed a strong dependence of water transport on the rotational velocity of $NH_{4}^{+}$ , as evidenced by the lower water flux of $ND_{4}^{+}-M$ (808 g m $^{-2}$ h $^{-1}$ ) compared with mix-M (1070 g m $^{-2}$ h $^{-1}$ ) and $NH_{4}^{+}-M$ (1145 g m $^{-2}$ h $^{-1}$ ), implying the direct positive impact of $NH_{4}^{+}$ rotation on water transport.

These results were further corroborated by spin-spin relaxation time $(T_{2})$ analysis in ${}^{1}H$ time-domain NMR (Fig. 1F), which distinguishes $NH_{4}^{+}$ -bound water ( $10^{2}$ ms range) and free water ( $10^{3}$ ms range). $NH_{4}^{+}$ -M exhibited the longest $T_{2}$ in both regimes, followed by $ND_{4}^{+}$ -M and untreated-M, indicating enhanced mobility of confined water with faster functionality rotation (33). Consistently, pulse-field gradient-stimulated-echo NMR (PFG-NMR) analysis revealed enhanced water mobility in $NH_{4}^{+}$ -M, with a self-diffusion coefficient of $2.47 \times 10^{-9}$ $m^{2}$ $s^{-1}$ , higher than those of $ND_{4}^{+}$ -M ( $2.09 \times 10^{-9}$ $m^{2}$ $s^{-1}$ ) and untreated-M ( $2.01 \times 10^{-9}$ $m^{2}$ $s^{-1}$ ), approaching that of bulk water (Fig. 1, G and H) (4). This isotope-dependent enhancement further supports the kinetic role of $NH_{4}^{+}$ rotation in confined-water transport.

Because $NH_{4}^{+}$ functionalization could also potentially regulate solvent transport by altering solvent sorption within the channels (2, 34), we measured solvent uptake by untreated-M and $NH_{4}^{+}-M$ in both gaseous and liquid states (figs. S20 and S21). These measurements showed that $NH_{4}^{+}$ incorporation had negligible, if not negative, effects on water and ethanol uptake, largely excluding enhanced sorption as the origin of increased water permeation. Channel surface free energy also showed minimal changes in dispersive and polar components after $NH_{4}^{+}$ functionalization (supplementary text and fig. S22). These results indicate that the enhanced water flux arises from accelerated transport kinetics rather than changes in solvent sorption or partitioning.

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The role of functionality interconnection

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To further probe how rotating $NH_{4}^{+}$ regulates transport, we varied its distribution by tuning its loading within the channels. The equilibrium $NH_{4}^{+}$ content in $NH_{4}^{+}-M$ was reflected by the molar ratio of N-H in $NH_{4}^{+}$ to -F on the MXene channel walls (N-H/-F), which increased from 0 to 0.46, 0.78, and 1.01 with increasing $NH_{4}^{+}$ loading (fig. S23). This led to a gradual channel contraction from 5.3 to 4.9 Å (fig. S24). Consequently, ethanol permeation progressively slowed down, whereas water flux continued to increase and exhibited a pronounced jump when the ratio exceeded 0.78 (Fig. 2A). These trends indicate that the transport-regulating role of $NH_{4}^{+}$ remains effective across both sparsely and densely populated states. In particular, this water transport enhancement becomes pronounced when the rotating $NH_{4}^{+}$ reaches saturation, suggesting cooperative transport effects among neighboring functionalities, a phenomenon associated with their interconnection (17, 35).

To determine the critical distance below which neighboring $NH_{4}^{+}$ sites can interconnect with each other, we investigated the structure of hydrated $NH_{4}^{+}$ using the radial distribution function (RDF) in molecular dynamics (MD) simulations (Fig. 2B), which revealed a well-defined inner hydration shell around $NH_{4}^{+}$ with a radius of 3.7 Å, corresponding to a critical distance of 7.4 Å. Meanwhile, we calculated the average spacing between neighboring $NH_{4}^{+}$ sites at varying N-H/-F ratios (Fig. 2C and supplementary text) and compared it with this distance. With increasing $NH_{4}^{+}$ loading, the average inter- $NH_{4}^{+}$ distance decreased rapidly from 9.1 Å (ratio = 0.46) to 7.5 Å (ratio = 0.78) and further dropped to 6.7 Å (ratio = 1.01) to allow interconnection. This process was also visualized by mapping the distribution of hydrated $NH_{4}^{+}$ in the channel (Fig. 2, D to F). As the channel was crowded with more $NH_{4}^{+}$ , their hydration shells gradually overlapped, eventually forming interconnected pathways from channel entry to exit. Consistently, coupled atomic force microscopy and infrared spectroscopy measurements provided additional evidence for the formation and interconnection of water clusters around $NH_{4}^{+}$ under humid conditions (fig. S25).

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Fig. 2. Interconnection of dynamic functionalities in nanochannels. (A) Water and ethanol permeation fluxes through $NH_{4}^{+}-M$ with varied $NH_{4}^{+}$ coverage (represented by the N–H/F molar ratio). (B) N–O RDFs of water molecules surrounding $NH_{4}^{+}$ within water-equilibrated $NH_{4}^{+}-M$ channels at different $NH_{4}^{+}$ coverage. The inset highlights the critical inter- $NH_{4}^{+}$ distance for $NH_{4}^{+}$ interconnection. (C) Average inter- $NH_{4}^{+}$ distances as a function of the N–H/F molar ratio. The inset illustrates the definition of the inter- $NH_{4}^{+}$ distance. (D to F) Visualization of water cluster distributions within water-equilibrated $NH_{4}^{+}-M$ channels at N–H/F molar ratios of 0.46 (D), 0.93 (E), and 1.39 (F). For each case, the top and bottom panels present side-view and top-view presentations of the channel, respectively.

Collectively, these observations underscore the role of $NH_{4}^{+}$ interconnection in regulating solvent transport, particularly water transport. Although individual rotating $NH_{4}^{+}$ promotes local water passage, interconnected $NH_{4}^{+}$ further accelerates transport by linking discrete water domains into extended fluidic pathways that enable more continuous and directional water propagation than in an unfunctionalized region.

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Dynamic functionality-enabled transport mechanisms

We used MD simulations to elucidate the synergistic impact of functional rotation and interconnection on mass transport. Three types of MXene channels were constructed: (i) no $NH_{4}^{+}$ , (ii) fixed $NH_{4}^{+}$ (fully immobilized), and (iii) pinned-site $NH_{4}^{+}$ with orientational mobility (translation suppressed, but rotation allowed). Water transport and ethanol transport were evaluated at varying $NH_{4}^{+}$ loadings. Compared with the $NH_{4}^{+}$ -free case, functionalized channels presented three trends consistent with experiments. First, the status of $NH_{4}^{+}$ mobility strongly influenced water transport, with fixed $NH_{4}^{+}$ impeding permeation as a “barrier,” whereas rotating $NH_{4}^{+}$ nearly doubled the permeation rate as a “facilitator” (Fig. 3A). Second, increasing $NH_{4}^{+}$ loading potentially amplified these opposing effects, most prominently at saturation (N-H/-F ≈ 1.39) (Fig. 3B). Third, $NH_{4}^{+}$ functionalization, regardless of its mobility, always reduced ethanol permeation (Fig. 3C).

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To explain the unusual water transport, we first revisited the classic “functionality (carrier)–mediated” transport theory, which describes molecular migration between carriers in three stages (Fig. 3D and fig. S26) (8, 9). This process comprises (i) capture and release, where a molecule associates with the first carrier, reorients, and dissociates; (ii) hopping, during which the dissociated molecule diffuses toward a neighboring carrier; and (iii) recapture and relay, where it is rebound by the second carrier to complete this transport cycle. Our analysis revealed that rotating $NH_{4}^{+}$ reshaped water transport across all three stages, extending this classic theory to dynamic carriers. In stage 1, they accelerated the capture-release process by shortening the water-retention time at each site, as quantified by the $NH_{4}^{+}$ hydration-shell lifetime, a proxy for local water-exchange rates. As shown in Fig. 3E, the distribution of hydration-shell lifetimes shifted toward shorter times for rotating $NH_{4}^{+}$ (0 to 10 ps), whereas fixed $NH_{4}^{+}$ favored longer-lived shells (10 to 40 ps). The corresponding mean lifetime decreased from 8.3 to 6.1 ps, indicating that $NH_{4}^{+}$ reduced local trapping and increased water-exchange turnover at each site.

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Fig. 3. Dynamic functionality-mediated transport mechanisms. (A) Water permeation through channels featuring no $NH_{4}^{+}$ , fixed $NH_{4}^{+}$ , or rotating $NH_{4}^{+}$ over time. (B) Water permeation through channels with different $NH_{4}^{+}$ coverage. (C) Ethanol permeation through channels without $NH_{4}^{+}$ and with fixed or rotating $NH_{4}^{+}$ over time. (D) Schematic illustration of $NH_{4}^{+}$ -enabled molecular transport behavior in confined channels. (E) Lifetime distribution of water molecules surrounding fixed or rotating $NH_{4}^{+}$ within channels. (F) Representative trajectories of water molecules within channels containing fixed or rotating $NH_{4}^{+}$ . Each curve represents an individual water molecule, and the color evolution along the trajectory at 1-ps intervals indicates the temporal progression of its motion through the channel. (G) Probability of consecutive $NH_{4}^{+}$ -water collisions during water transport within channels featuring fixed or rotating $NH_{4}^{+}$ (in both interconnected and partially functionalized cases). The inset shows the corresponding probability of overall $NH_{4}^{+}$ -water collisions.

The brief $NH_{4}^{+}$ -water contact events (hereafter referred to as collisions) reshape stage 2 water motion through transient energy and momentum redistribution. Analysis of the net postcollision change in the translational kinetic energy of tagged water molecules reveals a contrast between the two limiting cases (fig. S27). Collisions with fixed $NH_{4}^{+}$ produce only a negligible net effect on water kinetic energy, whereas collisions with rotating $NH_{4}^{+}$ lead to a substantial positive kinetic-energy gain (19.1%). Thus, $NH_{4}^{+}$ rotation promotes transient kinetic-energy transfer to permeating water during close encounters. This additional energy translated into higher initial hopping velocities (0.68 versus 0.26 nm ps $^{-1}$ ) and longer single-step displacements, as revealed by trajectory mapping (Fig. 3F and fig. S28A). Consequently, the random back-and-forth motion of water molecules was reduced, and the total travel path length decreased from 24.3 nm to 16.3 nm, indicating more directional transport (fig. S28B). Moreover, variable-temperature MD revealed a dependence of water permeation rates on $NH_{4}^{+}$ rotational speed, further supporting this kinetic energy transfer mechanism (fig. S29).

In addition, $NH_{4}^{+}$ rotation and interconnection complement each other to enhance water recapture in stage 3. Because water release and hopping are stochastic, recapture by downstream $NH_{4}^{+}$ is inherently limited. Our tracking of $NH_{4}^{+}$ -water collision events during the simulation found that overall collision probability peaked at 26.8% when $NH_{4}^{+}$ sites were both rotating and fully interconnected (Fig. 3G, inset). By contrast, fixing $NH_{4}^{+}$ reduced this probability to 22.3%, possibly because suppressed configurational fluctuations reduced its effective contact cross section with water. Likewise, partly removing $NH_{4}^{+}$ from the channel caused a further drop, to 9.3%, as increased intersite spacing extended hopping distances and reduced contact frequency.

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More importantly, rotation and interconnection increased the probability of successive $NH_{4}^{+}$ -water collisions within the channel. As illustrated in Fig. 3G, water in the rotating and interconnected system exhibited the highest probability (43%) of multiple collisions (1 < n < 10), compared with 36 and 40% for the fixed and partially functionalized systems, respectively. Collectively, these results demonstrate that the rotational and cooperative dynamics of $NH_{4}^{+}$ transform these functionalities from otherwise passive barriers into active carriers, enabling a fast molecular relay along the nanochannel. In contrast, ethanol transport remained consistently suppressed because $NH_{4}^{+}$ -induced steric hindrance excluded most ethanol at the channel entrance and retarded its passage through the channel.

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Dynamic functionality-enabled solvent separations

We then examined how the rotation-dependent transport features of $NH_{4}^{+}-M$ could mitigate the permeability-selectivity trade-off in realistic solvent separations (36). Using 90 wt % ethanol-water mixtures as a model system (fig. S30), we found that $NH_{4}^{+}-M$ increased the water flux from 985 to 1422 g m $^{-2}$ h $^{-1}$ while suppressing ethanol flux from 39 to 4 g m $^{-2}$ h $^{-1}$ , yielding a separation factor of about 4000, more than an order of magnitude higher than that of untreated-M (240; fig. S31A). This selectivity was retained at different operating temperatures and feed compositions, demonstrating consistent performance (fig. S31, B and C).

Azeotropic mixtures, which are industrially challenging to separate by conventional distillation, offer a stringent benchmark for assessing membrane performance. When tested with a 95 wt % ethanol-water azeotrope, $NH_{4}^{+}-M$ achieved a separation factor of 3860, far surpassing the value of 167 obtained for untreated-M (Fig. 4A). Comparable trends were observed for isopropanol-water and ethyl acetate–water mixtures (Fig. 4, B and C), where water permeation was promoted, whereas organic solvent transport was effectively suppressed. Meanwhile,

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Fig. 4. Separation performance. (A to C) Solvent-water separation performance of untreated-M and $NH_{4}^{+}-M$ in treating near-azeotropic mixtures including (A) 95 wt % ethanol-water at $40^{\circ}C$ , (B) 90 wt % isopropanol-water at $40^{\circ}C$ , and (C) 94 wt % ethyl acetate–water at $50^{\circ}C$ . (D) Long-term operational stability of $NH_{4}^{+}-M$ in treating a 95 wt % ethanol-water mixture. (E) Comparison of the ethanol-water separation performance of $NH_{4}^{+}-M$ with reported membranes.

$NH_{4}^{+}-M$ exhibited robust structural and chemical stability (figs. S15, S32, and S33), delivering consistent separation performance over long-term continuous operation under water-ethanol binary conditions (Fig. 4D) and under industrially relevant, impurity-containing conditions (fig. S34). Collectively, these results demonstrate that membranes displaying dynamic functionalities can be applied to practical dehydration processes with improved energy efficiency (fig. S35).

The dynamic functionality strategy was extended to graphene oxide (GO) membranes (fig. S36). Despite a slight reduction in channel width (10.5 to 9.2 Å), $NH_{4}^{+}$ -functionalized GO exhibited enhanced water transport and hindered ethanol permeation (fig. S37), consistent with the transport mechanism identified in MXene systems. Finally, comparison with state-of-the-art polymeric, 2D, mixed-matrix, and commercial membranes confirmed that $NH_{4}^{+}-M$ , when operating at low-to-moderate temperatures, outperformed the conventional permeability-selectivity upper bound (Fig. 4E and table S2).

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Conclusions

We identify nanochannel dynamics as a promising avenue for transport control beyond channel geometry and surface chemistry. Harnessing the intrinsic mobility of functionalities, exemplified by self-rotating $NH_{4}^{+}$ , converts static channels into dynamic transport environments, enabling fast and selective subnanometer transport. These dynamics enhance energy transfer and successive molecular hopping, extending carrier-mediated transport theories developed largely for static functionalities and enabling solvent separations beyond the conventional permeability-selectivity trade-off. Beyond rotation, this principle can extend to functionalities with translational or vibrational freedom, offering a modular route to tune nanoconfined transport (1, 37). Combined with other dynamic building blocks (37, 38), it could enable tailored transport in nanofluidic devices, separation membranes, and ionic conductors.

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ACKNOWLEDGMENTS

We thank J. Wu (Instrumental Analysis Center, SJTU) and R. Gao (Instruments Center for Physical Science, USTC) for their assistance with NMR measurements and valuable discussions. We also acknowledge the use of the facilities and the assistance of J. Ma at the Monash X-ray Platform. H.Z. thanks the China Scholarship Council and the University of Queensland for his scholarships. This work was also supported by resources provided by ANSTO, the Monash Centre for Electron Microscopy, and the Centre for Microscopy and Microanalysis at the University of Queensland. Funding: Y.K. and C.H.L. thank the European Union's Horizon 2024 research and innovation program under Marie Skłodowska-Curie grant agreement no. 101203526. C.H.L. acknowledges funding from EPSRC for his EPSRC Fellowship (EP/X042286/1). X.Z. thanks the Australian Research Council for his ARC Future Fellowship (FT210100593) and the ARC Centre of Excellence for Green Electrochemical Transformation of Carbon Dioxide (CE230100017). J.Z.L. and F.F. thank the Australian Research Council for the ARC Future Fellowship (FT220100149). Author contributions: Conceptualization: H.Z., Y.K., X.Z.; Formal analysis: H.Z., Y.K., F.F., T.H., J.Z.L., H.W., X.Z.; Funding acquisition: Y.K., C.H.L., J.Z.L., X.Z.; Investigation: H.Z., Y.K., F.F., T.H.; Methodology: H.Z., Y.K., T.H., R.X., H.Y., K.H., Z.Y., Z.W.; Project administration: Y.K., J.Z.L., X.Z.; Resources: R.X., H.Y., C.H.L., Z.-X.L., Q.G., X.Z.; Software: F.F., T.H., Q.G., J.Z.L.; Supervision: Y.K., J.Z.L., X.Z.; Validation: H.Z., Y.K., Q.G., J.Z.L.; Visualization: H.Z., Y.K., R.X.; Writing – original draft: H.Z., Y.K.; Writing – review & editing: Y.K., Z.-X.L., J.Z.L., H.W., and X.Z. Competing interests: The authors declare that they have no competing interests. Data, code, and materials availability: All data are available in the main text or the supplementary materials. Details for the synthesis and characterization of all materials are provided in the supplementary materials. License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.aed8319

Materials and Methods; Supplementary Text; Figs. S1 to S37; Tables S1 and S2;

References (39–104)

Submitted 11 November 2025; accepted 25 August 2026

2D MATERIALS

Visualizing symmetry-broken Chern insulators and their quantum melting

Minhao He $^{1\dagger}$ , Yen-Chen Tsui $^{1\dagger}$ , Ran Peng $^{2}$ , Kenji Watanabe $^{3}$ , Takashi Taniguchi $^{4}$ , Oskar Vafek $^{2,5}$ , Ali Yazdani $^{1*}$

In the presence of a magnetic field, electronic states of moiré quantum materials develop a Hofstadter spectrum that provides a distinctive setting for studying the interplay between band topology and strong electron-electron interaction. Using scanning tunneling microscopy, we studied Hofstadter's states in bilayer graphene aligned with hexagonal boron nitride and directly visualized the formation of interaction-driven symmetry breaking Chern insulators. Our measurements revealed the formation of phases that double, triple, or quadruple the moiré unit cell at fractional filling of the Hofstadter bands as well as states with complex intra-unit cell wave functions. We visualized two distinct quantum phenomena in different Chern states, including quantum melting driven by the appearance and proliferation of topological defects and a quantum transition co-occurring with phase competition and separation.

The interplay between magnetic fields and lattice periodicity gives rise to fractal energy bands, as first predicted by Hofstadter (1). Originally proposed in electronic systems, the Hofstadter's model has since been realized in a wide range of experimental platforms, such as waveguide array (2), optical lattice (3, 4), superconducting qubit chain (5), or GaAs/AlGaAs heterostructure by fabricating lateral artificial superlattice (6). Moiré superlattices in stacked van der Waals materials, formed by twist or lattice mismatch, provide an ideal platform for studying the Hofstadter's spectrum and its topology. Early experiments (7–9) have demonstrated that topological states, called Chern insulators (CIs), emerge when the Hofstadter subbands are filled up to a single particle gap. Each CI can be described by two quantum indices: the Chern number C (10) and the band filling index s (11). The fractal Hofstadter energy spectrum giving rise to these incompressible states has recently been detected using scanning tunneling spectroscopy (STS) (12).

Unusual correlated and topological phases (13, 14) emerge at partial fillings of the Hofstadter subbands when their bandwidth becomes narrow and comparable with Coulomb interaction. In this situation, topological invariants (C and/or s) alone do not offer a complete description, because they are insensitive to presence of any broken symmetries. As a result, fundamentally distinct many-body states can share identical topological indices while differing in their underlying microscopic symmetry structures. Theoretical predictions of strongly interacting Hofstadter's states include two possible ground states: incompressible states with quasiparticles associated with fractional charges (15–18) and phases that break the moiré translational symmetry (19). Despite their presence in various graphene-based moiré materials (13, 14, 20–23), there has been no microscopic study of the wave functions and symmetries of these strongly interacting Hofstadter states (24). An equally important open question is the nature of the quantum phase transitions that drive the loss of broken symmetry or topological order of such phases.

Recent scanning tunneling microscopy (STM) measurements have demonstrated the capability of imaging delicate electronic phases with minimal tip-sample work function mismatch (25–27). In this work, we report direct imaging of the symmetry broken Hofstadter's states and visualize their associated quantum melting in Bernal-stacked bilayer graphene (BLG) fully aligned with hexagonal boron nitride (h-BN) using STM. We used spectroscopic measurements to identify various CI insulating phases (by measuring their C and s) and found symmetry-broken Chern insulators (SBCIs) that either double, triple, or quadruple the moiré unit cell, some with intricate intra-unit cell structures. Our approach can be applied to also directly visualize the process of quantum melting of SBCIs and CIs that has remained inaccessible to macroscopically averaged techniques.

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Moiré superlattice and the emergence of Hofstadter states

The BLG devices studied here are fully aligned with the h-BN substrate. Figure 1A shows a typical constant current topographic image within an ultraclean area, with an extracted moiré periodicity $\lambda$ of $14.28\mathrm{nm}$ , consistent with superlattice periodicity of a fully aligned BLG/h-BN (28, 29). A flux ratio as large as $\phi/\phi_0 \approx 0.6$ was reached at perpendicular magnetic field $B = 14\mathrm{T}$ , enabling real-space imaging of electronic wave functions in the fractal Hofstadter's spectrum. Here, $\phi = B\left(\sqrt{3} \times \lambda^2/2\right)$ is the magnetic flux through one moiré unit cell, and $\phi_0 = h/e$ is magnetic flux quantum, where $h$ is Planck's constant and $e$ is the elementary charge.

In Fig. 1B, we show STS as a function of gate voltage $V_{G}$ measured in this region at B = 13.8 T. Similar to previous work on misaligned BLG/hBN samples (26) [fig. S1, section S1 (30)], a strong intrinsic displacement field ( $D_{0}$ ) in our devices (hBN on only one side of BLG) lifts the layer degeneracy of the eight lowest Landau levels (LLLs) and favors filling the bottom layer polarized (hBN proximate) LLs first. Being further from the tunneling tip, this makes the spectral weight at $V_{G} < 0$ weaker than at $V_{G} > 0$ . Nevertheless, we observed substantial differences from the hBN misaligned samples, including a series of additional incompressible states (Fig. 1B). When the electrons were polarized to the bottom layer ( $V_{G} < 0$ ), we observed sharp peak energy shifts (also visible in remote bands) signifying chemical potential jumps across incompressible states at carrier densities distinct from the quantum Hall ferromagnets at LL filling factor $v_{LL} = -3$ , -2, -1 [Fig. 1B and fig. S2, section S2 (30)]. These states highlight the strong moiré effect that arises when electrons are polarized close to the moiré interface and can be assigned to CIs in the Hofstadter spectrum. This is further supported by the CIs are only observed above B = 6 T [fig. S3, section S3 (30)]. When the electrons were polarized to the top layer ( $V_{G} > 0$ ), we still observed the additional Hofstadter's states but with much weaker spectral features [fig. S4, section S4 (30)], indicating a less pronounced moiré effect.

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Identifying CIs

We first identified each CI by determining their quantum indices: C and s. We closely inspected the Hofstadter states at $V_{G} < 0$ , focusing on the spectral features near the Fermi level (bias voltage, $V_{B} = 0$ ). The incompressible gaps were identified as peaks in the tunneling threshold gap $\Delta_{t}$ defined with an onset tunneling current [fig. S5, section S5 (30)]. We performed magnetic field-dependent STS to construct the Wannier diagram (Fig. 1C), a plot of carrier density n versus magnetic flux per moiré unit cell $\phi/\phi_{0}$ in which each incompressible state follows a straight line (figs. S6 and S7). From the slope and intercept of these lines, we determined the Chern number C and band-filling index s using the Diophantine relation $n/n_{s} = C\phi/\phi_{0} + s$ . Here, $n_{s} = 1/(\sqrt{3} \times \lambda^{2}/2)$ is the carrier density corresponding to one electron per moiré unit cell with periodicity $\lambda$ . Our measurements spanned a large range of magnetic fields, notably in the vicinity of magnetic flux ratio $\phi/\phi_{0} = 1/2$ , where we observed spectral features of a dispersive Hofstadter subbands, as predicted [fig. S8, section S6 (30)]. We classified the observed states [fig. S9, section S7 (30)] and summarized a full phase diagram in Fig. 1C, including similar measurements performed at $V_{\mathrm{G}} > 0$ (figs. S10 and S11).

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Fig. 1. Spectroscopic studies of Hofstadter's spectrum in Bernal-stacked bilayer graphene/hBN heterostructure. (A) A clean topograph of a device with periodic structure of bilayer graphene/hBN moiré. The black scale bar is 50 nm. The inset shows the Fourier transform of the topography map. The Bragg peaks of the moiré are marked by red circles, and the corresponding periodicity is 14.28 nm. The white scale bar of the inset is 0.5 nm $^{-1}$ . (B) A density (tuned by gate voltages $V_{G}$ )-dependent STS measured at B = 13.8 T, $\phi/\phi_{0} = 0.588$ . The vertical axis is the tip bias voltage $V_{B}$ , where it probes the electron (hole) excitation at $V_{B} > 0$ ( $V_{B} < 0$ ). On $V_{G} > 0$ ( $V_{G} < 0$ ), the electrons are away from (close to) moiré. The insulating gaps can be identified as gap opening at the Fermi level. Gaps opening at $V_{G} > 0$ are asymmetric to $V_{G} < 0$ with respect to the charge neutrality. The top horizontal axis shows the LL filling factor $v_{LL}$ . dl/dV, differential conductance (see materials and methods for details). (C) Wannier diagram of the insulating phases observed in density $n/n_{s}$ -dependent STS as a function of $\phi/\phi_{0}$ (for $\phi/\phi_{0} > 1/2$ ). The topological indices (C, s) are listed above and are characterized by formula $n/n_{s} = C\phi/\phi_{0} + s$ . The colored lines represent the corresponding (C, s) states, and the orange points represent the data points. All data were collected at effective temperature $T_{eff} = 210$ mK. IQH, integer quantum Hall gap; FQH, fractional quantum Hall gap. (D) An illustration of the dispersive band structure at $\phi/\phi_{0} = 1/2$ . Two identical magnetic subbands, which are enforced by the magnetic translational symmetry, are shown. (E) As the flux increased further for $\phi/\phi_{0} > 1/2$ , the minimum of each magnetic subband formed LLs. Here, for the (C, s) = (-2, 1) state, the lowest two degenerate LLs were fully filled (black dots mean fully filled at field B). (F) When we half-filled the lowest two degenerate LLs, an interaction-driven SBCI state (C, s) = (-1, 1/2) was formed by spontaneously breaking the moiré translational symmetry.

The moiré potential impacts mostly the phase diagram at $V_{G} < 0$ , where the carrier density is tuned in the layer closest to the moiré potential. In this regime, we observed four sets of CIs that followed the sequence $(C, s) = [-2(N + s_{0}), N](N = 0, 1, \ldots)$ , with each set crossing $\phi/\phi_{0} = 1/2$ at a different density $-s_{0} = 0, -1, -1.5$ , and -2. These CIs can be understood as arising from the Landau quantization of the maxima or minima of dispersive magnetic subbands at $\phi/\phi_{0} = 1/2$ (Fig. 1, D and E). In other words, when the flux $\phi$ is shifted from half flux quantum, electron orbits near the extrema of these dispersive magnetic subbands become quantized into LLs according to the detuned flux ratio $\delta\phi = \phi/\phi_{0} - 1/2$ . The magnetic subbands at $\phi/\phi_{0} = 1/2$ can be constructed using the eigenfunctions of magnetic translation group (MTG) (3I). In general, for flux $\phi/\phi_{0} = p/q$ with Landau gauge $\mathbf{A} = (0, Bx, 0)$ , the magnetic lattice momentum is written as $k = k_{1}g_{1} = k_{2}g_{2}$ , where $k_{1} \in [0, 1)$ and $k_{2} \in [0, 1/q)$ . The discrete magnetic translation symmetry of the moiré superlattice requires the energy of subbands to be degenerate under $k_{1} \to k_{1} + 1/q$ [section S8 (30)]. Therefore, at flux $\phi/\phi_{0} = 1/2$ , the magnetic subbands and the LLs that emerge when flux is shifted away from half flux are twofold degenerate as long as the translation symmetry is preserved (3I) (Fig. 1D). This in turn explains why the Chern numbers of translation symmetry preserving states in each set differ from each other by even integers. To demonstrate this point, consider depleting two LLs emanating from the maxima of the charge neutrality point valance subbands at half flux, as in the schematic in Fig. 1E. The filling of such a state is $n / n_{\mathrm{s}} = -2\delta \phi = -2(\phi /\phi_0 - 1 / 2)$ , corresponding to $(C,s) = (-2,1)$ (Fig. 1E). More generally, depleting $2N$ such LLs gives the sequence $(-2N,N)$ . The sequences with nonzero $s_0$ can be similarly understood as first placing the Fermi level inside the Chern $-2s_0$ gap between the dispersive subbands at half flux and then depleting $2N$ half flux-shifted LLs. The filling of such a state is then $n / n_{\mathrm{s}} = -2s_0\phi /\phi_0 - 2N(\phi /\phi_0 - 1 / 2)$ , resulting in observed sequence $(C,s) = [-2(N + s_0),N]$ . Note that because each subband carries an integer Chern number, $2s_0$ is an integer (which can be even or odd).

More notably, we also observed interacting Hofstadter states with integer C but fractional s (13, 14). Plausible ground-state candidates for these states include charge density waves (CDWs) with broken moiré translation symmetry (14, 21–23). With translation symmetry broken in one direction, the degeneracy between the states at $k_{1}$ and $k_{1} + 1/2$ is lifted, which allows a single half flux-shifted LL to be filled atop Chern -4 gap, resulting in $(-3, -1/2)$ , or to be emptied starting from the charge neutrality point Chern 0 gap, resulting in $(-1, 1/2)$ (Fig. 1F). However, such broken symmetry states have never been experimentally established, because previous studies lack microscopic information.

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Visualizing CIs and their broken symmetries

To determine whether the CIs at fractional filling break any translational symmetry, we used STM to directly visualize the spatial structure of their electronic density of states. We measured the spatial modulation of the tunneling current $\delta|I_{dc}|$ at small bias voltages [section S9 (30)]. As expected, the integrated density of state maps for the CI with $(C, s) = (-2, 1)$ preserved the moiré translational symmetry, as shown in Fig. 2A. This was further confirmed in their structure factor $S(\bar{q})$ , shown in Fig. 2F [section S9 (30)], with six sharp moiré Bragg peaks (in red hexagons) in $C_{3}$ symmetry. Notably, a CI with $(C, s) = (-4, 1)$ , although preserving moiré translational symmetry, developed an emergent Kagome charge order with intra-moiré unit cell structure (Fig. 2B). This feature gave rise to the higher-order Bragg peaks (blue circles) in Fig. 2G. The rich intra-moiré unit cell structure highlights the importance of Coulomb interaction within a unit cell (32), even in the cases of CIs with integer $(C, s)$ .

A signature of breaking the moiré translational symmetry appears in the STM images of CIs with fractional s, such as the state $(C, s) = (-1, 1/2)$ shown in Fig. 2C. Instead of the original triangular moiré translation symmetry, we measured a stripe-like charge order with reconstructed unit cell (green rectangles). The structure factor $S(\overline{q})$ maps (Fig. 2H) constructed from these images show the absence of $C_{3}$ symmetric moiré Bragg peaks (red hexagons) and the emergence of new $C_{2}$ symmetric Bragg peaks (green squares). The dominant Bragg peaks appear at half of the reciprocal vector b (denoted in Fig. 2F) of the moiré superlattice, showing that the real-space periodicity of the stripe charge order is twice the moiré lattice constant. Our observation is consistent with a CDW doubling the moiré unit cell at half filling of the Hofstadter's subband. Our observation of CDWs with a finite Chern number C is distinct from previous reports of moiré commensurate CDWs, termed generalized Wigner crystals (33), which are topologically trivial.

Our imaging experiments established the ground state for the case of integer C and fractional s to be the anticipated symmetry broken Chern insulators (SBCIs). Our experiments demonstrated this behavior for all incompressible states with integer C and fractional s, including those at $V_{G} > 0$ [Fig. 2, D, E, I, and J, and figs. S13 to S15, section S10(30)]. Figure 2D shows STM imaging of the $(C, s) = (2, 1/3)$ state, which shows three times the size of the moiré unit cell (orange parallelogram). The corresponding $S(\overline{q})$ map (Fig. 2I) also shows the corresponding $C_{3}$ symmetric Bragg peaks (orange hexagons), appearing at the reciprocal vectors of $|b| / \sqrt{3}$ . This is consistent with the simplest picture of one-third filling of a Hofstadter subband in which one electron charge is distributed over three moiré unit cells. In addition, we show that the broken translation symmetry can take on forms more complicated than existing predictions, as in the case of $(C, s) = (1, 1/2)$ (Fig. 2E). The band-filling index s indicates a half-filled Hofstadter subband, which, in the simplest case, corresponds to one charge in two moiré unit cells. Instead, we observed electronic structure that quadruples the unit cell (pink parallelogram). Correspondingly, six sharp peaks with magnitude of $|b| / 2$ appeared in the $S(\overline{q})$ map (Fig. 2J). Our real-space imaging suggests that the $(C, s) = (1, 1/2)$ SBCI corresponds to a quadrupled reconstructed unit cell, which incorporates two electron charges.

In addition to the rich inter-unit cell reconstruction, we observed complicated intra-unit cell structures of these SBCIs that are either due to higher harmonics of the moiré potential or formed owing to the strong electron-electron interactions. Moreover, we also found that the orientation of the $(-1, 1/2)$ stripe SBCI in the same field of view rotates upon slight charge doping [fig. S16, section S11 (30)], suggesting that this electronic order is not strongly coupled to the underlying lattice or sample strain. However, whether SBCI forms because of electron-phonon coupling or a pure electronic Coulomb interaction remains an open question.

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Quantum melting and topological defects

Our imaging technique also enabled a direct study of the process of quantum melting of SBCI tuned by electron density and determined the role of topological defects that may be present as these phases approached melting. Imaging the stripe SBCI $(C, s) = (-1, 1/2)$ (Fig. 3A) over a large field of view, we observed a number of notable features, such as domains with stripes in different orientation, and also boundaries that separate them. The three stripes gave rise to the reciprocal wave vector $q_{i=1,2,3}$ shown in the fast Fourier transform (FFT) map (Fig. 3B) at half of the original moiré wave vector $b_{i}/2$ . We characterized the properties of this intertwined SBCI using an analysis that separately investigates the individual stripe component following methods previously used to analyze similar phenomena in stripe phases (34, 35) [section S12 (30)].

Figure 3, D to F, shows the relative phase $\varphi_{\boldsymbol{q}_1}(\boldsymbol{r})$ , the SBCI amplitude distribution $\rho_{\boldsymbol{q}_1}^o (\boldsymbol {r})$ , and the cosine charge modulation $\cos [\boldsymbol {q}_1\cdot \boldsymbol {r} + \varphi_{\boldsymbol{q}_1}(\boldsymbol {r})]$ of the stripe SBCI associated with $\boldsymbol{q}_1$ , respectively. The same operation can be repeated for $\boldsymbol{q}_2$ and $\boldsymbol{q}_3$ (fig. S17). Figure 3C shows the normalized

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Fig. 2. Direct imaging of Cls. (A to E) Real-space tunneling current $\delta |I_{\mathrm{dc}}|$ maps measured at $B = 13.2\mathrm{T}$ [(A) to (C)] or $13.8\mathrm{T}$ [(D) and (E)] and low bias voltages $V_{\mathrm{B}}$ of each $(C,s)$ state. The white scale bar is $40~\mathrm{nm}$ . (F to J) Structure factor $S(\overline{q})$ of the tunneling current modulation $\delta |I_{\mathrm{dc}}|$ in panels (A) to (E), respectively. The scale bar is $0.5\mathrm{nm}^{-1}$ . The bilayer graphene/hBN moiré Bragg peaks are identified by red hexagons. [(A) and (F)] The $(-2,1)$ state respects the moiré translational symmetry. The red parallelogram in (A) represents the moiré unit cell. [(B) and (G)] Emergent Kagome lattice for $(-4,1)$ state respects the moiré translational symmetry. The Kagome structure shows up as higher harmonics (blue circles) in the $S(\overline{q})$ map (G). [(C) and (H)] The $(-1,1/2)$ state breaks moiré translational symmetry by doubling the unit cell and forms a topological stripe phase (green rectangle as the unit cell). The Bragg peaks of the emergent stripe phase are identified as the green squares, and the stripe order can be identified by the two dominant Bragg peaks, which have length of half of the reciprocal vector $(b)/2$ . [(D) and (I)] The $(2,1/3)$ state breaks the moiré translational symmetry by tripling the unit cell and forms a triangular lattice [orange parallelogram (D) as the unit cell]. The Bragg peaks are identified as six $\sqrt{3}$ orange hexagons (I). [(E) and (J)] The $(1,1/2)$ state breaks moiré translational symmetry by quadrupling the unit cell and forms a triangular lattice [pink parallelogram (E) as the unit cell]. The Bragg peaks of the emergent triangular lattice are identified as the six pink hexagons (J). All data are collected at $T_{\mathrm{eff}} = 210\mathrm{mK}$ .

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Fig. 3. Topological melting of an SBCI ( $C = -1, s = 1/2$ ). (A) A large real-space tunneling current $\delta|I_{dc}|$ map measured at $B = 13.8$ T and $V_{\mathrm{B}} = 6$ mV. The stripes with three different orientations can be observed. (B) FFT of the $\delta|I_{dc}|$ map in (A). The stripes with different orientations are identified by $\boldsymbol{q}_{i=1,2,3}$ vectors. The scale bar is $0.25$ nm $^{-1}$ . (C) The real-space distribution of normalized amplitude of the three $\boldsymbol{q}_{i=1,2,3}$ vectors. (D) The extracted relative phase $\varphi_{\boldsymbol{q}_1}(\boldsymbol{r})$ map. Where the topological defect is identified by dotted black (red) circles, the clockwise winding of the phase is $2\pi (-2\pi)$ . The dotted black (red) circle represents the dislocation (antidislocation). (E) The amplitude $\rho_{\boldsymbol{q}_1}^o (\boldsymbol{r})$ map of $\boldsymbol{q}_1$ , showing the strength of stripe along the $\boldsymbol{q}_1$ direction. (F) The cos $[\boldsymbol{q}_1 \cdot \boldsymbol{r} + \varphi_{\boldsymbol{q}_1}(\boldsymbol{r})]$ map, with a sharp boundary shifting half of the unit cell. (G) A density-dependent STS across the insulating gap of SBCI ( $C = -1$ , $s = 1/2$ ). (H) Selected cos $[\boldsymbol{q}_1 \cdot r + \varphi_{\boldsymbol{q}_1}(\boldsymbol{r})]$ maps as a function of $V_{\mathrm{G}}$ across the gap. The top, middle, and bottom rows are for $\boldsymbol{q}_1$ , $\boldsymbol{q}_2$ , and $\boldsymbol{q}_3$ , respectively. The dislocations (antidislocations) are marked as black (red) dots in the maps. The number of topological defects increases upon doping away from the gap center ( $V_{\mathrm{G}} = -0.168$ V). (I) The number of topological defects (dislocation + antidislocation) as a function of $V_{\mathrm{G}}$ . Topological defects proliferate as the system is doped away from the gap center, suggesting that the SBCI stripe phase melts through a topology-driven mechanism. The white scale bars in all panels are $50~\mathrm{nm}$ . All data are collected at $T_{\mathrm{eff}} = 210$ mK. h-dope, hole doped; e-dope, electron doped.

The topological defects are not pinned to specific topographic features, such as lattice point defects. Instead, we observed that the topological defects change locations when doping the SBCI (Fig. 3H). We show a zoomed-in STS at gate voltages $V_{\mathrm{G}}$ nearby the $(C, s) = (-1, 1/2)$ SBCI in Fig. 3G. We imaged the charge order with broken translation symmetry at eight different $V_{\mathrm{G}}$ (figs. S18 and S19) and analyzed the locations and types of topological defects, as in Fig. 3H. The total number of topological defects, summing all three wave vectors $q_{i}$ , are plotted

Focusing on the relative phase $\varphi_{\boldsymbol{q}_{1}}(\boldsymbol{r})$ shown in Fig. 3D, we discuss the presence of topological defects within a single stripe orientation. The two topological defects are dislocations and antidislocations, corresponding respectively to where stripes terminate and where they merge. In the phase map, they appear as singular points: A clockwise loop around a dislocation gives a $+2\pi$ phase winding (black), whereas a clockwise loop around an antidislocation gives a $-2\pi$ phase winding (red). We observed a pair of dislocation and antidislocation; they are responsible for the sharp boundary that separates two patches of the stripes shown in Fig. 3F, with an offset of one moiré superlattice constant. A notable question is whether a (anti-)dislocation carries fractional charge.

SBCI amplitude distribution of the three wave vectors $q_{i}$ , represented by red, green, and blue, respectively. We found that the amplitude distribution analysis shows that all three directions can coexist with each other.

in Fig. 3I as a function of $V_{G}$ . We observed a trend of increasing the total number of (anti-)dislocations as the system is doped away from the center of the incompressible gap near $V_{G} = -0.168$ V. Our measurements indicate that the quantum phase transition for this SBCI to a compressible phase is mediated by proliferation of topological defects, consistent with a Kosterlitz-Thouless transition (36, 37).

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Quantum melting and phase separation

Lastly, we present an example of a quantum phase transition for a CI that occurs through phase separation and a possible signature of topological edge modes at the phase boundary. Figure 4 shows a series of images near the $(C,s) = (-4,1)$ (indicated in Fig. 4A), which has a Kagome lattice structure (Fig. 4B). Upon increasing $V_{\mathrm{G}}$ , there was a quantum phase transition between the incompressible Kagome Chern phase to another incompressible phase with petallike electronic structure [fig. S20, section S13 (30)]. Real-space maps show phase separation during this transition. As $V_{G}$ increased, the Kagome lattice region shrunk, while the petallike region expanded (Fig. 4, C to E), ultimately filling the entire field of view (Fig. 4F). The spectroscopy in Fig. 4A shows the closing and opening of a gap when the phase boundary crosses the location of the STM tip (red stars, Fig. 4, B to G) as $V_{\mathrm{G}}$ is varied, indicating that the boundary involves a gapless mode, as anticipated at the boundary of a CI (38). Although we could not experimentally detect hysteresis in the gate-dependent spectra for this transition, the observation of phase separation suggests a first-order phase transition for melting of this interacting Chern phase. Lastly, with further electron doping, the petallike structure evolved into a compressible state exhibiting intricate intra-unit cell structure [Fig. 4G and fig. S20, section S14 (30)].

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Fig. 4. Phase separation and quantum melting of a Kagome Cl. (A) STS near a $(C,s) = (-4,1)$ state at magnetic field $B = 13.2\mathrm{T}$ . The incompressible spectroscopic features of the Kagome Cl as well as gap closing (between orange and yellow arrows) are labeled. The gap closing happens when the sharp phase boundary in (C) and (D) passes underneath the tip, indicating that the phase boundary is compressible. The gate voltages for images in (B) to (G) are marked with colored arrows on the right side of the spectrum. (B) The tunneling current $\delta |I_{\mathrm{dc}}|$ map measured at $V_{\mathrm{G}} = -1.982\mathrm{V}$ (red) and $V_{\mathrm{B}} = 4.8\mathrm{mV}$ shows an emergent Kagome lattice. The moiré unit cell is marked with a red parallelogram. (C) The $\delta |I_{\mathrm{dc}}|$ map measured at $V_{\mathrm{G}} = -1.972\mathrm{V}$ (orange) and $V_{\mathrm{B}} = 3.6\mathrm{mV}$ shows an atomically sharp phase boundary of the Kagome lattice. (D) The $\delta |I_{\mathrm{dc}}|$ map measured at $V_{\mathrm{G}} = -1.962\mathrm{V}$ (yellow) and $V_{\mathrm{B}} = 5.6\mathrm{mV}$ shows a phase boundary between the incompressible Kagome lattice and the incompressible petallike structure with the Kagome lattice island shrinking. (E) The $\delta |I_{\mathrm{dc}}|$ map measured at $V_{\mathrm{G}} = -1.952\mathrm{V}$ (green) and $V_{\mathrm{B}} = 5.0\mathrm{mV}$ . (F) The $\delta |I_{\mathrm{dc}}|$ map measured at $V_{\mathrm{G}} = -1.922\mathrm{V}$ (blue) and $V_{\mathrm{B}} = 4.0\mathrm{mV}$ . The entire field of view is filled with petallike electronic structure. (G) The $\delta |I_{\mathrm{dc}}|$ map measured at $V_{\mathrm{G}} = -1.860\mathrm{V}$ (purple) and $V_{\mathrm{B}} = 1.6\mathrm{mV}$ . The system enters a compressible state with complex intra-unit cell structure. The scale bars in all $\delta |I_{\mathrm{dc}}|$ maps are $40~\mathrm{nm}$ . The red stars in (B) to (G) indicate the location of the tip while measuring the spectrum in (A). All data were collected at $T_{\mathrm{eff}} = 210\mathrm{mK}$ .

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Conclusions and outlook

Our study visualizes a plethora of SBCI states and directly determines the relationship between the quantum indices describing such phases (C and s) and the spatial structure of their wave functions, showing examples of states that enlarge the unit cell as well as those with complex intra-unit cell structures. Detailed understanding of what stabilizes these broken symmetry phases awaits further theoretical investigation. We also provide a distinctive perspective on the quantum phase transitions of correlated and topological phases, demonstrating that both Kosterlitz-Thouless-type defect-mediated and phase separation-type transitions can occur. Looking ahead, our techniques can provide important new insights when applied to similar experiments on both in-field and zero-field fractional CIs. A notable setting is the in-field fractional CI states, because theoretical studies predict topological defects to host fractionalized charges and have non-Abelian statistics (39).

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ACKNOWLEDGMENTS

We thank T. Wang, J. Y. Lee, and M. Zaletel for useful conversations. Funding: This work was primarily supported by DOE-BES grant DE-FG02-07ER46419, the Gordon and Betty Moore Foundation's EPIQS initiative grants GBMF9469, and US Army Research Office MURI project under grant nos. W911NF-21-2-0147 and W911NF261A052 to A.Y. Other support for the experimental work was provided by the National Science Foundation Materials Research Science and Engineering Center (NSF-MRSEC) through the Princeton Center for Complex Materials NSF-DMR-2011750, NSF grant DMR-2312311, NSF grant OMA-2326767, and ONR N00012-21-1-2592. O.V. was supported in part by the Gordon and Betty Moore Foundation's EPIQS Initiative (grant no. GBMF11070) and by a grant from the Simons Foundation SFIMPS-NFS00006741-09. A.Y. acknowledges the hospitality of the Trinity College, the Physics Department, and the Cavendish Laboratory in Cambridge UK. Author contributions: M.H., Y.-C.T., and A.Y. devised the experiments. M.H. and Y.-C.T. created device structures and carried out the STM measurements and data analysis. R.P. and O.V. carried out the theoretical calculations. K.W. and T.T. provided the h-BN substrates. M.H., Y.-C.T., A.Y., R.P., and O.V. all collaborated in writing of the manuscript. Competing interests: The authors declare that they have no competing interests. Data, code, and materials availability: The data from this study are available at Figshare (40). Details for the synthesis and characterization of all compounds and materials are in the methods section. License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse

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SUPPLEMENTARY MATERIALS

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science.org/doi/10.1126/science.aef0940

Materials and Methods; Supplementary Text; Figs. S1 to S20; References (41–44); Movie S1 Submitted 29 December 2025; accepted 24 July 2026

COMPARATIVE COGNITION

Ultrarapid decision-making in an avian brain

Philipp Schmidbauer and Andreas Nieder\*

Perceptual decision-making is well studied in mammals, but its operation in other vertebrates remains unclear. We show that carrion crows (Corvus corone) make deliberate decisions in a classic visual motion discrimination task with unprecedented speed, reporting choices in approximately 235 milliseconds on average, which is roughly twice as fast as has been observed in monkeys or humans and without sacrificing accuracy. Recordings from the pallial endbrain reveal that direction-selective neurons encode the upcoming choice as early as about 70 milliseconds after stimulus onset and about 170 milliseconds before the response, with ramping activity scaling with sensory evidence and converging at response onset. These findings highlight the extraordinary efficiency of avian decision-making circuitry, possibly shaped by evolutionary pressures for rapid visuomotor control.

Perceptual decision-making involves integrating sensory information to guide behavior critical for survival (1–3). In primates performing random-dot motion discrimination tasks, perceptual decisions unfold over hundreds of milliseconds as neurons in the posterior parietal cortex accumulate sensory evidence under sequential sampling dynamics until their activity reaches a threshold signaling commitment to a choice (4–6). It remains unclear whether these canonical decision mechanisms are specific to the mammalian neocortex or if they can also emerge in other vertebrates through distinct neural architectures.

Corvid songbirds such as ravens, crows, and jays offer a powerful comparative model for addressing this question because they exhibit highly sophisticated perceptual and cognitive abilities (7–10). Having diverged from mammals more than 360 million years ago (11), birds evolved a distinct nuclear pallium that lacks the layered neocortex (12, 13) yet retains key organizational and computational principles characteristic of mammalian brains (14). Central to these capacities is the nidopallium caudolaterale (NCL), an associative pallial region at the apex of the avian pallial processing hierarchy. The NCL is widely regarded as a functional analog of the primate prefrontal cortex (15), supporting the executive functions underlying flexible decision-making in intelligent birds such as crows (16, 17).

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Crows' motion discrimination performance

To investigate the behavioral and neural correlates of perceptual decision-making in birds, we tested two carrion crows (Corvus corone). The crows were trained to discriminate visual motion direction in a classic random-dot motion task with dynamic dot patterns of varying coherence (Fig. 1A) (see the materials and methods). Each trial began when the crow positioned its head in front of the stimulus screen, monitored by an infrared light barrier. Dot patterns moved in one of four directions (left versus right or up versus down) at 3%, 9%, 27%, or 81% coherence, plus a 0% random-motion condition. Two response targets (left-right or up-down) flanked the central stimulus, and crows reported their decision by pecking one target after leaving the light barrier.

Crow 1 and crow 2 completed 55 and 102 sessions, respectively, with mean numbers of correct trials per session of 207 and 209 and mean total trials per session of 276 and 285, respectively. Overall choice accuracy was $75.0 \pm 0.4\%$ (crow 1) and $73.4 \pm 0.3\%$ (crow 2) and strongly depended on motion strength (Fig. 1B and table S1). Accuracy reached ceiling at 81% coherence (crow 1: $99.9 \pm 0.1\%$ ; crow 2: $99.4 \pm 0.2\%$ ) and declined with weaker motion, approaching threshold ( $\sim75\%$ ) at 9% coherence (crow 1: $78.5 \pm 0.8\%$ ; crow 2: $71.8 \pm 0.6\%$ ). Both crows performed above chance at 3% coherence (crow 1: $56.5 \pm 0.8\%$ , $t_{(54)} = 7.8$ ; crow 2: $57.5 \pm 0.7\%$ , $t_{(101)} = 10.9$ , both P < 0.001; one-sample t test). As expected, choices were approximately evenly distributed between the two directions at 0% coherence, where the “correct” direction was randomly assigned (crow 1: $49.8 \pm 1.0\%$ , $t_{(54)} = -0.25$ , P = 0.803; crow 2: $49.6 \pm 0.7\%$ , $t_{(101)} = -0.6$ , P = 0.575; one-sample t test), indicating no systematic directional bias.

Reaction time, the interval from stimulus onset to head-movement initiation, was very short, with average across session medians incorporating all correct trials and 0% trial independent of choice of $235 \pm 2$ ms (crow 1) and $235 \pm 1$ ms (crow 2). Reaction times varied only modestly with motion strength (Fig. 1C and table S1), ranging from 220 ms (81% coherence) to 254 ms (0% coherence) in crow 1 and from 216 to 243 ms in crow 2, indicating minimal influence of task difficulty on decision time. Both crows showed small biases in accuracy and reaction times across horizontal (fig. S1) and vertical (fig. S2) target layouts. In error trials, both crows responded significantly more slowly than on correct trials (fig. S3), consistent with deliberate, evidence-based decision-making (4).

To test whether the crows' performance depended on dot density, motion algorithm, or a brief post-motion-onset waiting period, we tested four classical random-dot motion variants that differed in all three factors (18). Accuracy and reaction times were comparable across random-dot motion stimulus types, dot densities, and in the absence of a brief waiting period (fig. S4). Crow 1 even responded slightly faster in the absence of a brief waiting period. Together, these results suggest that the crows' accurate yet rapid decision-making is not explained by task or stimulus design, but rather reflects an intrinsic biological capacity.

We tested whether crows' performance during recordings conformed to a drift-diffusion model of decision-making (19, 20). The standard model, which assumes a linear mapping between drift rate and sensory evidence, poorly captured the crows' reaction time distributions (figs. S5 and S6). Motivated by the nonlinear relationship between perceived and physical stimulus intensity known from psychophysics, we evaluated nonlinear mappings between coherence and drift rate.

Exponential $(x^{1/2}, x^{1/3})$ and logarithmic $(\log_{2}x)$ functions all improved model fits compared with the linear mapping [crow 1: $F_{(54)} = 1975.0, P < 0.001$ ; crow 2: $F_{(101)} = 3701.6, P < 0.001$ ; repeated-measures analysis of variance (ANOVA)]. The logarithmic mapping provided the best fit for both crows ( $P_{corrected} < 0.05$ , post hoc paired t tests; Fig. 1, B and C, green line, and figs. S5B and S6B), indicating a nonlinear relation between motion coherence and evidence accumulation.

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Direction-selective NCL neurons predict behavioral choice

During task performance, we recorded activity from 248 neurons in the NCL (crow 1: 127; crow 2: 121; Fig. 1D), which is known to contain neurons sensitive to random-dot motion direction (21). For each neuron, the preferred motion direction was defined as the one evoking the highest firing rate during decision formation (80 ms after stimulus onset until response); the opposite was designated antipreferred.

One-fourth of neurons (58/248, 23.4%) were direction selective, showing significantly stronger firing for the preferred direction during correct trials [receiver operating characteristic (ROC) analysis, P < 0.05]. Preferred-direction activity ramped up steadily after stimulus onset, peaking near the behavioral response, whereas antipreferred responses remained flat (Fig. 1, E and F).

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Fig. 1. Decision behavior and motion-direction selective neurons in NCL. (A) Task design. Trials began with the crow positioning its head in a light barrier in front of the touchscreen. After a prestimulus period, two choice targets appeared on opposite sides of the screen, followed by a dynamic dot stimulus at the center. Crows reported the perceived global motion direction (arrow shown for illustration) by pecking the corresponding target, immediately terminating the motion stimulus. (B) Discrimination accuracy of crows 1 and 2 (55 and 102 sessions) across five motion coherence levels (0 to 81%). (C) Average median reaction times, measured from motion-stimulus onset to head movement out of the light barrier. Black circles denote session-averaged behavioral data (mean ± SEM); green curves show the mean session-wise drift-diffusion model (DDM) fits, with shaded areas indicating SEM. (D) Schematic lateral view of the crow brain showing the recording site in the NCL (gray). Tel., telencephalon; Cb, cerebellum; TeO, optic tectum. (E and F) Example neurons discriminating preferred and antipreferred (up/down) motion directions. Trials were aligned to stimulus onset (left) or response onset (right). Top panels show spike rasters (each line represents a trial; each dot an action potential), and bottom panels show spike-density functions smoothed with a 100-ms Gaussian kernel. Gray shading indicates the distributions of stimulus onset and response times, respectively.

Population analyses revealed that NCL activity reflected the upcoming choice early. In correct trials (3 to 81% coherence), preferred-direction activity ramped continuously from stimulus onset to response (Fig. 2A), diverging from antipreferred activity 67 ms after stimulus onset and 171 ms before movement (sliding-window Wilcoxon signed-rank test, P < 0.05, n = 58). We verified the time course of neuronal selectivity using a sliding Mann-Whitney U test with a larger smoothing window, which reduces temporal precision (fig. S7), and obtained timing estimates closely matching the original analysis.

We derived the area under the ROC curve (AUC), which quantifies how well a neuron's firing rate distinguishes between two motion directions, with 0.5 indicating no discrimination and 1.0 indicating perfect discrimination. Across neurons, AUC values exceeded the chance level of 0.5 (mean = 0.631, $t_{(57)} = 18.06$ , P < 0.001, one-sample t test), indicating significant discrimination between motion directions and linking NCL activity to the crows' perceptual decisions (Fig. 2B). A time-resolved sliding ROC analysis based on individual neuron firing rates for preferred versus antipreferred directions supported the observed separation of activity during decision formation (fig. S8).

To separate sensory from choice-related activity, we analyzed random-motion trials (0% coherence) grouped by chosen side. Even without directional motion cues, NCL activity predicted choice: Preferred and antipreferred signals diverged 96 ms after stimulus onset and 99 ms before response (in correct trials 69 and 161 ms, respectively; P < 0.05, n = 56) (Fig. 2C), with AUC = 0.569 ( $t_{(55)} = 5.21$ , P < 0.001; one-sample t test; Fig. 2D).

Error trials showed a similar pattern. When crows chose the preferred target despite motion toward the antipreferred side, NCL activity resembled correct preferred-direction responses and vice versa (Fig. 2E). Divergences occurred 63 ms after stimulus onset in correct trials and 113 ms in errors (171 versus 55 ms before response, respectively; P < 0.05, n = 49). AUC values in error trials (mean = 0.571, $t_{(48)} = 4.87$ , P < 0.001; one-sample t test; Fig. 2F) confirmed choice-related coding.

A support vector machine (SVM) classifier trained on firing rates in correct trials successfully decoded the chosen direction in correct (87.3%), random-motion (72.5%), and error trials (67.7%), outperforming shuffled controls (95th percentile = 65%; Fig. 2G). These results demonstrate that NCL activity encodes the decision outcome independently of sensory input.

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NCL neurons encode sensory evidence

We next investigated how motion coherence modulated direction-selective activity (Fig. 3). Population activity scaled with motion coherence after stimulus onset and immediately before response (Fig. 3A). Single-neuron examples illustrating motion coherence-dependent activity are shown in fig. S9. For each neuron, average normalized activity during decision formation increased with coherence in the preferred direction $t_{(42)} = 3.00, P = 0.002$ ; one-sample t test; Fig. 3, B and C), but not in the antipreferred direction $t_{(42)} = 0.70, P = 0.246$ . Population activity tracked motion coherence over time before becoming coherence independent late in the decision period (fig. S10). Thus, NCL neurons encoded both decision outcome and the amount of sensory evidence, corresponding to gradually accumulated information provided by motion coherence to reach a decision threshold.

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Fig. 2. Population activity of direction-selective NCL neurons encoded the choice. (A) Normalized activity of all direction-selective neurons ( $n = 58$ ) during correct trials (3 to $81\%$ coherence) for preferred (blue) and antipreferred (red) directions aligned to stimulus onset (left) or response onset (right) and smoothed with a 100-ms Gaussian kernel. Shading indicates SEM across neurons. Black bars mark significant differences between preferred and antipreferred activity (sliding-window Wilcoxon signed-rank test, 50-ms window, 1-ms steps, $P < 0.05$ ). Gray shading indicates the distributions of response and stimulus onset times, respectively. (B) Distribution of AUC for direction-selective neurons during correct trials. AUC was calculated from spike rates between stimulus onset and response. Arrow indicates the mean; asterisks denote values significantly $>0.5$ (one-sided one-sample $t$ test). (C) Activity of direction-selective neurons ( $n = 56$ ) during correct trials as in (A) (preferred, blue; antipreferred, red) and random-motion trials ( $0\%$ coherence; chosen target, light blue/orange) grouped by the target selected by the crows. (D) AUC distribution in random-motion trials. (E) Normalized activity of direction-selective neurons ( $n = 49$ ) during correct (preferred, blue; antipreferred, red) and error trials (light blue/orange). Error trials were grouped by the target chosen by the crows, opposite to the stimulus direction. (F) AUC distribution in error trials. (G) Accuracy of an SVM classifier trained on spike rates from correct trials ( $n = 48$ neurons; 10,000 repetitions) and tested on correct, random-motion, and error trials. Control shows performance with permuted labels; dashed line indicates the 95th percentile of the control distribution.

To relate neuronal dynamics to sensory evidence (i.e., motion coherence), we quantified ramping rates, activity increase per second, in the preferred direction. Ramping rates were extracted within a 150-ms window centered on the inflection point (110 ms after stimulus) of the population signal. Average ramping rates increased with motion coherence, although modestly $(t_{(42)} = 1.64, P = 0.055;$ one-sample t test; Fig. 3, D and F).

Because behavioral modeling revealed a logarithmic relationship between motion coherence and evidence accumulation, we tested whether ramping rates followed a similar pattern. Linear regression of ramping rate versus motion coherence showed a superior fit on a logarithmic scale $(R^{2}=0.83, P=0.032)$ compared with a linear scale $(R^{2}=0.65, P=0.103;$ Fig. 3E). Across neurons, slope distributions on the log scale were significantly above zero $(t_{(42)}=2.17, P=0.018;$ Fig. 3F), confirming a robust positive relationship between ramping rate and log-transformed motion coherence. This mirrors the nonlinear relationship between motion coherence as sensory evidence and accumulation rate suggested by behavior.

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Decision-related dynamics of NCL neurons

To link decision-signal dynamics with behavior, trials were grouped by reaction time into short, medium, and long categories (Fig. 4 and fig. S11). Spike-density functions revealed that, after stimulus onset, activity in trials with long reaction times rose more slowly than in short or medium trials (Fig. 4A, left), demonstrating a tight coupling between decision time and ramping rate. When aligned to response onset, however, all reaction time groups exhibited similar temporal profiles (Fig. 4A, right), with activity converging toward a similar level during the purely premotor period within 50 ms before the response (Fig. 4B; short: $0.99 \pm 0.19$ SD; medium: $0.67 \pm 0.21$ SD; long: $0.77 \pm 0.27$ SD; $\chi^{2}_{(2)} = 4.42$ , P = 0.110; Kruskal-Wallis test). This approximate convergence is consistent with a threshold-like termination of evidence accumulation, although the lack of complete convergence indicates that NCL activity is not governed by a simple fixed threshold. Indeed, recent work in monkey lateral intraparietal area using a similar task revealed substantial heterogeneity in response profiles, with only a subset of neurons showing classical ramp-to-threshold activity and others exhibiting coherence-dependent responses proposed to reflect decision confidence (22). Thus, as in lateral intraparietal area, additional cognitive variables may modulate the choice-related activity in NCL, contributing to the heterogeneity of firing rates at response onset.

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Rapid decision-making in crows: A cross-species comparison

We showed that neurons in the crow NCL encode a robust neural correlate of motion-direction decisions, with temporal dynamics consistent with evidence accumulation under sequential sampling and closely paralleling canonical decision-making processes in the neocortex (4–6, 22–26). Even without explicit pressure to respond quickly, the crows reported motion direction with head movements in an average of 235 ms

across motion coherences while maintaining high accuracy. By comparison, even when monkeys and humans report motion direction as quickly as possible using saccades, among the fastest deliberate motor responses in primates, with latencies as short as \~70 ms and typically \~140 ms (27, 28), their reaction times remain roughly twice those of crows despite the crows' use of high-inertia head movements (fig. S12).

In closely matched, self-paced random-dot motion tasks, monkeys showed reaction times of $\sim 410$ , $\sim 490$ , and $\sim 600$ ms across three studies at comparable motion coherence levels (29-31) (fig. S12). Primates can exhibit very fast responses under certain conditions (32–34), but these studies differ substantially from the classical random-dot motion paradigm used here, particularly in task structure, stimulus properties, and temporal constraints. The reaction times of monkeys in self-paced random-dot motion tasks are comparable to those of humans performing the same task, who showed mean reaction times of $\sim$ 450, $\sim$ 510, and $\sim$ 820 ms across three studies (35–37) (fig. S12). Rats performing a self-paced random-dot motion task showed mean reaction times of $\sim$ 500 to 1000 ms, depending on stimulus difficulty, and were therefore slower than monkeys (38). Ants and bees can also make rapid visual discrimination decisions, but these results are not directly comparable to crow and monkey random-dot motion studies because the task and decision-making paradigms differ fundamentally (39, 40).

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Fig. 3. Population activity also reflects the amount of sensory evidence. (A) Normalized activity of direction-selective neurons ( $n = 43$ ) across motion coherences aligned to stimulus onset (left) or response onset (right). Solid lines show trials in which crows chose the neuron's preferred target; dashed lines show antipreferred choices. Activity was smoothed with a 100-ms Gaussian kernel and averaged across neurons. Gray shading indicates the distributions of response and stimulus onset times, respectively. (B) Average activity across motion coherences in preferred and antipreferred directions measured from 80 ms after stimulus onset to each trial's response. Gray lines show the mean linear fits to coherence-dependent activity across individual neurons. (C) Distribution of slopes from linear fits to each neuron's activity for preferred (top) and antipreferred (bottom) choices. (D) Average increase in normalized activity per second ( $\Delta \text{rate}_{\text{norm}}/\text{s}$ ) as a function of motion coherence. Error bars indicate SEM across neurons; the black line shows a linear fit ( $R^2 = 0.65$ ). (E) Average ramping rate as a function of motion coherence on a logarithmic scale. The black line shows a linear fit on the log scale ( $R^2 = 0.83$ ). (F) Distribution of slopes from linear fits to each neuron's ramping rate on linear (top) and logarithmic (bottom) motion-coherence scales.

Fig. 4. Reaction time-dependent activity of direction-selective neurons. Trials were grouped by reaction time (short: 175 to 225 ms; medium: 230 to 280 ms; and long: 285 to 335 ms). (A) Normalized population activity of direction-selective neurons grouped by reaction time (short: n = 58; medium: n = 58; long: n = 43), aligned to stimulus (left) or response onset (right). Solid lines show preferred-direction activity smoothed with a 100-ms Gaussian kernel; gray shading indicates the preresponse analysis window. (B) Average normalized activity for each reaction time group in preferred and antipreferred directions during the 50 ms preceding the response [gray shading in (A), right]. Error bars indicate SEM across neurons.

Crows made decisions approximately twice as fast as primates without sacrificing accuracy. This performance suggests faster evidence accumulation and decision commitment rather than a shift along the speed-accuracy trade-off. The rapid emergence of choice-selective NCL activity \~70 ms after stimulus onset and \~170 ms before the behavioral response further supports this conclusion.

The crows' ultrafast decision speed may in part reflect the high temporal precision of the avian visual system, potentially shaped by selection for rapid sensory-motor processing. Birds exhibit exceptionally high temporal visual resolution, with some songbird species resolving flickering light at frequencies of up to 145 Hz (critical flicker-fusion frequency) (41, 42). At the neuronal level, rapid visual processing is supported by fast retinal spike conduction (43) and an efficient avian tectofugal pathway, with optic tectum responses emerging within \~5 ms of stimulus onset (44, 45) and downstream rotundus activity within \~20 ms (46). Although these latencies overlap with early visual responses in primates, they indicate rapid propagation of visual signals through the avian tectofugal pathway to higher-order processing stages. Such rapid early visual processing, combined with short conduction distances and dense recurrent connectivity in the compact avian pallium (15–17, 47, 48), may facilitate efficient transformation of sensory evidence into perceptual decisions, with small latency advantages accumulating across processing stages to accelerate perception-action cycles.

Together, these findings suggest that the corvid NCL represents a convergent solution to perceptual decision-making. It supports primate-like computational dynamics within a distinct neural architecture, with markedly higher temporal efficiency. This speed may reflect evolutionary pressures on avian visuomotor control for rapid beak movements, predator detection, and flight navigation (49, 50).

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ACKNOWLEDGMENTS

We thank Z. Hafed for help with generating the motion stimuli. Author contributions: P.S. and A.N. designed the experiments. P.S. conducted the experiments. P.S. and A.N. analyzed the data. P.S. and A.N. wrote the manuscript. P.S. and A.N. edited the manuscript. A.N. supervised the study. Competing interests: The authors declare no competing interests. Data, code, and materials availability: Data to reproduce the analyses and figures are available at the Figshare digital repository (51). License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.aed6459

Materials and Methods; Table S1; Figs. S1 to S12; References (52–56);

MDAR Reproducibility Checklist

Submitted 4 November 2025; accepted 25 August 2026

10.1126/science.aed6459

2D MATERIALS

Imaging electron-hole asymmetry in the quantum melting of generalized Wigner crystals

Emma Berger $^{1,2,*}$ \$ \dagger \$ , Michael Arumainayagam \$ ^{1} \$ \$ \dagger \$ , Zhihuan Dong $^{1}$ , Lucas Schneider $^{1}$ , Tianle Wang $^{1,3}$ , Greyson Nichols $^{4}$ , Salman Kahn $^{1,5}$ , Rwik Dutta $^{6}$ , Gaoqiang Wang $^{7}$ , Takashi Taniguchi $^{8}$ , Kenji Watanabe $^{9}$ , Mit H. Naik $^{6,10}$ , Michael P. Zaletel $^{1}$ , Feng Wang $^{1,5,11,*}$ , Michael F. Crommie $^{1,5,11,*}$

Two-dimensional moiré materials provide a versatile platform to explore phase transitions in strongly correlated systems. Using scanning tunneling microscopy, we imaged the density-driven melting of generalized Wigner crystals (GWCs) and Mott insulators (MIs) in electron-doped, near-60°-twisted molybdenum diselenide bilayers featuring a triangular moiré superlattice. We observed notable electron-hole asymmetry in GWC melting: Hole-doped GWCs yielded interaction-driven disordered states, whereas electron-doped GWCs melted into delocalized liquid-like states. This asymmetry arose from the broken particle-hole symmetry of the moiré superlattice, which produced electron and hole Fermi pockets with different momentum geometries upon GWC condensation. MI states melted without such asymmetry, consistent with the absence of a symmetry-breaking density modulation. This work provides direct visualization of the emergent phases that appear as GWCs undergo quantum melting transitions.

The competition between commensurate and incommensurate phases when strongly interacting charges are placed on a two-dimensional (2D) periodic lattice is predicted to lead to new many-body states. These include "pinball liquids" (1–4), disordered "electron slush" (5–11), and nematic liquid crystals (12), where the balance of potential and kinetic energy leads to unusual combinations of localization, delocalization, and disorder. Understanding density-tuned "quantum melting" transitions between such phases is a central challenge in condensed matter physics relevant to many areas from frustrated magnetism (13, 14) to high-temperature superconductivity (15, 16). Moiré superlattices made from twisted atomically thin materials are ideal platforms to explore this behavior because they host strongly correlated generalized Wigner crystal (GWC) (17–20) and Mott insulator (MI) (21–25) states that can be continuously doped through electrostatic gating. Some evidence for quantum melting in moiré systems has already been seen through bulk characterization techniques (26, 27), but the microscopic mechanisms at play are not well understood because these techniques lack direct visualization. For example, the separate roles of electron-electron interactions versus quenched disorder remain unclear. Scanning tunneling microscopy (STM) is ideally suited to explore this topic because it can image both electronic structure and disorder down to the atomic scale (28–33). Although STM has been used to image commensurate GWCs in transition metal dichalcogenide (TMD) moiré bilayers (18, 34), the quantum melting of GWCs as they are doped into states with incommensurate filling has not yet been visualized.

In this study, we report STM imaging of the quantum melting of GWC and MI states in an electron-doped molybdenum diselenide homobilayer twisted near $60^{\circ}$ (tMoSe $_{2}$ ), which features a triangular moiré superlattice. We observed a pronounced electron-hole asymmetry in density-tuned GWC melting at slight departures from commensurate filling of the moiré superlattice, with hole doping favoring interaction-driven disordered states and electron doping inducing uniform, delocalized liquid-like states. This trend was observed for stripe-ordered GWCs at v = 1/2 as well as honeycomb-ordered GWCs at v = 2/3, where v is the number of electrons per moiré unit cell. By contrast, doping the MI state at v = 1 resulted in uniform, liquid-like states for both doping polarities. Our images suggest that disorder in hole-doped GWCs is driven mainly by correlation effects, with quenched disorder helping to stabilize a subset of nearly degenerate states. These results are consistent with previous theoretical work that predicts interaction-driven disordered phases (5–8, 11, 12, 35) at incommensurate fillings in moiré systems, but our experimental observation of strong electron-hole asymmetry in GWC quantum melting was unexpected. Using a Hartree-Fock framework, we show that this behavior arises because doped holes and electrons occupy different regions in the emergent GWC Brillouin zone.

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STM imaging of GWCs in tMoSe $_{2}$

Our experimental setup sketched in Fig. 1A consists of a near- $60^{\circ}$ tMoSe $_{2}$ homobilayer supported by a $\sim$ 60-nm-thick hexagonal boron nitride (hBN) insulator placed atop a Si/SiO $_{2}$ wafer. Electrical contact to the tMoSe $_{2}$ was made using a graphite nanoribbon array to reduce contact resistance while enabling STM imaging of the bare TMD surface (29–33, 36, 37). The tMoSe $_{2}$ carrier density was controlled by applying a back gate voltage ( $V_{G}$ ) between the Si substrate and the graphite contact, and tunnel current was obtained by applying a bias voltage ( $V_{B}$ ) to this contact relative to the grounded STM tip (38). Figure 1B shows a typical STM topographic image of the tMoSe $_{2}$ moiré pattern with a twist angle of $\sim$ 57.4°, corresponding to a moiré lattice constant of $\sim$ 7.4 nm (all STM data were taken at T = 4.8 K). A close-up of the topography in Fig. 1C shows three distinct stacking sites in the tMoSe $_{2}$ moiré unit cell (MX, XX, and MM, where M = Mo and X = Se; Fig. 1D). Electrons doped into the tMoSe $_{2}$ conduction band (CB) occupy the low-energy MM stacking sites [section 2 of (38)] (33, 39, 40).

Figure 1E shows the STM tunnel current obtained with the tip held above an MM site as $V_{G}$ and $V_{B}$ were varied. “Direct” tunneling occurred for $V_{B} > 0$ , where electrons from the STM tip tunnel into empty states in the tMoSe $_{2}$ CB (Fig. 1F). “In-gap” tunneling occurred for $V_{B} < 0$ , where electrons from the tMoSe $_{2}$ CB tunnel into the tip, whose Fermi level ( $E_{F}$ ) lies within the tMoSe $_{2}$ band gap (hence the term “ingap”) (Fig. 1G) (29–31, 33). The dark region bracketing $V_{B} = 0$ in Fig. 1E represents a tunnel gap of width $\Delta V_{B}$ , where STM current does not flow. This occurs owing to a combination of band-bending from work function mismatch between the tip and the surface, contact resistance between graphite and tMoSe $_{2}$ , and correlated charge gaps (29, 33, 41, 42). Enhancements in $\Delta V_{B}$ at particular $V_{G}$ values (white arrows) align with commensurate fillings of the moiré superlattice, as labeled in Fig. 1E [see details in section 3 of (38)]. We attribute these increases in $\Delta V_{B}$ to correlated charge gaps characteristic of insulating GWC and MI states, which require additional energy to create charged excitations (34). The charge gaps are broadened in $V_{G}$ because of the presence of sample inhomogeneities and tip-gating effects (42).

Images of these GWC and MI states and their corresponding structure factors, $S(\boldsymbol{k})$ , can be seen in Fig. 2 for $1/3 \leq v \leq 2$ [raw images shown in fig. S1 of (38)]. We minimized the electric field between the STM tip and tMoSe $_2$ by tuning $V_{\text{B}}$ to reduce tip perturbation effects [section 4 of (38)] (29–31, 33). GWCs at $\nu = 1/3$ and 4/3 show triangular lattices (Figs. 2, A and I), GWCs at $\nu = 1/2$ and 3/2 show stripe order (Figs. 2, B and J), and GWCs at $\nu = 2/3$ and 5/3 show honeycomb lattices (Figs. 2, C and K). The corresponding structure factors show the GWC Bragg peaks (circled in green) and moiré Bragg peaks (circled in purple), the latter of which are also higher-order GWC Bragg peaks. Strain-induced anisotropy causes the stripe order at $\nu = 1/2$ and 3/2 to align with the direction where electron-electron separation is greatest [section 5 of (38)]. The GWC patterns for $\nu \leq 1$ are similar to those imaged previously using a graphene sensor layer device geometry in tungsten disulfide (WS $_2$ )/tungsten diselenide (WSe $_2$ ) heterobilayers (18, 34) but with improved spatial resolution because here, STM imaging was performed on the bare TMD surface. The GWCs imaged for fractions $\nu' > 1$ resembled the $\nu = \nu' - 1$ GWCs except for an additional background of one electron per moiré site. Integer fillings $\nu = 1$ and 2 (Figs. 2, D and L) exhibited triangular lattices identical to the moiré superlattice corresponding to Mott and band insulator states, respectively (21–24). The moiré sites at $\nu = 2$ appeared larger than those at $\nu = 1$ sites, but the individual electrons at $\nu = 2$ could not be resolved [unlike in tWS $_2$ (33)], presumably owing to the relative contributions of the intrasite electron-electron interactions and moiré potential energy level separation (40, 43).

Fig. 1. Device geometry and STM measurement scheme. (A) Schematic of the tMoSe $_2$ device. A \~57.4°-twisted homobilayer of MoSe $_2$ is placed on top of a hBN dielectric on a SiO $_2$ /Si substrate. A bias voltage ( $V_B$ ) is applied between the grounded STM tip and the graphite nanoribbon array contacting the tMoSe $_2$ . A back gate voltage ( $V_G$ ) is applied between the tMoSe $_2$ and the Si substrate. (B) Large-area topographic map of the tMoSe $_2$ moiré superlattice, where Z denotes the topographic height (current $I = 1$ nA, $V_B = 1.5$ V, $V_G = 60$ V). (C) Close-up of the topography within the white-dashed region in (B) with the same scan parameters. (D) The atomic stacking configurations of the high-symmetry moiré unit cell regions identified in (C) (blue, Mo; red, Se). (E) Constant-height gate-sweep $I-V_B$ curves acquired with the tip above an MM site. Correlated insulating gaps are indicated in the plot (white arrows). The gap at $\nu = 5/3$ appears suppressed because the tip is on top of a doubly occupied MM site in the $\nu = 5/3$ honeycomb pattern (setpoint: $I = 5$ nA, $V_B = 1$ V, $V_G = 70$ V). (F and G) Schematic diagrams of (F) “direct” tunneling ( $V_B > 0$ ) and (G) “in-gap” tunneling ( $V_B < 0$ ) techniques. All STM data were taken at $T = 4.8$ K.

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Electron-hole asymmetry in GWC quantum melting

Quantum melting of the v = 2/3 GWC as a function of electron density is shown in Fig. 3. In the hole-doped GWC regime (v = 2/3 - δ = 0.61; Fig. 3A), we observed a disordered phase with spatially and dynamically inhomogeneous local electron density characterized by telegraph noise that depends on position and v [section 6 of (38)]. The site-to-site variations in tunnel current in the disordered pattern were found to be uncorrelated with the positions of point defects [section 9 of (38)]. As the electron density increased to $\nu = 0.63$ , a honeycomb pattern began to emerge (Fig. 3B), and by $\nu = 0.66$ , the pattern shifted by one lattice site and solidified into a more stable honeycomb charge order (Fig. 3C). The uniform charge density in the bottom left corner shows a melted region, with a green line drawn to mark the domain wall melting front. Upon further electron-doping ( $\nu > 0.66$ ), this domain wall advanced from the bottom left to the top right of the image until the electron density was uniform across the region (Figs. 3, D to F, and fig. S2). No telegraph noise was observed in the uniform electron-doped phase. The motion of the melting front followed the strain gradient of the moiré lattice (Fig. 3G) because local regions with smaller unit cells require higher charge density to reach the same $\nu$ [details in section 7 of (38)]. The pronounced difference in charge distribution between the hole- and electron-doped cases is further quantified in Fig. 3H, which shows the integrated intensity of the GWC Fourier peaks in $S(\pmb{k})$ , $\rho_{\mathrm{g}}$ , as a function of $\nu$ . Near $\nu = 2/3$ , $\rho_{\mathrm{g}}$ exhibited a maximum due to robust honeycomb order (Fig. 3H, inset) and then decayed sharply as $\nu$ was further increased. As $\nu$ was decreased below $\nu = 2/3$ , on the other hand, $\rho_{\mathrm{g}}$ decayed more gradually. The slight dip in $\rho_{\mathrm{g}}$ at $\nu \sim 0.64$ corresponds to an unstable transition between two honeycomb-ordered states shifted by one lattice site, which briefly weakens long-range order.

Similar doping asymmetry in quantum melting was seen for the stripe-ordered GWC at v = 1/2 (Fig. 4). Here, the hole-doped regime (v = 1/2 - δ =

0.46) exhibited disorder characterized by site-to-site intensity variations, short-range stripes, columnar dimers, and small remnant $\nu = 1/3$ triangular domains (Fig. 4A). As in the $\nu = 2/3 - \delta$ case, the disordered electron density at $\nu = 1/2 - \delta$ was uncorrelated with the locations of point defects [section 9 of (38)]. The short stripes seen in the hole-doped regime elongated as the electron density reached $\nu = 1/2$ (Fig. 4B), at which point, two large, well-ordered striped GWC domains crystallized, separated by a disordered boundary. The two domains were shifted relative to each other by one moiré lattice site, likely owing to different defect-induced pinning potentials. In contrast to hole-doping, electron-doping the striped GWC ( $\nu = 1/2 + \delta = 0.58$ ) caused the stripe order to melt into a uniform state through the progression of a domain wall melting front that follows the strain gradient (Fig. 4C; the full $\nu = 1/2$ melting series is shown in fig. S3).

Inspection of $S(\mathbf{k})$ for v = 1/2 - δ showed that hole doping splits the striped GWC Fourier peaks, consistent with the emergence of short-range nematic order (Fig. 4D, blue dashed ellipses). As $v \rightarrow 1/2$ , the split peaks merged, indicating stripe elongation to more robust stripe order (Fig. 4E). The electron-doped behavior was very different, as the intensity of the stripe-order peaks decreased monotonically for $v = 1/2 + \delta$ rather than splitting (Fig. 4F). This is highlighted in Fig. 4G, which shows linecuts through the stripe-order peaks in $S(\mathbf{k})$ along q (upper inset) as v is varied. The splitting on the hole-doped side corresponds to $\Delta q = 1/l_{s}$ , where $l_{s} \sim 20$ nm (2 to 3 moiré lattice constants; lower inset) is the average length of the shortened stripes. This electron-hole asymmetry is also seen in the integrated intensity of the stripe-order $S(\mathbf{k})$ peaks, which exhibits a shoulder (blue arrow) only on the hole-doped side owing to the presence of short-range stripe order (Fig. 4H).

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Quantum melting of the v = 1 Mott insulator

The electron-hole asymmetry seen in quantum melting for $\nu < 1$ GWCs was absent for quantum melting of the v = 1 MI state (Fig. 5). The MI state instead melted into spatially uniform states for both doping polarities, with no electronic disorder. This can be seen in the in-gap tunnel current map taken near v = 1 (Fig. 5A), which exhibits three regions with distinct electron occupancy caused by strain-induced inhomogeneity: (i) $v = 1 - \delta \approx 0.95$ (bottom), (ii) $v \approx 1$ (middle), and (iii) $v = 1 + \delta \approx 1.10$ (top). The proposed band alignments for these states are sketched in Fig. 5B. Region (ii) is dark and featureless because the filling corresponds to a gapped MI state and both the tip and sample Fermi energies lie within the Mott gap (this differs from Fig. 2D, which was acquired at a more negative $V_{B}$ , allowing electrons in the MI to tunnel into the tip). Region (i), on the other hand, is hole-doped relative to v = 1, causing the Mott gap to collapse and form a compressible state where electrons can freely tunnel to the tip. The Mott gap similarly collapses in region (iii), except now, the sample is electron-doped with v > 1. The melted states were spatially uniform for both doping polarities, and there were no signs of doping-induced electronic disorder (see fig. S4 for large-scale images). Electron-doped sites in region (iii) appear larger than those in region (i) owing to the increased probability of containing a second electron.

Fig. 2. Images of GWC and MI states. (A to D) In-gap tunnel current maps of correlated insulator states in tMoSe $_{2}$ for (A) v = 1/3, (B) v = 1/2, (C) v = 2/3, and (D) v = 1. Corresponding structure factors, S(k), are shown in (E to H). (I to L) Current maps of states observed for v > 1 are shown for (I) v = 4/3, (J) v = 3/2, (K) v = 5/3, and (L) v = 2. Corresponding structure factors, S(k), are shown in (M to P). Fourier peaks in S(k) associated with the triangular moiré lattice and GWC order are circled in purple and green, respectively. A plane has been subtracted from the raw STM images; raw data are shown in fig. S1. All S(k) maps were calculated from full-size autocorrelation functions using uncropped in-gap tunnel current maps.

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Discussion and outlook

Our data show a pronounced electron-hole asymmetry for GWC quantum melting: Hole doping GWCs produced electronic disorder that is uncorrelated with quenched disorder, whereas electron doping GWCs yielded uniform, liquid-like phases. This is consistent with previous optical measurements (27) that have detected asymmetry in GWC quantum melting in $WS_{2}/WSe_{2}$ heterobilayers doped near v = 1/2. Theoretical studies using both classical (12, 27, 35) and quantum (6, 7) models have also predicted different incommensurate phases, from Fermi liquids (6, 44) to disordered states arising from competing charge orders that are roughly consistent with our observations (5–7). However, none of the previous theoretical or experimental studies clearly captured the pronounced electron-hole melting asymmetry that we observed. To explain this behavior, we performed self-consistent Hartree-Fock (SCHF) calculations that solve an extended Hubbard model consisting of electrons on a triangular lattice at fillings near $\nu = 1/2$ and 2/3. Our treatment provides a framework that shows how the particle-hole asymmetry of the moiré triangular lattice (45) gives rise to the GWC melting asymmetry that we observed experimentally.

Fig. 3. Quantum melting of the v = 2/3 GWC. (A to F) In-gap tunnel current maps near the v = 2/3 filling for (A) v = 0.61, (B) v = 0.63, (C) v = 0.66, (D) v = 0.68, (E) v = 0.70, and (F) v = 0.72. A domain wall (green line) separates melted and charge-ordered regions. (G) Map of the moiré unit cell areas in the same region as that from (A) to (F) with a 10-nm scale bar. (H) The integrated intensity, $\rho_{g}$ , of the honeycomb-order GWC Fourier peaks (inset, blue circles) is shown as a function of v ( $\rho_{g}$ is normalized by the integrated intensity of the moiré Fourier peaks). (I) SCHF bands at v = 2/3 along the path K-Γ-K' in the rBZ. The rBZ is shown in the inset (solid line) with the moiré Brillouin zone for reference (dashed line). At v = 2/3, the chemical potential $\mu_{v} = 2/3$ (dashed red line) lies between the LHB and UHB. Electrons doped above v = 2/3 occupy the rBZ edges (filled circles), whereas hole doping removes electrons from the rBZ center (open circles).

E

H

Fig. 5. Quantum melting of the v = 1 MI state. (A) In-gap tunnel current map near v = 1. Strain variation leads to three distinct doped regions: (i) $\nu = 1 - \delta \approx 0.95$ , (ii) $v \approx 1$ , and (iii) $v = 1 + \delta \approx 1.10$ , where v is estimated from average unit cell area in the bracketed regions. Region (ii) appears dark because the tip Fermi level lies within the Mott gap, unlike for Fig. 2D, which was acquired with a more negative $V_{B}$ . (B) Schematic of the sample and tip density of states (DOS), showing their energy level alignments in the three regions: For region (ii), the sample and tip chemical potentials both lie in the MI energy gap, and no in-gap tunneling occurs. For regions (i) and (iii), charge doping the MI causes the Mott energy gap to collapse, and in-gap tunnel current is able to flow.

Our starting point is to think of the v = 2/3 GWC as a charge density wave (CDW) on a triangular lattice that folds the single, partially occupied moiré conduction band into three bands within a reduced Brillouin zone (rBZ). For v = 2/3, the chemical potential lies between the top two folded bands (Fig. 3I; spin was ignored in this treatment). Solving an extended Hubbard model within SCHF, we found that the CDW potential opens a correlated gap along the rBZ edges between the top two bands [i.e., the lower- and upper-Hubbard bands (LHB and UHB, respectively)], which reduces the system's overall energy. The resulting electron-hole asymmetric band structure exhibits an indirect gap between the LHB and UHB. Electron doping the UHB populated states along the rBZ boundary (near K and $K'$ ), which destabilized the v = 2/3 CDW because the system could then reduce its energy by closing the CDW gap and melting into a liquid state. By contrast, hole doping the LHB emptied states near the zone center (near $\Gamma$ ) and therefore left the CDW gap in place and the charge order partially intact. The asymmetry in the GWC order parameter

Fig. 4. Quantum melting of the v = 1/2 GWC. (A to C) In-gap tunnel current maps near the v = 1/2 filling for (A) v = 0.46, (B) v = 0.50, and (C) v = 0.58. The corresponding structure factors, $S(\boldsymbol{k})$ , are shown in (D to F) [dashed blue ellipses highlight the stripe-order Fourier peaks used to calculate $\rho_{g}$ in (H)]. (G) Linecuts through stripe-order Fourier peaks in $S(\boldsymbol{k})$ as a function of v. (Upper inset) The red dashed line indicates the direction of linecuts along the q axis. (Lower inset) The linecut at v = 0.45 (black dashed line) shows splitting of Fourier peaks. (H) Integrated intensity of the stripe-order Fourier peaks in blue ellipses, $\rho_{g}$ , as a function of v. $\rho_{g}$ is normalized by the integrated intensity of the moiré Fourier peaks. An asymmetric shoulder on the hole side of v = 1/2 is indicated by the blue arrow.

$(\rho_{\mathrm{g}})$ observed experimentally (in Fig. 3H) was qualitatively reproduced by our SCHF calculations (fig. S11). The case for $\nu = 1/2$ is similar, as discussed in section 8 of (38). This mechanism also accounts for the lack of electron-hole asymmetric melting for the MI state, given that there is no spontaneously generated CDW at $\nu = 1$ .

Electron-doped GWCs thus melt into uniform phases because the CDW gap collapses, yielding liquid-like states stabilized by quantum fluctuations that favor electron delocalization (6, 44, 46). Hole-doped GWCs, on the other hand, retain a finite correlated CDW gap, giving rise to disordered states that reflect the competition between different charge orders. Our data suggest that the disordered states that we observed are driven by electron-electron interactions, as we found no correlation between site-to-site variations in the tunnel current intensity and the spatial configuration of point defects. Telegraph noise (a sign of competing orders) was also seen only in the hole-doped case. The disorder that we observed for hole-doped v = 1/2 and 2/3 GWCs is additionally consistent with theoretical predictions for disordered “electron-slush” states (5–8, 10) at incommensurate fillings even in the absence of quenched disorder. Classical Monte Carlo simulations, for example, predict a splitting of $S(\boldsymbol{k})$ stripe-order peaks at $v = 1/2 - \delta$ owing to interaction-driven short-range nematic disorder, in agreement with our experiment (Fig. 4, D and G) (12, 27, 35).

Although electron-electron correlations drive the disordered state, it is likely that intrinsic material disorder stabilizes the interaction-driven disorder. We did not observe hysteresis in the electronic disordered patterns upon sweeping the back gate voltage, implying that quenched disorder pins a small subset of the otherwise large number of degenerate disordered states. The experimentally observed telegraph noise likely arises from fluctuations between these competing ground states (Fig. 3, A and B, and fig. S9). Our data are consistent with previous theoretical predictions that quenched disorder should stabilize interaction-driven “electron slush” phases (7, 47).

We observed pronounced electron-hole asymmetry for GWC quantum melting at v = 1/2 and 2/3, with hole doping favoring electronic disordered states and electron doping favoring liquid-like states. This asymmetry can be explained at the level of SCHF theory as arising from differences in momentum-space geometries for electron versus hole pockets that strongly affect GWC stability. Our results show how new electronic disordered phases can arise from electron-electron interactions even in the presence of quenched disorder. Future temperature-dependent and dynamical measurements should help to quantify the energetics of correlation-driven electronic disordered states.

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ACKNOWLEDGMENTS

We acknowledge helpful discussions with V. Dobrosavljević and experimental advice from Z. Ge, Z. Xiang, and Q. Li. Funding: US Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division contract DE-AC02-05-CH11231 within the van der Waals heterostructure program KCWF16 (M.F.C., F.W., M.P.Z.: STM imaging, SCHF theory). Department of Defense Vannevar Bush Faculty Fellowship N00014-23-1-2869 (M.F.C.: device fabrication). National Science Foundation award DMR-2528960 (M.F.C.: telegraph noise analysis). National Science Foundation Graduate Research Fellowship Program under grant no. DGE 2146752 (E.B.). Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) project no. 529232793 (L.S.: postdoctoral fellowship). National Science Foundation MRSEC DMR-2308817 (M.H.N.). Texas Advanced Computing Center (TACC) at The University of Texas at Austin (M.H.N., R.D.: DFT computation). Stampede3 computational facilities at The University of Texas at Austin through allocation PHY250206 from the Advanced Cyberinfrastructure Coordination Ecosystem: Services and Support (ACCESS) program, which is supported by National Science Foundation grants 2138259, 2138286, 2138307, 2137603, and 2138296 (M.H.N., R.D.: DFT computation). Texas Quantum Institute Graduate Fellowship (R.D.). JSPS KAKENHI grants 21H05233 and 23H02052 (K.W., T.T.: hBN crystal fabrication). CREST grant JPMJCR24A5 (K.W., T.T.: hBN crystal characterization). JST and World Premier International Research Center Initiative (WPI), MEXT, Japan (K.W., T.T.: hBN synthesis development). Author contributions: Conceptualization: M.F.C., F.W.; Supervision: M.F.C., F.W.; Device fabrication: E.B., M.A., G.N., S.K.; hBN crystal growth and characterization: K.W., T.T.; Measurements: E.B., M.A., L.S., G.W.; SCHF calculations: Z.D., T.W., M.P.Z.; DFT electronic structure calculations: R.D., M.H.N.; Data analysis: E.B., M.A., L.S.; Writing: E.B., M.A., L.S., M.F.C. Competing interests: The authors declare that they have no competing interests. Data, code, and materials availability: All data shown in the main text and supplement are available on Zenodo (48). Details for the synthesis and characterization of all compounds and materials are available in the methods section (38). License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.aee6967

Materials and Methods; Supplementary Text; Figs. S1 to S12; Tables S1 and S2;

References (49–63)

Submitted 18 December 2025; accepted 18 August 2026

GLACIAL INCEPTION

Late Holocene reexpansion of the Laurentide Ice Sheet

Nicolás E. Young $^{1*}$ , Gifford H. Miller $^{2,3}$ , Martha Raynolds $^{4}$ , Helga Bueltmann $^{5}$ , Scott J. Lehman $^{2}$ , Jonathan H. Raberg $^{2\dagger}$ , Kylie Seward $^{6}$ , Simon L. Pendleton $^{7}$ , John T. Andrews $^{2,3}$ , Patrick J. Webber $^{8}$ , Joerg M. Schaefer $^{1,6}$

During interglaciations, the Laurentide Ice Sheet (LIS), which is the largest of the Pleistocene ice sheets, retreats to Arctic Canada, where it achieves a minimum configuration. The reexpansion of the LIS following this minimum marks the start of the next glaciation. Here, we show that the last remaining remnant of the most recent LIS, Barnes Ice Cap (Baffin Island, Canada), achieved its minimum interglacial dimensions after \~3.6 thousand years ago, before reexpanding \~2000 years ago, marking the onset of the next glaciation. The new LIS reached maximum dimensions in \~1960 CE, after which anthropogenic summer warming resulted in a negative mass balance, ice margin recession, and the termination of the next glaciation. The demise of the next glaciation, despite the ongoing decline in summer insolation, illustrates the influence of anomalous greenhouse gas forcing on climate.

Cyclic glacial-interglacial variations of up to 2 per mil ( $\%$ o) in benthic $\delta^{18}\mathrm{O}$ records from Earth's oceans have been driven largely by changes in terrestrial ice volume over the course of the Quaternary Period (2.58 million years ago to present), with the Laurentide Ice Sheet (LIS) exerting the largest influence [up to $\sim 80$ -m sea level equivalent ice volume; (1-3)]. Following maxima, the LIS retreated northeasterly into the Eastern Canadian Arctic, achieving interglacial minima, before reexpanding at the onset of the next glacial cycle (4-7). Terrestrial evidence of ice sheet minima and subsequent ice sheet regrowth (i.e., glacial inception), however, has largely been destroyed by repeated glaciations or rests beneath modern ice sheets, making it difficult to gain insight into when exactly an ice sheet begins its millennial-scale march toward the next Quaternary glacial maximum. Models indicate a likely origin of glaciations over Baffin Island in the Eastern Canadian Arctic (4, 5, 7, 8), and today, Baffin Island hosts Barnes Ice Cap (BIC; Fig. 1), which is the last remaining remnant of the LIS that has survived the present interglacial period [the Holocene; 11.7 thousand years ago (ka) to present]. Located on the central Baffin Island plateau (Fig. 1), BIC contains three generations of ice based on $^{18}\mathrm{O}$ values: interglacial Holocene ice at the surface, ice from the last glacial period below Holocene ice, and, at the bottom, older ice with $^{18}\mathrm{O}$ values similar to Holocene values (9). Thus, the BIC preserves the last remaining remnants of the LIS and evidence of past LIS regrowth, supporting the long-held hypothesis that the central Baffin Island plateau is a primary inception point for continental-scale glaciation (6, 10-12).

BIC is particularly climate sensitive because unlike other extant ice caps in the Canadian Arctic that rest on high-elevation bedrock (>1500 m above sea level), BIC rests on low-elevation bedrock (\~500 m above sea level). Only the thickness of BIC itself (\~700 m) enabled the ice surface to, until recently, intersect the regional snowline, allowing for its preservation (13). For example, \~35% of the BIC surface area was above the mean 1960–1980 CE snowline, whereas by the early 2000s, only \~3% remained above the mean 2000–2012 CE snowline, followed by the loss of the BIC accumulation area since 2010 CE (13). Between \~1960 CE and 2022 CE, the BIC margin retreated \~200 to 800 m, exposing a distinctive swath of terrain containing vegetation killed by an initial phase of LIS expansion following its interglacial minimum configuration and reexposed by its subsequent contemporary retreat (Fig. 1). We capitalize on two new datasets—in situ $^{10}$ Be measurements from bedrock and erratic boulders in the BIC forefield and radiocarbon ages on entombed vegetation that have emerged from beneath the receding BIC margin—to constrain the final episode of LIS retreat and the reversal to LIS growth. Here, we show that as snowline descended and intersected the Baffin plateau \~2 ka, the LIS mass balance turned positive and began to reexpand, marking the natural inception of the next glaciation. LIS regrowth continued until \~1960 CE, when increased melt from contemporary summer warming turned mass balance negative, driving ice cap retreat.

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Ice margin chronology

The BIC forefield hosts an abrupt trimline marking the \~1960 CE historical maximum BIC margin [see supplementary materials (SM)]. The 1960 CE trimline is marked by a sharp tonal change between lichenated and vegetated bedrock terrain outside of trimline versus terrain that hosts little live vegetation between the trimline and modern ice margin (Figs. 1C and 2 and figs. S1 to S3). This distinct tonal trimline serves as a key temporal boundary between the landscape that was deglaciated during the Holocene and the landscape immediately inside the trimline, which deglaciated in the Holocene but became reglaciated as BIC readvanced toward the 1960 CE margin. In addition, the absence of a depositional moraine indicates the presence of cold-based to polythermal ice at the base of BIC (13, 14). Cold-based ice caps are widespread across the Arctic, and because cold-based ice is frozen to its bed, basal sliding is negligible and ice cap evolution is controlled primarily by climate-driven changes to surface mass balance (15–18). The absence of basal sliding in our field area allows BIC to act as a preservation agent instead of an erosive agent as the ice margin readvances (18–20).

First, we constrained when the LIS retreated across the modern BIC forefield in the Holocene. New ${}^{10}$ Be surface exposure ages from erratic boulders in an extensive moraine system located \~7 to 9 km from the modern BIC margin (n = 10; Fig. 1C, figs. S1 and S4, and tables S1 and S2), bedrock surfaces located immediately outside the 1960 CE historical trimline (n = 13), and bedrock surfaces inside the trimline (n = 12) all statistically overlap (Figs. 1C and 3 and table S1). Overlapping ${}^{10}$ Be ages on all three morphostratigraphic units indicate that the LIS retreated relatively quickly across the landscape and behind its 2022 CE margin at $3.56 \pm 0.24$ ka before present (BP) (equivalent to 1950 CE; see SM for details; Figs. 1C and 3, fig. S5, and table S1). This age is consistent with local minimum-limiting radiocarbon ages of $3275 \pm 420$ and $4110 \pm 670$ calibrated years BP (Fig. 1C and table S3) and individual ${}^{10}$ Be ages of $3.59 \pm 0.22$ ka BP and $3.24 \pm 0.31$ ka BP from the northern end of BIC (21)

Next, we constrained the timing of BIC readvance after deglaciation of the forefield at $3.56 \pm 0.24$ ka BP. Because BIC is frozen to its bed in our study region (13, 14), we hypothesized that ${}^{14}C$ dates on preserved in situ dead moss and woody plants would constrain periods of BIC expansion. Collections of in situ dead moss and vegetation adjacent to cold-based ice caps have been used for decades to reconstruct ice margin change on Baffin Island (18–20, 22–24). We first adopted the well-established strategy of collecting samples within a few meters of an ice margin, where each radiocarbon age is a kill date defining when ice advanced over that specific site (18, 20, 25). In addition, recent work has demonstrated that a transect of ${}^{14}$ C dates from in situ dead moss and vegetation extending away from the ice margin can constrain the timing of ice advance toward the eventual historical maximum extent (23). Eighty-eight new calibrated radiocarbon ages on previously ice-entombed in situ vegetation collected at or near the 2022 CE margin (table S4 for distances) are equally distributed across the southern and northern domes of BIC and constrain the widespread regrowth of a renewed LIS (Figs. 1, B and C, and 2; fig. S6; and table S4). Approximately 70% (n = 64) of our radiocarbon measurements have median ages $1800 \pm 200$ CE, indicating that these plants were killed near the culmination of the Little Ice Age, during what were likely the coldest summers of the Common Era between 1780 and 1880 CE [(18, 26); Figs. 2 and 3 and table S4; see SM for calibration discussion]. Radiocarbon ages do not differ between domes, suggesting that any differences in ice margin change between the northern and southern domes is likely negligible despite slight differences in aspect, ice velocity, ice thickness, and mass balance (13).

Fig. 1. The last remnant of the LIS. (A) Areal extent of the North American Ice Sheet Complex at the Last Glacial Maximum \~22 ka calibrated BP (42). The LIS is contiguous with the much smaller Cordilleran Ice Complex (CIC) to the west and Greenland Ice Sheet (GrIS) to the east. (B) BIC on Baffin Island (2015 CE Landsat composite image). Yellow and pink circles mark locations of new $^{10}$ Be and entombed plant radiocarbon dates (tables S1 and S4). Previously published $^{10}$ Be (yellow diamonds) and radiocarbon ages (pink diamonds) indicate that the paleo-LIS was nearing the dimensions of the modern-day BIC \~4 ka BP. Location 1: 3240 ± 310 years BP (21); location 2: 3590 ± 220 years BP (21); location 3: 4290 ± 520 and 4180 ± 460 years BP (43); location 4: 4040+380/–400 years BP (61). Radiocarbon ages from entombed plants from the plateau ice caps (green diamonds; Fig. 3) constrain the initial intersection of regional snowline with the landscape to just before or early in the Common Era (18). (C) Primary field area along the southeastern margin of BIC with the positions of the \~1960 CE historical maximum extent (blue dashed line), paleo-shoreline of the former proglacial lake filling the valley during BIC retreat (white dashed line), and prominent cross-valley moraines described in a previous work [(61); September 2024 CE Landsat image]. $^{10}$ Be ages (yellow circles; 1σ uncertainties; outliers in italics; figs. S4 and S5) suggest rapid retreat of the ice margin through this valley and inside the 2022 CE ice margin \~3.6 ka BP, consistent with previously published radiocarbon constraints [pink diamonds; calibrated years BP; (61)]. Median calibrated ages in calendar years are shown for new radiocarbon dates on recently exposed plant material along the BIC margin (pink dots; Fig. 2 and table S4); additional new radiocarbon ages are shown in Fig. 2.

A subset of our ${}^{14}$ C dates provides a longer record of LIS reexpansion. We collected a series of samples (n = 16) along an \~800-m transect between the historical maximum trimline and a segment of the 2022 CE BIC margin that has retreated $\sim$ 400 m more than the adjacent ice margin [(27); Fig. 2]. Enhanced localized retreat of this segment of the BIC margin was driven by a small, now drained, proglacial lake, which allowed us to capture a longer record of ice advance (Fig. 2). As seen with glaciers elsewhere on Baffin Island, radiocarbon ages along this transect become progressively younger with increasing distance from the ice margin, consistent with an advancing ice front (23). The oldest of these radiocarbon ages, adjacent to the ice margin and $\sim$ 700 to 750 m from the trimline, indicate that the new LIS began advancing toward the historical maximum extent $\sim$ 1000 CE (Fig. 2). Two $^{14}$ C dates from the same location $\sim$ 150 m from the historical trimline have median calibrated ages that differ by 300 years (1530 and 1830 CE; Fig. 2, A and C, and table S4). One possibility is that there was an episode of BIC expansion at $\sim$ 1450 to 1500 CE, as constrained by seven $^{14}$ C dates in our transect (Fig. 2), slight ice recession, followed by ice reexpansion in the early 1800s CE. Our two samples at the same location with discordant $^{14}$ C dates highlight that the BIC margin likely experienced several episodes of retreat and advance. These small fluctuations, however, occurred during a period of overall net ice expansion after $\sim$ 1000 CE, as required by our $^{14}$ C kill dates.

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The LIS Holocene minimum, reexpansion, and contemporary retreat

Our ${}^{10}$ Be and ${}^{14}$ C datasets limit the minimum extent of the LIS to a $\sim$ 2.6-thousand year (kyr) window between 3.56 $\pm$ 0.24 ka BP and $\sim$ 1000 CE. We drew on additional datasets to further refine the timing of the LIS minimum. First, unless the LIS stopped precisely at the 2022 CE margin during initial retreat at 3.56 $\pm$ 0.24 ka BP, ice reexpansion must have occurred before $\sim$ 1000 CE. Plants older than $\sim$ 1000 CE, however, remain ice covered today, and only continued retreat of BIC will expose them. Next, an extensive series of ${}^{14}$ C dates from ice-entombed vegetation emerging from nearby independent ice caps and glaciers on the Baffin plateau [plateau ice caps (PICs)] provide

additional insights into the likely pre-1000 CE timing of LIS expansion (Figs. 1B and 3). Of the $186^{14}\mathrm{C}$ dates comprising this dataset (18), none predate the Common Era. The lack of a single pre-Common Era ${}^{14}\mathrm{C}$ date indicates that it was not until just before or early in the Common Era (i.e., $\sim 2$ ka BP) that regional snowline intersected the central Baffin Island plateau [ $\sim 800\mathrm{m}$ above sea level; (18)], including the paleo-LIS, triggering widespread ice cap and glacier inception or expansion. Combined, these additional lines of evidence indicate that the LIS stabilized between $\sim 3$ and $2\mathrm{kaBP}$ -its true minimum configuration at dimensions smaller than those today—before beginning reexpansion $\sim 2\mathrm{kaBP}$ (Figs. 3 and 4).

The PIC dataset also includes distinct clusters of ${}^{14}$ C kill dates between \~250 and 450 CE, 850 and 1000 CE, and 1250 and 1450 CE that define additional pulses of regional snowline lowering (18). Conversely, the PIC dataset does not contain the primary peak in ${}^{14}$ C kill dates centered on 1800 ± 200 CE that is present in the BIC dataset (Fig. 3). The differing ${}^{14}$ C peaks across the PIC and BIC datasets are due to the magnitude of ice cap retreat combined with vegetation sampling strategies. Both the PICs and BIC have retreated from their respective historical maximum extents. However, because PICs are relatively thin with less ice mass and thus have faster response times to climate forcing (15, 18, 28), they have retreated more than BIC from their historical maximum extents. Entombed vegetation is primarily collected directly adjacent to modern ice margins, and thus older ${}^{14}$ C dates are to be expected adjacent to the margins of PICs. Although the \~1800 CE peak is absent from the PIC dataset, it was predicted from large regions at elevations lower than those of extant ice caps that are devoid of dense plant cover that represent ice cap expansions to their lowest elevations during what were the coldest summers of the Little Ice Age around \~1780 to 1880 CE (18, 26, 29). Nonetheless, pulses of snowline lowering \~250 to 450 CE, 850 to 1000 CE, and 1250 to 1450 CE likely drove the continued reexpansion of the LIS, and we note that both the PIC and BIC records share the peak in kill dates \~1450 CE, which is suggestive of a common climate forcing across the region (Fig. 3). These intervals of snowline lowering correspond to terrestrial proxy and modeled temperature cooling trends over the past 2 kyr, consistent with modern observations that reveal summer temperature as the primary driver of glacier change on Baffin Island [Fig. 3; (17, 18, 30–32)].

A

B

Fig. 2. BIC radiocarbon data. (A) Locations of an \~800-m sampling transect from the ice margin to the \~1960 CE historical maximum extent (blue dashed line) as seen on QuickBird-2 imagery (©2011 Vantor). Values are median calibrated radiocarbon ages in calendar years CE; sample IDs are in parentheses (table S4). Samples marked with an asterisk are not part of the primary transect shown in (C) but are shown here for completeness. Here, the BIC margin is \~400 m more recessed than the adjacent margin owing to the influence of a now-drained proglacial lake (L) on retreat dynamics exposing the oldest plants found anywhere along the BIC margin. The broader BIC margin remained at its historical maximum extent until \~1960 CE, but at our transect site, retreat was underway by 1957 CE owing to the influence of the proglacial lake (see SM). (B) Probability density function of all radiocarbon dates on vegetation killed by the late Holocene readvance of BIC. (C) Median $^{14}\mathrm{C}$ dates from (A) plotted with distance from the 2024 CE ice margin. Stars mark the ice margin position from aerial or satellite imagery. Error bars represent the 1σ range in the calibration.

The renewed LIS was approaching its historical maximum trimline by $1800 \pm 200$ CE, and aerial photographs reveal isolated ice margin retreat in 1957 CE, with the broader BIC remaining at its historical maximum until \~1961 CE (see SM and figs. S2 and S3). These constraints are consistent with early glaciological studies indicating that the ice cap was in near-mass balance equilibrium at that time (13, 33, 34). Considering these historical constraints, we mark 1960 CE as the widespread onset of contemporary BIC retreat. Regional records show a notable increase in summer temperatures, beginning in the late 18th to early 19th centuries (Fig. 3). This warming drove the early recession for thin, low-elevation PICs, whereas the BIC remained at its historical maximum extent until \~1960 CE, likely reflecting the longer lag between a climate perturbation and ice margin response inherent to larger cold-based glaciers and ice caps in the Arctic (15, 28). Ice cap-specific glaciological properties or changes in precipitation patterns can also drive ice cap retreat, but since the early 1960s, BIC mass loss can be almost entirely explained by rising summer temperatures (17). Moreover, widespread retreat of ice caps across the Canadian Arctic Archipelago and the broader North Atlantic region suggests that retreat is driven by summer temperatures (16, 17, 35). The increase in summer temperatures is mirrored by the increase in net effective radiative forcing associated with the measured increase in well-mixed greenhouse gases (GHGs) since \~1750 CE [CO₂, CH₄, and N₂O; (36–39)]. The concentration of well-mixed GHGs had increased by only \~12 parts per million (ppm) carbon dioxide equivalent (CO₂e) between \~1750 and 1850 CE, coinciding with the disappearance of the lowest-elevation PICs (18). By 1960 CE, when BIC retreat was underway, GHGs had increased an additional \~50 ppm CO₂e, with an additional 138 ppm CO₂e by 2024 CE (Fig. 3).

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Holocene evolution of the LIS and glacial inception

Regional ice core and terrestrial proxy records indicate that the warmest temperatures of the Holocene at high northern latitudes coincided with peak summer boreal insolation \~11 to 10 ka BP, followed by net multicentennial-scale cooling as radiative forcing declined through the Holocene [Fig. 4; (24, 30, 40, 41)]. Yet despite this long-term cooling trend, the LIS retreated through the Holocene, and it was not until \~2 ka BP

that the LIS began to regrow (42–44). Retreat of the LIS through the Holocene indicates that the geometry of the LIS was out of equilibrium with climate; the surface elevation of the receding LIS was not high enough to maintain a positive mass balance, despite evidence that regional snowline had been lowering since \~9 ka BP and accelerating after \~5 ka BP [Fig. 4; (22, 24)]. The lag between initial snowline lowering \~9 ka BP and LIS reexpansion \~2 ka BP was magnified in part by extreme dynamical ice discharge during the late glacial and early Holocene (45), resulting in an ice sheet surface that was lower than what would be expected solely from climate forcing. Residual isostatic uplift raised the elevation of BIC \~20 m over the past 3 kyr, which would slightly improve its mass balance but likely not enough to explain the transition from recession to advance (46, 47). It was not until \~2 ka BP that snowline was sufficiently depressed to intersect the Baffin plateau, allowing the reexpansion of the LIS.

Recent temperature reconstructions using data assimilation techniques suggest that in contrast to cooling through the Holocene, surface temperatures were nearly flat or even rose through the Holocene [Fig. 4; (48–50)]. These reconstructions, however, either do not include terrestrial proxies or suggest that data assimilation approaches underestimate temporal variability and do not fully capture feedbacks in the climate system (50). Although these temperature trends could possibly explain the retreat of the LIS through the Holocene until \~2 ka BP, they likely cannot drive the late Holocene reexpansion of the LIS. In addition to late Holocene reexpansion of the LIS, glaciers across the Arctic and Northern Hemisphere experienced net advance through the Holocene (51, 52). This canonical pattern of long-term glacier expansion starting in the middle Holocene and culminating in the Little Ice Age across the Northern Hemisphere is difficult to reconcile with temperature reconstructions that show minimal temperature variability or warming through the Holocene.

A

C

E

Fig. 3. The Common Era. (A) Probability density functions of calibrated radiocarbon ages from the PICs (Fig.1B) and BIC. No radiocarbon age from the PICs predates the Common Era ( $n = 186$ ), indicating that the regional snowline did not begin to intersect the landscape (as needed to drive ice cap expansion) until the beginning of the Common Era (18). The BIC probability density function constrains the main pulse of ice advance to $1800 \pm 200$ CE. (B) Time-distance relationship (distance from 2024 CE ice margin) of ice margin advance along the transect of radiocarbon ages (dots) and historical constraints (stars) shown in Fig. 2C. (C) Estimated mean-annual temperature anomalies from the Agassiz ice core with $2\sigma$ uncertainties (shading) (30). (D) Community Earth System Model (CESM) past2ka modeled summer temperatures (50-year smooth) through the Common Era (32). Modeled temperatures are similar to Agassiz temperatures and suggest that the coldest summers of the Holocene occurred around 1780 to 1880 CE. (E) Measured atmospheric $\mathrm{CO}_{2}$ concentrations [symbols and black line; (62–64)] and well-mixed GHGs ( $\mathrm{CO}_{2}\mathrm{e}$ red line). WAIS, West Antarctic Ice Sheet. Blue bars highlight pulses of ice cap expansion across central-northern Baffin Island that are constrained by the PIC and BIC datasets coinciding with cool intervals displayed in both the Agassiz and CESM temperature records.

Late Holocene cooling driven by declining high-latitude Northern Hemisphere summer insolation and associated positive climate feedbacks is a necessary precursor to glacial inception, according to Milankovitch theory (50, 53). We suggest that the \~2-kyr expansion of the renewed LIS in the late Holocene represents the inception of the next glaciation. BIC retreat commencing around \~1960 CE, driven by anthropogenic summer warming, reversed a 2-kyr interval of advance, marking the termination of the next glaciation. A modest \~20-ppm CO₂e increase between \~8 and 2 ka BP coincides with the final interval of LIS recession, but this magnitude of CO₂e increase was insufficient to overtake insolation-driven regional cooling and the expansion of Baffin plateau ice caps, including the renewed LIS \~2 ka BP (Figs. 3 and 4). The BIC and PIC records of ice cap expansion highlight that the relatively low-relief central Baffin Island plateau is particularly vulnerable to modest snowline decline that rapidly expands permanent snow cover across the landscape. Associated changes in surface albedo led to strong positive feedbacks that likely accelerated the expansion of Arctic sea ice and further summer temperature decline over the past 2 kyr (18, 54). The Baffin Island plateau, coupled with the last remains of the LIS from the previous glaciation, provides the ideal setting for glacial inception and supports the long-held hypothesis of “instantaneous glacierization” as a key ingredient for the onset of glaciations (4, 11, 12).

Fig. 4. The past 11 kyr. (A) July insolation at 65°N (40). (B) Estimated mean-annual temperature anomalies from the Agassiz ice core with 2σ uncertainties (shading) relative to 1750 CE. Peak temperatures coincide with peak insolation, and the coldest temperatures immediately predate contemporary warming (30). (C) Summer (June to August) temperature reconstruction from central Greenland ice cores relative to 1860 to 2000 CE (41). (D) Last Glacial Maximum reanalysis (LGMR) (48) and Holocene (49) data assimilation (DA) products (relative to 1850–1900 CE) showing long-term Holocene warming or minimal change in contrast to regional records in (B) and (C). The shaded regions indicate 1σ uncertainty. (E) Atmospheric CO₂ concentrations and well-mixed GHGs (CO₂, CH₄, N₂O) over the past 11 kyr plotted as CO₂e relative to the lowest concentrations in GHGs occurring \~8.1 ka BP (36–39). (F) Areal extent of the North American Ice Sheet Complex (NAISC) with minimum and maximum estimates (error bars); this record is almost entirely dominated by the LIS beginning \~10 ka BP (42). (G) Probability density functions (PDFs). Radiocarbon ages from entombed vegetation constrain the first pulse of Holocene snowline lowering over Baffin Island to \~9.3 ka BP [blue; (24)]. $^{10}$ Be ages constrain retreat of the paleo-LIS margin to inside the 2022 CE ice margin extent 3.56 ± 0.24 ka BP (this study; red lines are individual $^{10}$ Be ages, and the black line is the summed distribution; fig. S5), with LIS reexpansion likely beginning \~2 ka BP [green PDF; this study and previous work (18)] and ice approaching its modern margin by \~1000 CE (pink PDF; this study).

As atmospheric $CO_{2}$ concentrations continue to increase, a return to glacial conditions is extremely unlikely (55, 56), but our new paleo-LIS dataset informs ongoing discussion as to when, and how, a glacial inception would have occurred in a preindustrial climate state. Previous modeling work suggests that the next glacial inception would not have occurred for several thousand to tens of thousands of years. But importantly, inception is most often defined by Northern Hemisphere ice sheets with several meters of sea level equivalent (56–59). True glacial inception, however, would never be recognized by this traditional threshold marker of paleo-glacial times, because this definition cannot capture the first instance of post-interglacial ice sheet expansion. A previous work (60) explored empirical relationships between orbital parameters and benthic ocean $\delta^{18}O$ values to suggest that peak interglacial conditions occurred 1.8 to -0.1 ka BP. Peak interglacial conditions were defined as the predicted change from decreasing to increasing $\delta^{18}O$ values, that is, the first instance of ice sheet growth. The timing of this predicted transition is markedly similar to our new direct geological observations that reveal that a renewed LIS began to regrow around $\sim2$ ka BP, marking the inception of the next glaciation (Fig. 4).

The landscape just emerging from beneath BIC provides insights into the LIS's most recent deglaciation history, its minimum interglacial configuration, and the timing of glacial reexpansion. The LIS retreated to within the 2022 CE margin \~3.6 ka BP but did not completely disappear during the late Holocene. Instead, the LIS began to regrow \~2 ka BP, marking the first direct evidence of a LIS inception phase. Inception occurred under the backdrop of a modest increase in GHG forcing through the Holocene. Yet this increase in GHG forcing was unable to reverse the millennial trend in high-northern-latitude summer cooling and regional snowline lowering. Regional cooling over the past \~2 kyr was likely aided by positive feedbacks that accelerated the expansion of permanent snowfields and ice caps on Baffin Island. Contemporary ice margin retreat, driven by anthropogenic warming, has reversed \~2 kyr of LIS advance, marking the anthropogenic termination of the next glaciation.

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ACKNOWLEDGMENTS

We acknowledge the Qikiqtaani Inuit and the government of Nunavut for providing us permission to access their land through research permit no. 02-28-22R-M issued by the Nunavut Research Institute (NRI), and we thank the NRI for logistical assistance in Iqaluit. Batelle ARO provided additional logistical support. We also thank R. Schwartz and J. Hanley for $^{10}$ Be sample preparation assistance and the Lawrence Livermore Center for Accelerator Mass Spectrometry for final $^{10}$ Be measurements. We also thank the INSTAAR Laboratory for AMS Radiocarbon Preparation and Analysis for sample preparation and the Keck Carbon Cycle AMS Laboratory University of California–Irvine for radiocarbon measurements. Funding: This work was funded by National Science Foundation (NSF) Arctic Natural Sciences award nos. 1927148 and 2416598 (N.E.Y., J.M.S.) and 1927153 (G.H.M.). NSF Office of Polar Programs award nos. 1043681, 1559691, and 2129685 provided geospatial support for this work. Author contributions: Conceptualization: N.E.Y., G.H.M., J.M.S.; Methodology: N.E.Y., G.H.M., J.M.S., M.R., H.B., S.J.L., J.H.R., K.S.; Investigation: N.E.Y., G.H.M., M.R., H.B., S.J.L., J.H.R., K.S., S.L.P., J.T.A., P.J.W., J.M.S.; Visualization: N.E.Y., G.H.M., S.L.P.; Funding acquisition: N.E.Y., G.H.M., J.M.S.; Project administration: N.E.Y., G.H.M., J.M.S.; Supervision: N.E.Y., G.H.M., J.M.S.; Writing – original draft: N.E.Y., G.H.M.; Writing – review & editing: N.E.Y., G.H.M., M.R., S.J.L., J.H.R., S.L.P., J.T.A., P.J.W., J.M.S. Competing interests: The authors declare that they have no competing interests. Data, code, and materials availability: All data are available in the main text or the supplementary materials and can also be found in the NSF Arctic Data Repository (65, 66). No new materials were generated for this study. License information: Copyright © 2026 the authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original US government works. https://www.science.org/about/science-licenses-journal-article-reuse

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SUPPLEMENTARY MATERIALS

science.org/doi/10.1126/science.aed3379

Materials and Methods; Figs. S1 to S6; Tables S1 to S4; References (67–96)

Submitted 23 October 2025; accepted 29 August 2026

10.1126/science.aed3379

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We're here to help. For over 20 years, Science has conducted its annual Top Employers survey to explore what sets the best pharma and biotech companies apart. In 2026, more than 5,100 readers weighed in, highlighting three priorities: science and innovation, patient focus, and employee support.

This year, however, respondents' attitudes toward AI showed a notable shift. Comments reflected an expectation that AI will become core infrastructure rather than simply a supporting tool. As AI takes on new roles across the life science sector, applicants are mindful to articulate how their AI abilities can serve as a competitive advantage across an organization, whether it's in R&D, product development, quality control, or other departments.

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My hidden homeless past

Sage Raymond

Checking emails between flights at the airport, I was excited to see long-awaited reviews for a paper I had submitted with my Ph.D. adviser. It was an editorial in which I proposed a framework for identifying and mitigating conflict between urban coyotes and people experiencing unsheltered homelessness. Based on my thesis research, it contained more of my heart and soul than any I had previously written. But the reviews were resoundingly negative. I appreciated the valid scientific criticisms, but I struggled with comments questioning our qualifications and expertise. One in particular froze me: “The authors are naïve about homelessness.” Nothing could be further from the truth.

Following a tumultuous home life, I spent my late teenage years and early 20s in and out of homelessness, sometimes living on the street, camping illegally, and living in a car. I earned a 2-year college diploma while working full time and living in an unheated camper without water or power through Canadian winters. I finished my undergraduate degree while working as a wilderness guide, camping through the summers and retreating to a different moldy basement bedroom each winter. Some combination of stubbornness, inertia, and a genuine curiosity about the natural world kept me going. I loved time outdoors, watching animals. I wanted a job where I could ask and answer my own ecological questions.

By the time grad school was an option, it was an obvious choice—after all, I would get paid for it! I accepted a position studying the effects of urbanization on coyote behavior. Fieldwork for this project led to the editorial.

It wasn't easy to write. My sentences struggled to capture the enormity of the problems I had observed. In my fieldwork, I'd seen coyotes scavenging from encampments, eating low-quality food that would make them sick. Elsewhere, I'd collected coyote scat infected with a potentially deadly tapeworm, knowing the people in the encampments could be exposed but would struggle to access health care. These observations mingled with memories I wish I didn't have. The unique smell of dumpster diving in a sleeping city. Laughing and braiding the hair of a friend who later died violently in the streets. I pushed those memories away to write as cleanly and objectively as possible.

Homelessness took things from me, but it also gave me things. I am observant. I am resourceful. I am phenomenal at camping. I thrive in bad weather. These skills have helped me walk so many worthwhile roads—as a professional wilderness guide, a recreationist comfortable solo camping in wild places, and, crucially, as an urban ecologist. I am comfortable conducting fieldwork in urban spaces where others might not be. It's exactly this aptitude that let me notice the things I had described in my paper, which was eventually published at another journal.

I can't know exactly what the reviewer who accused us of naivety was thinking, but they seemingly never imagined an author of such a piece might have firsthand experience of homelessness. That assumption shook me: It suggested someone with my history did not belong in academia. It was not the first time I have felt that way. I recalled the way fellow grad students had expressed fear of a man sleeping in the entrance to a university building, and an urban ecology safety briefing that focused on the dangers of homeless people rather than on ways to communicate with or support people in need.

Many of the life experiences that bring diversity to science are invisible, or are sufficiently personal and taboo that we don't talk about them—abuse, poverty, rape, addiction, a schizophrenic family member, a history of homelessness. Our assumptions about who researchers are and what their past lives looked like create an isolating landscape of erasure—an environment where certain histories are assumed to be absent, keeping the people who hold those histories from feeling they belong.

For years, I worked hard to hide my history of homelessness. Now, I am more neutral—it was a challenging and sometimes unpleasant chapter, like puberty, or, more recently, learning Bayesian statistics. I am committed to not letting my history define me. But I also don't want my colleagues to assume no scientist could have a past like mine. □

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书评等

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📰 报刊故事还原:乔恩·科恩(JON COHEN),发自圣迭戈佩特科公园球场

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该报道刊发于《a950fa_Science___22_October_2026_ebooksyard》要闻版面,折射出当地社会在日常生活与观念层面的真实关注点。
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诗歌阐明证据为何重要

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💡 驻外文化与社会背景解码:
该报道刊发于《a950fa_Science___22_October_2026_ebooksyard》要闻版面,折射出当地社会在日常生活与观念层面的真实关注点。
🏛️ 二、本期所在国制度、机构与历史百科 (Local Encyclopedia)
本期专有背景词条已内嵌于正文注释中。
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乔恩·科恩(JON COHEN),发自圣迭戈佩特科公园球场

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诗歌阐明证据为何重要

诗歌与科学之间的关系通常被界定为一种沟通关系:诗歌和其他艺术形式可以帮助向更广泛的受众解释科学。虽然这确实没错,但这低估了两者在对话中各自能带来的独特贡献。

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为自然保护培养连接感

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保护决策很少仅基于生态信息。它们还受到历史、文化、身份、记忆和生活经验的影响。这些形式的知识很难在地图、模型或期刊文章中捕捉,但它们能强烈影响保护工作的成败。艺术实践——包括讲故事、诗歌、摄影、表演和其他创意方法——提供了让生活经验、文化记

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下一个前沿

尽管人们对艺术与科学协作的兴趣日益浓厚,但关于其长期保护效果的严谨证据仍然有限。近期的大量文献由概念框架、综合论文、项目描述以及对新兴实践的反思组成,而非对保护结果的评估 [例如,(14)]。尽管如此,这项工作为艺术家确定了极具前景的新角色

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牙买加公共债务与 GDP 的轨迹

历史路径显示,债务从 2013 年的 $\sim 144\%$ 下降到 2024 年底的 $\sim 65\%$。在“梅丽莎”飓风之后,债务率预计将达到峰值 $68.5\%$ ,比没有风暴的假设情况($\sim 60\%$)增加了 8.5

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冰缘年代学

BIC 前缘存在一条明显的修整线(trimline),标志着约 1960 CE 的历史最大 BIC 边缘 [见补充材料 (SM)]。1960 CE 的修整线以色调的剧烈变化为标志:修整线之外是长有地衣和植被的基岩地形,而修整线与现代冰缘之间

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