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A crowd of marine embryos self-assembles into a living solid 一群海洋胚胎自我组装成一个有生命的固体
IF 19.6 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY Pub Date : 2026-02-23 DOI: 10.1038/s41567-026-03190-x
Vivek N. Prakash
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引用次数: 0
Suppression and enhancement of bosonic stimulation by atomic interactions 原子相互作用对玻色子刺激的抑制和增强
IF 19.6 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY Pub Date : 2026-02-20 DOI: 10.1038/s41567-025-03155-6
Konstantinos Konstantinou, Yansheng Zhang, Paul H. C. Wong, Feiyang Wang, Yu-Kun Lu, Nishant Dogra, Christoph Eigen, Tanish Satoor, Wolfgang Ketterle, Zoran Hadzibabic
The tendency of identical bosons to bunch, seen in the Hanbury Brown–Twiss effect and Bose–Einstein condensation, is a hallmark of quantum statistics. This bunching can enhance the rates of fundamental processes such as atom–atom and atom–light scattering when atoms scatter into already occupied states. For non-interacting bosons, the enhancement of light scattering follows directly from the occupation of the atom’s final momentum state. Here we study scattering between off-resonant light and atoms in a quasi-homogeneous Bose gas with tunable interactions and show that even weak interactions, which essentially do not alter the momentum distribution, strongly affect atom–light scattering. Changes in local atomic correlations suppress the bosonic enhancement under weak repulsive interactions and increase the scattering rate under attractive ones. Moreover, if the interactions are rapidly tuned, light scattering reveals correlation dynamics that are orders of magnitude faster than the collisional dynamics of the momentum-space populations. Its extreme sensitivity to correlation effects makes off-resonant light scattering a powerful probe of many-body physics in ultracold atomic gases.
在汉伯里布朗-特维斯效应和玻色子-爱因斯坦凝聚中看到的相同玻色子聚束的趋势是量子统计学的一个标志。当原子散射到已经占据的状态时,这种聚束可以提高原子-原子和原子-光散射等基本过程的速率。对于非相互作用玻色子,光散射的增强直接来自于原子最终动量态的占据。本文研究了具有可调谐相互作用的准均匀玻色气体中非共振光与原子之间的散射,并表明即使是弱相互作用(基本上不改变动量分布)也会强烈影响原子光散射。局域原子相关的变化抑制了弱排斥作用下玻色子的增强,而增加了吸引作用下的散射速率。此外,如果快速调整相互作用,光散射揭示的相关动力学比动量-空间居群的碰撞动力学快几个数量级。非共振光散射对相关效应的极端敏感性使其成为研究超冷原子气体中多体物理的有力探针。
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引用次数: 0
Fatigue failure in glasses under cyclic shear deformation 循环剪切变形作用下玻璃的疲劳破坏
IF 19.6 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY Pub Date : 2026-02-20 DOI: 10.1038/s41567-026-03174-x
Swarnendu Maity, Himangsu Bhaumik, Shivakumar Athani, Srikanth Sastry
Solids subjected to repeated cycles of stress or deformation can fail after several cycles, a phenomenon termed fatigue failure. Although intensely investigated for a wide range of materials owing to its obvious practical importance, a microscopic understanding of the initiation of fatigue failure continues to be actively pursued, in particular for soft and amorphous materials. Employing computer simulations, here we show that upon approaching the so-called fatigue limit, the failure times of glasses subjected to cyclic shear deformation display a power-law divergence, which is at variance with commonly used functional forms, and exhibit a strong dependence on the degree of annealing of the glasses. Our simulations explore measures of damage based on a quantification of plastic rearrangements and on energy dissipated. The fraction of particles that undergo plastic rearrangements and the percolation transition they undergo are both predictive of failure. We also find a robust power law between the accumulated damage, which is quantified by the energy dissipated or the non-affine displacements, and the failure times, which permits prediction of failure times based on the behaviour in the initial cycles. These observations reveal salient new microscopic features of fatigue failure and indicate approaches for developing a full microscopic picture of fatigue failure in amorphous solids.
固体受到反复的应力或变形循环后,会在几个循环后失效,这种现象称为疲劳失效。尽管由于其明显的实际重要性,对广泛的材料进行了深入的研究,但对疲劳失效起始的微观理解仍在积极追求,特别是对软质和非晶材料。利用计算机模拟,我们在这里表明,在接近所谓的疲劳极限时,玻璃遭受循环剪切变形的破坏时间显示幂律发散,这与常用的函数形式不同,并且表现出强烈的依赖于玻璃的退火程度。我们的模拟探索了基于量化塑性重排和能量耗散的损伤措施。经历塑性重排的颗粒比例和它们经历的渗透转变都预示着失败。我们还发现累积损伤(由耗散的能量或非仿射位移量化)与失效时间之间存在鲁棒幂律,这允许基于初始循环中的行为预测失效时间。这些观察结果揭示了疲劳失效的新的显著微观特征,并指出了发展非晶固体疲劳失效的完整微观图像的方法。
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引用次数: 0
How light scattering loses its boost 光散射是如何失去动力的
IF 19.6 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY Pub Date : 2026-02-20 DOI: 10.1038/s41567-025-03156-5
Giovanni Ferioli
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引用次数: 0
Statistical localization of U(1) lattice gauge theory in a Rydberg simulator Rydberg模拟器中U(1)晶格规范理论的统计局部化
IF 19.6 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY Pub Date : 2026-02-18 DOI: 10.1038/s41567-026-03183-w
Prithvi Raj Datla, Luheng Zhao, Wen Wei Ho, Natalie Klco, Huanqian Loh
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引用次数: 0
An exciton crystal in a moiré excitonic insulator 振动激子绝缘体中的激子晶体
IF 19.6 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY Pub Date : 2026-02-18 DOI: 10.1038/s41567-026-03184-9
Ruishi Qi, Qize Li, Haleem Kim, Jiahui Nie, Zuocheng Zhang, Ruichen Xia, Zhiyuan Cui, Jianghan Xiao, Takashi Taniguchi, Kenji Watanabe, Michael F. Crommie, Feng Wang
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引用次数: 0
Discontinuous transition to shear flow turbulence 不连续过渡到剪切流湍流
IF 19.6 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY Pub Date : 2026-02-17 DOI: 10.1038/s41567-025-03166-3
Bowen Yang, Yi Zhuang, Gökhan Yalnız, Vasudevan Mukund, Elena Marensi, Björn Hof
Depending on the type of flow, the transition to turbulence can take one of two forms: either turbulence arises from a sequence of instabilities or from the spatial proliferation of transiently chaotic domains, a process analogous to directed percolation. The former scenario is commonly referred to as a supercritical transition and frequently encountered in flows destabilized by body forces, whereas the latter subcritical transition is common in shear flows. Both cases are inherently continuous in a sense that the transformation from ordered laminar to fully turbulent fluid motion is only accomplished gradually with flow speed. Here we show that these established transition types do not account for the more general setting of shear flows subject to body forces. The combination of the two continuous scenarios leads to the attenuation of spatial coupling; with increasing forcing amplitude, the transition becomes increasingly sharp and eventually discontinuous. We argue that the suppression of laminar–turbulent coexistence and the approach towards a discontinuous phase transition potentially apply to a broad range of situations including flows subject to, for example, buoyancy, centrifugal or electromagnetic forces.
根据流动类型的不同,向湍流的过渡可以采取以下两种形式之一:湍流要么是由一系列不稳定性引起的,要么是由瞬态混沌域的空间扩散引起的,这一过程类似于定向渗透。前一种情况通常被称为超临界转变,经常在由体力破坏稳定的流动中遇到,而后者的亚临界转变在剪切流动中很常见。从某种意义上说,这两种情况都是内在连续的,即从有序层流到完全湍流的流体运动的转变只能随着流速逐渐完成。在这里,我们表明,这些建立的过渡类型不考虑更一般的设置剪切流受身体的力量。两种连续情景的结合导致了空间耦合的衰减;随着强迫幅值的增大,转变逐渐剧烈并最终不连续。我们认为,抑制层流-湍流共存和朝向不连续相变的方法可能适用于广泛的情况,包括受浮力、离心力或电磁力影响的流动。
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引用次数: 0
Topological Kondo insulator in MoTe2/WSe2 moiré bilayers MoTe2/WSe2膜层的拓扑近藤绝缘子
IF 19.6 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY Pub Date : 2026-02-16 DOI: 10.1038/s41567-026-03170-1
Zhongdong Han, Yiyu Xia, Zhengchao Xia, Wenjin Zhao, Yichi Zhang, Kenji Watanabe, Takashi Taniguchi, Jie Shan, Kin Fai Mak
Topological Kondo insulators are a topologically protected insulating state induced by Kondo exchange interactions between itinerant electrons and local magnetic moments, as opposed to single-particle band inversion. They are characterized by an insulating bulk with Dirac surface states in three dimensions and helical edge states in two dimensions. Although experiments have supported the emergence of these insulators in the rare-earth compound SmB 6 , their observation in two-dimensional systems has not been demonstrated. Here we report the experimental evidence of a two-dimensional topological Kondo insulator in MoTe 2 /WSe 2 moiré bilayers. Using dual-gated devices, we prepare a triangular lattice of local moments in the MoTe 2 layer and a half-filled dispersive band in the WSe 2 layer with a chiral Kondo coupling. Using transport and compressibility measurements, we show that the state supports metallic transport at high temperature and an insulating bulk with helical edge conduction protected by spin- S z conservation at low temperature. Under high magnetic fields, the insulating state at low temperature becomes metallic. Our results demonstrate a highly tunable platform based on moiré materials for studying the interplay of strong interactions and topological order.
拓扑近藤绝缘体是一种受拓扑保护的绝缘状态,由流动电子和局部磁矩之间的近藤交换相互作用引起,而不是单粒子带反转。它们的特点是具有三维狄拉克表面态和二维螺旋边缘态的绝缘体。虽然实验支持这些绝缘体在稀土化合物smb6中的出现,但它们在二维系统中的观察尚未得到证实。在这里,我们报告了在MoTe 2 /WSe 2 moir双层中二维拓扑近藤绝缘子的实验证据。利用双门控器件,我们在MoTe 2层中制备了局部矩的三角形晶格,并在WSe 2层中制备了具有手性近藤耦合的半填充色散带。通过输运和可压缩性测量,我们证明了该态在高温下支持金属输运,在低温下支持具有螺旋边传导的绝缘体,并受到自旋- S - z守恒的保护。在强磁场作用下,低温下的绝缘状态变为金属态。我们的研究结果展示了一个基于莫尔材料的高度可调平台,用于研究强相互作用和拓扑顺序的相互作用。
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引用次数: 0
The paper trail of nuclear strategy 核战略的书面记录
IF 18.4 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY Pub Date : 2026-02-13 DOI: 10.1038/s41567-025-03153-8
Paul Erickson
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引用次数: 0
Many-foot dynamics Many-foot动力学
IF 18.4 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY Pub Date : 2026-02-13 DOI: 10.1038/s41567-026-03195-6
Bart Verberck
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引用次数: 0
期刊
Nature Physics
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