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过冷液体中的急动促进与玻璃态动力学。

Emergent facilitation and glassy dynamics in supercooled liquids.

作者信息

Hasyim Muhammad R, Mandadapu Kranthi K

机构信息

Department of Chemical and Biomolecular Engineering, University of California, Berkeley, CA 94720.

Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720.

出版信息

Proc Natl Acad Sci U S A. 2024 Jun 4;121(23):e2322592121. doi: 10.1073/pnas.2322592121. Epub 2024 May 28.

Abstract

In supercooled liquids, dynamical facilitation refers to a phenomenon where microscopic motion begets further motion nearby, resulting in spatially heterogeneous dynamics. This is central to the glassy relaxation dynamics of such liquids, which show super-Arrhenius growth of relaxation timescales with decreasing temperature. Despite the importance of dynamical facilitation, there is no theoretical understanding of how facilitation emerges and impacts relaxation dynamics. Here, we present a theory that explains the microscopic origins of dynamical facilitation. We show that dynamics proceeds by localized bond-exchange events, also known as excitations, resulting in the accumulation of elastic stresses with which new excitations can interact. At low temperatures, these elastic interactions dominate and facilitate the creation of new excitations near prior excitations. Using the theory of linear elasticity and Markov processes, we simulate a model, which reproduces multiple aspects of glassy dynamics observed in experiments and molecular simulations, including the stretched exponential decay of relaxation functions, the super-Arrhenius behavior of relaxation timescales as well as their two-dimensional finite-size effects. The model also predicts the subdiffusive behavior of the mean squared displacement (MSD) on short, intermediate timescales. Furthermore, we derive the phonon contributions to diffusion and relaxation, which when combined with the excitation contributions produce the two-step relaxation processes, and the ballistic-subdiffusive-diffusive crossover MSD behaviors commonly found in supercooled liquids.

摘要

在过冷液体中,动力学促进是指微观运动引发附近进一步运动,从而导致空间非均匀动力学的一种现象。这是此类液体玻璃态弛豫动力学的核心,这种动力学表现出弛豫时间尺度随温度降低呈超阿伦尼乌斯增长。尽管动力学促进很重要,但对于促进如何出现以及如何影响弛豫动力学尚无理论理解。在此,我们提出一种理论来解释动力学促进的微观起源。我们表明动力学通过局部键交换事件(也称为激发)进行,导致弹性应力的积累,新的激发可以与这些弹性应力相互作用。在低温下,这些弹性相互作用占主导并促进在先前激发附近产生新的激发。利用线性弹性理论和马尔可夫过程,我们模拟了一个一个模型,该模型再现了实验和分子模拟中观察到的玻璃态动力学的多个方面,包括弛豫函数的拉伸指数衰减、弛豫时间尺度的超阿伦尼乌斯行为以及它们的二维有限尺寸效应。该模型还预测了短、中时间尺度上平均平方位移(MSD)的亚扩散行为。此外,我们推导了声子对扩散和弛豫的贡献,当与激发贡献相结合时会产生两步弛豫过程,以及过冷液体中常见的弹道 - 亚扩散 - 扩散交叉MSD行为。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/eb3d/11161792/189a01c16f56/pnas.2322592121fig01.jpg

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