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Two-step relaxation and the breakdown of the Stokes-Einstein relation in glass-forming liquids

机译:两步放松和斯托克斯 - 爱因斯坦在玻璃形成液体中的崩溃

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摘要

It is well known that glass-forming liquids exhibit a number of anomalous dynamical phenomena, most notably a two-step relaxation in the self-intermediate scattering function and the breakdown of the Stokes- Einstein (SE) relation, as they are cooled toward the glass transition temperature. While these phenomena are generally ascribed to dynamic heterogeneity, specifically to the presence of slow- and fast-moving particles, a quantitative elucidation of the two-step relaxation and the violation of the SE relation in terms of these concepts has not been successful. In this work, we propose a classification of particles according to the rank order of their displacements (from an arbitrarily defined origin of time), and we divide the particles into long-distance (LD), medium-distance, and short-distance (SD) traveling particle groups. Using molecular-dynamics simulation data of the Kob-Andersen model, we show quantitatively that the LD group is responsible for the fast relaxation in the two-step relaxation process in the intermediate scattering function, while the SD group gives rise to the slow (α) relaxation. Furthermore, our analysis reveals that τ_α is controlled by the SD group, while the ensemble-averaged diffusion coefficient D is controlled by both the LD and SD groups. The combination of these two features provides a natural explanation for the breakdown in the SE relation at low temperature. In addition, we find that the α-relaxation time, τ_α, of the overall system is related to the relaxation time of the LD particles, τ_(LD), as τ_α = τ_0 exp(?τ_(LD)/k_BT ).
机译:众所周知,玻璃形成液体表现出许多异常动态现象,最特别是在自我中间散射功能和斯托克斯 - 爱因斯坦(SE)关系中的两步松弛,因为它们被冷却玻璃化转变温度。虽然这些现象通常归因于动态异质性,但特别是在存在缓慢和快速移动的颗粒的情况下,两步松弛的定量阐明和违反这些概念的侵犯了SE关系并未成功。在这项工作中,我们提出了根据其位移的等级顺序(从任意定义的时间起源)的颗粒分类,并且我们将粒子划分为长距离(LD),中距离和短距离( SD)行驶粒子组。使用Kob-Andersen模型的分子动力学模拟数据,我们定量地显示了LD组在中间散射功能中的两步松弛过程中的快速松弛,而SD组引起慢(α ) 松弛。此外,我们的分析揭示了τ_α由SD组控制,而集合平均扩散系数D由LD和SD组控制。这两个特征的组合为在低温下的SE关系中的击穿提供了自然的解释。此外,我们发现整个系统的α-松弛时间τ_α与LD粒子,τ_(ld)的松弛时间有关,如τ_α=τ_0exp(?τ_(ld)/ k_bt)。

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