论文标题

结构放松,软球液体中的动态逮捕和老化

Structural relaxation, dynamical arrest and aging in soft-sphere liquids

论文作者

Mendoza-Méndez, Patricia, Peredo-Ortiz, Ricardo, Lázaro, Edilio Lázaro, Chávez-Paez, M., Pacheco-Vázquez, F., Medina-Noyola, M., Elizondo-Aguilera, L. F.

论文摘要

我们在玻璃过渡上方和下方研究了不同温度$ t_f $ $ t_f $的软球液体淬火($ ϕ = 0.7 $)的结构放松。为此,我们将广泛的布朗动力学模拟和理论计算结合在一起,基于非平衡自洽的广义Langevin方程(NE-SCGLE)理论。液体对淬火的反应通常包括随着系统年龄的增长$α$ - 递延时间的亚线性增加。从上方($ t_f> t^a $)接近理想的玻璃过渡温度时,作为瞬态过程,描述了淬火到几乎被捕的状态的广泛平衡交叉。这使我们能够经验确定一个平衡时间尺度$ t^{eq}(t_f)$,随着$ t_f $接近$ t^a $,它变得越来越长。 For quenches inside the glass ($T_f\leq T^a$) the growth rate of the structural relaxation time becomes progressively larger as $T_f$ decreases and, unlike the equilibration scenario, $τ_α$ remains evolving within the whole observation time-window.These features are consistently found in theory and simulations with remarkable semi-quantitative agreement, and coincide with those revealed in the similar and complementary exercise [物理。修订版{\ bf 96},022608(2017)],它考虑了一系列具有固定最终温度的淬灭序列$ t_f = 0 $,但增加了$ ϕ $,以使硬球动态逮捕量$ ϕ^a__ {hs} = 0.582 $。但是,NE-SCGLE分析揭示了玻璃转变的各个基本方面,涉及从普通平衡场景到持续的衰老效应的突然传递,这些效果是玻璃形成液体的特征。该理论还解释说,在任何实验观察的时间窗口中,只能将其视为连续的交叉。

We investigate the structural relaxation of a soft-sphere liquid quenched isochorically ($ϕ=0.7$) and instantaneously to different temperatures $T_f$ above and below the glass transition. For this, we combine extensive Brownian dynamics simulations and theoretical calculations based on the non-equilibrium self-consistent generalized Langevin equation (NE-SCGLE) theory. The response of the liquid to a quench generally consists of a sub-linear increase of the $α$-relaxation time with system's age. Approaching the ideal glass-transition temperature from above ($T_f>T^a$) sub-aging appears as a transient process describing a broad equilibration crossover for quenches to nearly arrested states. This allows us to empirically determine an equilibration timescale $t^{eq}(T_f)$ that becomes increasingly longer as $T_f$ approaches $T^a$. For quenches inside the glass ($T_f\leq T^a$) the growth rate of the structural relaxation time becomes progressively larger as $T_f$ decreases and, unlike the equilibration scenario, $τ_α$ remains evolving within the whole observation time-window.These features are consistently found in theory and simulations with remarkable semi-quantitative agreement, and coincide with those revealed in the similar and complementary exercise [Phys. Rev. {\bf 96}, 022608 (2017)] that considered a sequence of quenches with fixed final temperature $T_f=0$ but increasing $ϕ$ towards the hard-sphere dynamical arrest volume fraction $ϕ^a_{HS}=0.582$. The NE-SCGLE analysis, however, unveils various fundamental aspects of the glass transition, involving the abrupt passage from the ordinary equilibration scenario to the persistent aging effects that are characteristic of glass-forming liquids. The theory also explains that, within the time window of any experimental observation, this can only be observed as a continuous crossover.

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