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受限单原子流体中的玻璃态动力学。

Glassy dynamics in a confined monatomic fluid.

作者信息

Krishnan S H, Ayappa K G

机构信息

Department of Chemical Engineering, Indian Institute of Science, Bangalore 560012, India.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2012 Jul;86(1 Pt 1):011504. doi: 10.1103/PhysRevE.86.011504. Epub 2012 Jul 23.

Abstract

Molecular dynamic simulations of a strongly inhomogeneous system reveals that a single-component soft-sphere fluid can behave as a fragile glass former due to confinement. The self-intermediate scattering function, F(s)(k,t), of a Lennard-Jones fluid confined in slit-shaped pores, which can accommodate two to four fluid layers, exhibits a two-step relaxation at moderate temperatures. The mean-squared displacement data are found to follow time-temperature superposition and both the self-diffusivity and late α relaxation times exhibit power-law divergences as the fluid is cooled. The system possesses a crossover temperature and follows the scalings of mode coupling theory for the glass transition. The temperature dependence of the self-diffusivity can be expressed using the Vogel-Fulcher-Tammann equation, and estimates of the fragility index of the system indicates a fragile glass former. At lower temperatures, signatures of additional relaxation processes are observed in the various dynamical quantities with a three-step relaxation observed in the F(s)(k,t).

摘要

对强非均匀系统的分子动力学模拟表明,由于受限,单组分软球流体可表现为一种易碎的玻璃形成体。限制在狭缝形孔中的 Lennard-Jones 流体的自中间散射函数 F(s)(k,t),该孔可容纳两到四个流体层,在中等温度下呈现两步弛豫。发现均方位移数据遵循时间-温度叠加,并且随着流体冷却,自扩散系数和晚期 α 弛豫时间均呈现幂律发散。该系统具有一个交叉温度,并遵循玻璃化转变的模式耦合理论标度。自扩散系数的温度依赖性可以用 Vogel-Fulcher-Tammann 方程表示,系统脆性指数的估计表明它是一种易碎的玻璃形成体。在较低温度下,在各种动力学量中观察到额外弛豫过程的特征,在 F(s)(k,t) 中观察到三步弛豫。

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