Separdar L, Davatolhagh S
Department of Physics, College of Sciences, Shiraz University, Shiraz 71454, Iran.
Phys Rev E Stat Nonlin Soft Matter Phys. 2013 Feb;87(2):022305. doi: 10.1103/PhysRevE.87.022305. Epub 2013 Feb 19.
We investigate the static structure and diffusive dynamics of binary Lennard-Jones mixture upon supercooling in the presence of gold nanoparticle within the framework of the mode-coupling theory of the dynamic glass transition in the direct space by means of constant-NVT molecular dynamics simulations. It is found that the presence of gold nanoparticle causes the energy per particle and the pressure of this system to decrease with respect to the bulk binary Lennard-Jones mixture. Furthermore, the presence of nanoparticle has a direct effect on the liquid structure and causes the peaks of the radial distribution functions to become shorter with respect to the bulk binary Lennard-Jones liquid. The dynamics of the liquid at a given density is found to be consistent with the mode-coupling theory (MCT) predictions in a certain range at low temperatures. In accordance with the idealized MCT, the diffusion constants D(T) show a power-law behavior at low temperatures for both types of binary Lennard-Jones (BLJ) particles as well as the gold atoms comprising the nanoparticle. The mode-coupling crossover temperature T(c) is the same for all particle types; however, T(c)=0.4 is reduced with respect to that of the bulk BLJ liquid, and the γ exponent is found to depend on the particle type. The existence of the nanoparticle causes the short-time β-relaxation regime to shorten and the range of validity of the MCT shrinks with respect to the bulk BLJ. It is also found that at intermediate and low temperatures the curves of the mean-squared displacements (MSDs) versus tD(T) fall onto a master curve. The MSDs follow the master curve in an identical time range with the long-time α-relaxation regime of the mode-coupling theory. By obtaining the viscosity, it is observed that the Stokes-Einstein relation remains valid at high and intermediate temperatures but breaks down as the temperatures approach T(c) as a result of the cooperative motion or activated processes.
我们在直接空间中动态玻璃化转变的模式耦合理论框架下,通过恒压恒温分子动力学模拟,研究了在金纳米颗粒存在下二元 Lennard-Jones 混合物过冷时的静态结构和扩散动力学。研究发现,金纳米颗粒的存在导致该系统的每个粒子能量和压力相对于本体二元 Lennard-Jones 混合物降低。此外,纳米颗粒的存在对液体结构有直接影响,使径向分布函数的峰值相对于本体二元 Lennard-Jones 液体变得更短。发现在给定密度下液体的动力学在低温的一定范围内与模式耦合理论(MCT)预测一致。根据理想化的 MCT,对于两种类型的二元 Lennard-Jones(BLJ)粒子以及构成纳米颗粒的金原子,扩散常数 D(T) 在低温下均呈现幂律行为。所有粒子类型的模式耦合交叉温度 T(c) 相同;然而,相对于本体 BLJ 液体,T(c)=0.4 降低了,并且发现 γ 指数取决于粒子类型。纳米颗粒的存在导致短时间 β 弛豫区缩短,并且相对于本体 BLJ,MCT 的有效范围缩小。还发现,在中低温下,均方位移(MSD)与 tD(T) 的曲线落在一条主曲线上。MSD 在与模式耦合理论的长时间 α 弛豫区相同的时间范围内遵循主曲线。通过获得粘度,观察到斯托克斯-爱因斯坦关系在高温和中温下仍然有效,但随着温度接近 T(c) 由于协同运动或活化过程而失效。