Flenner Elijah, Zhang Min, Szamel Grzegorz
Department of Chemistry, Colorado State University, Fort Collins, Colorado 80523, USA.
Phys Rev E Stat Nonlin Soft Matter Phys. 2011 May;83(5 Pt 1):051501. doi: 10.1103/PhysRevE.83.051501. Epub 2011 May 2.
We examine a length scale that characterizes the spatial extent of heterogeneous dynamics in a glass-forming binary hard-sphere mixture up to the mode-coupling volume fraction ϕ(c). First, we characterize the system's dynamics. Then, we utilize a method [Phys. Rev. Lett. 105, 217801 (2010)] to extract and analyze the ensemble-independent dynamic susceptibility χ(4)(t) and the dynamic correlation length ξ(t) for a range of times between the β and α relaxation times. We find that in this time range the dynamic correlation length follows a volume fraction-independent master curve ξ(t)ln(t). For longer times, ξ(t) departs from this master curve and remains constant up to the largest time at which we can determine the length accurately. In addition to the previously established correlation τ(α)exp[ξ(τ(α))] between the α relaxation time, τ(α), and the dynamic correlation length at this time, ξ(τ(α)), we also find a similar correlation for the diffusion coefficient D~exp[ξ(τ(α))(θ)] with θ≈0.6. We discuss the relevance of these findings for different theories of the glass transition.
我们研究了一个长度尺度,它表征了玻璃形成二元硬球混合物中异质动力学的空间范围,直至模式耦合体积分数ϕ(c)。首先,我们表征了系统的动力学。然后,我们利用一种方法[《物理评论快报》105, 217801 (2010)],在β和α弛豫时间之间的一系列时间内,提取并分析与系综无关的动态磁化率χ(4)(t)和动态关联长度ξ(t)。我们发现,在这个时间范围内,动态关联长度遵循一条与体积分数无关的主曲线ξ(t)ln(t)。对于更长的时间,ξ(t)偏离这条主曲线,并在我们能够准确确定长度的最长时间之前保持恒定。除了先前建立的α弛豫时间τ(α)与此时的动态关联长度ξ(τ(α))之间的关联τ(α)exp[ξ(τ(α))]之外,我们还发现扩散系数D~exp[ξ(τ(α))(θ)]存在类似的关联,其中θ≈0.6。我们讨论了这些发现与不同玻璃转变理论的相关性。