Park Sang-Won, Kim Soree, Jung YounJoon
Department of Chemistry, Seoul National University, Seoul 08826, Korea.
Phys Chem Chem Phys. 2015 Nov 21;17(43):29281-92. doi: 10.1039/c5cp03390j.
We study how dynamic heterogeneity in ionic liquids is affected by the length scale of structural relaxation and the ionic charge distribution by the molecular dynamics simulations performed on two differently charged models of ionic liquid and their uncharged counterpart. In one model of ionic liquid, the charge distribution in the cation is asymmetric, and in the other it is symmetric, while their neutral counterpart has no charge with the ions. It is found that all the models display heterogeneous dynamics, exhibiting subdiffusive dynamics and a nonexponential decay of structural relaxation. We investigate the lifetime of dynamic heterogeneity, τ(dh), in these systems by calculating the three-time correlation functions to find that τ(dh) has in general a power-law behavior with respect to the structural relaxation time, τ(α), i.e., τ(dh) ∝ τ(α)(ζ(dh)). Although the dynamics of the asymmetric-charge model is seemingly more heterogeneous than that of the symmetric-charge model, the exponent is found to be similar, ζ(dh) ≈ 1.2, for all the models studied in this work. The same scaling relation is found regardless of interactions, i.e., with or without Coulomb interaction, and it holds even when the length scale of structural relaxation is long enough to become the Fickian diffusion. This fact indicates that τ(dh) is a distinctive time scale from τ(α), and the dynamic heterogeneity is mainly affected by the short-range interaction and the molecular structure.
我们通过对两种不同电荷模型的离子液体及其不带电对应物进行分子动力学模拟,研究了离子液体中的动态非均匀性如何受到结构弛豫长度尺度和离子电荷分布的影响。在一种离子液体模型中,阳离子中的电荷分布不对称,而在另一种模型中则是对称的,而它们的中性对应物中离子不带电。结果发现,所有模型都表现出非均匀动力学,呈现亚扩散动力学和结构弛豫的非指数衰减。我们通过计算三次关联函数来研究这些系统中动态非均匀性的寿命τ(dh),发现τ(dh)通常相对于结构弛豫时间τ(α)具有幂律行为,即τ(dh) ∝ τ(α)(ζ(dh))。尽管不对称电荷模型的动力学似乎比对称电荷模型的动力学更不均匀,但发现对于本工作中研究的所有模型,指数相似,ζ(dh) ≈ 1.2。无论有无相互作用,即有无库仑相互作用,都发现了相同的标度关系,并且即使结构弛豫的长度尺度足够长以至于变成菲克扩散,该关系仍然成立。这一事实表明,τ(dh)是与τ(α)不同的独特时间尺度,动态非均匀性主要受短程相互作用和分子结构的影响。