Habasaki Junko, Ngai K L
Department of Innovative and Engineered Materials, Interdisciplinary Graduate School of Science and Engineering, Tokyo Institute of Technology, Nagatsuta 4259, Yokohama 226-8502, Japan.
CNR-IPCF Dipartimento di Fisica, Università di Pisa, Largo Bruno Pontecorvo 3, I-56127 Pisa, Italy.
J Chem Phys. 2015 Apr 28;142(16):164501. doi: 10.1063/1.4918586.
The typical ionic liquid, 1-ethyl-3-methyl imidazolium nitrate (EMIM-NO3), was examined by molecular dynamics simulations of an all-atomistic model to show the characteristics of networks of cages and/or bonds in the course of vitrification of this fragile glass-former. The system shows changes of dynamics at two characteristic temperatures, TB (or Tc) and the glass transition temperature Tg, found in other fragile glass forming liquids [K. L. Ngai and J. Habasaki, J. Chem. Phys. 141, 114502 (2014)]. On decreasing temperature, the number of neighboring cation-anion pairs, NB, within the first minimum of the pair correlation function, g(r)min, increases. On crossing TB (>Tg), the system volume and diffusion coefficient both show changes in temperature dependence, and as usual at Tg. The glass transition temperature, Tg, is characterized by the saturation of the total number of "bonds," NB and the corresponding decrease in degree of freedom, F = [(3N - 6) - NB], of the system consisting of N particles. Similar behavior holds for the other ion-ion pairs. Therefore, as an alternative, the dynamics of glass transition can be interpreted conceptually by rigidity percolation. Before saturation occurring at Tg, the number of bonds shows a remarkable change at around TB. This temperature is associated with the disappearance of the loosely packed coordination polyhedra of anions around cation (or vice versa), related to the loss of geometrical freedom of the polyhedra, fg, of each coordination polyhedron, which can be defined by fg = [(3NV - 6) - Nb]. Here, 3Nv is the degree of freedom of NV vertices of the polyhedron, and Nb is number of fictive bonds. The packing of polyhedra is characterized by the soft percolation of cages, which allows further changes with decreasing temperature. The power spectrum of displacement of the central ion in the cage is found to be correlated with the fluctuation of Nb of cation-cation (or anion-anion) pairs in the polyhedron, although the effect from the coordination shells beyond the neighboring ions is not negligible.
通过全原子模型的分子动力学模拟研究了典型离子液体1-乙基-3-甲基咪唑鎓硝酸盐(EMIM-NO₃),以展现这种易碎玻璃形成体在玻璃化过程中笼状结构和/或键网络的特征。该体系在两个特征温度,即TB(或Tc)和玻璃化转变温度Tg处表现出动力学变化,这在其他易碎玻璃形成液体中也有发现[K. L. 恩盖和J. 羽崎,《化学物理杂志》141, 114502 (2014)]。随着温度降低,对关联函数g(r)min的第一个极小值内相邻阳离子-阴离子对的数量NB增加。在越过TB(>Tg)时,体系体积和扩散系数在温度依赖性上均出现变化,且在Tg处也如往常一样。玻璃化转变温度Tg的特征在于“键”总数NB的饱和以及由N个粒子组成的体系自由度F = [(3N - 6) - NB]的相应降低。其他离子-离子对也有类似行为。因此,作为一种替代方法,玻璃化转变的动力学可以从概念上用刚性逾渗来解释。在Tg处饱和发生之前,键的数量在TB附近有显著变化。这个温度与阳离子周围阴离子松散堆积的配位多面体的消失有关(反之亦然),这与每个配位多面体的几何自由度fg的丧失有关,fg可以定义为fg = [(3NV - 6) - Nb]。这里,3Nv是多面体NV个顶点的自由度,Nb是虚拟键的数量。多面体的堆积以笼状结构的软逾渗为特征,这使得随着温度降低会有进一步变化。尽管来自相邻离子之外的配位层的影响不可忽略,但发现笼中中心离子位移的功率谱与多面体中阳离子-阳离子(或阴离子-阴离子)对的Nb波动相关。