Institut de Chimie de Clermont-Ferrand, UMR 6296, CNRS∕Université Blaise Pascal, 63177 Aubière, France.
J Chem Phys. 2013 Aug 7;139(5):054510. doi: 10.1063/1.4817403.
Raman spectra in the range of the totally symmetric stretching mode of the PF6 anion, νs(PF6), have been measured for 1-alkyl-3-methylimidazolium ionic liquids [CnC1im][PF6], for n = 4, 6, and 8, as a function of pressure at room temperature. The ionic liquids [C6C1im][PF6] and [C8C1im][PF6] remain in an amorphous phase up to 3.5 GPa, in contrast to [C4C1im][PF6], which crystallizes above ~0.5 GPa. Equations of state based either on a group contribution model or Carnahan-Starling-van der Waals model have been used to estimate the densities of the ionic liquids at high pressures. The shifts of the vibrational frequency of νs(PF6) with density observed in [C6C1im][PF6] and in [C8C1im][PF6] have been calculated by a hard-sphere model of a pseudo-diatomic solute under short-range repulsive interactions with the neighboring particles. The stochastic model of Kubo for vibrational dephasing has been used to obtain the amplitude of vibrational frequency fluctuation, <Δω(2)>, and the relaxation time of frequency fluctuation, τc, as a function of density by Raman band shape analysis of the νs(PF6) mode of [C6C1im][PF6] and [C8C1im][PF6].
在室温下,我们测量了 1-烷基-3-甲基咪唑鎓离子液体 [CnC1im][PF6](n = 4、6 和 8)中 PF6阴离子的完全对称伸缩模式 νs(PF6)的拉曼光谱,作为压力的函数。[C6C1im][PF6]和 [C8C1im][PF6]离子液体在 3.5 GPa 以下保持非晶相,而 [C4C1im][PF6]则在 ~0.5 GPa 以上结晶。我们使用了基于基团贡献模型或 Carnahan-Starling-van der Waals 模型的状态方程来估算高压下离子液体的密度。通过短程排斥相互作用与相邻粒子的硬球模型,我们计算了在 [C6C1im][PF6]和 [C8C1im][PF6]中观察到的 νs(PF6)振动频率随密度的位移。我们使用 Kubo 的振动退相随机模型,通过对 [C6C1im][PF6]和 [C8C1im][PF6]的 νs(PF6)模式的拉曼光谱分析,获得了振动频率涨落的幅度 <Δω(2)> 和频率涨落的弛豫时间 τc 随密度的函数关系。