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咪唑鎓-PF6离子液体中的溶剂化动力学和电场弛豫:从室温到玻璃化转变

Solvation dynamics and electric field relaxation in an imidazolium-PF6 ionic liquid: from room temperature to the glass transition.

作者信息

Ito Naoki, Richert Ranko

机构信息

Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA.

出版信息

J Phys Chem B. 2007 May 10;111(18):5016-22. doi: 10.1021/jp0640023.

Abstract

Time-resolved phosphorescence spectra and anisotropy of quinoxaline were measured in an ionic liquid, 1-butyl-3-methylimidazolium hexafluorophosphate (BMIM-HFP), in its supercooled state near the glass-transition temperature. The solvation dynamics results are compared with the rotational motion of the probe and with the dielectric behavior of the neat ionic liquid. The dynamics in the viscous state are highly dispersive and show a super-Arrhenius temperature dependence, as typical for glass-forming materials. Combined with room-temperature results, solvation dynamics is observed to follow the structural relaxation times in terms of eta/T for more than 10 decades, from subnanoseconds at room temperature to seconds near the glass-transition temperature T(g). The dielectric modulus relaxation follows this trend only for temperatures T > 1.2T(g) and departs significantly from eta/T in the 1.1T(g) > T > T(g) range. This deviation is reminiscent of the enhanced translational diffusion or fractional Stokes-Einstein behavior observed in many fragile supercooled liquids. Because the electric field relaxation in BMIM-HFP includes dc conductivity, this correlation function involves translational motion and thus displays the effect of enhanced diffusivity. A microscopic model is required for rationalizing the decoupling of solvation dynamics from the longitudinal time scales and the limitation of this effect to the viscous regime with T < 1.2T(g).

摘要

在离子液体1-丁基-3-甲基咪唑六氟磷酸盐(BMIM-HFP)处于接近玻璃化转变温度的过冷状态下,测量了喹喔啉的时间分辨磷光光谱和各向异性。将溶剂化动力学结果与探针的旋转运动以及纯离子液体的介电行为进行了比较。粘性状态下的动力学具有高度分散性,并表现出超阿累尼乌斯温度依赖性,这是玻璃形成材料的典型特征。结合室温结果,观察到溶剂化动力学在超过10个数量级的η/T范围内遵循结构弛豫时间,从室温下的亚纳秒到接近玻璃化转变温度T(g)时的秒级。仅在温度T > 1.2T(g)时,介电模量弛豫遵循这一趋势,而在1.1T(g) > T > T(g)范围内与η/T有显著偏差。这种偏差让人联想到在许多脆弱的过冷液体中观察到的增强的平移扩散或分数斯托克斯-爱因斯坦行为。由于BMIM-HFP中的电场弛豫包括直流电导率,这种相关函数涉及平移运动,因此显示出增强扩散率的效应。需要一个微观模型来解释溶剂化动力学与纵向时间尺度的解耦以及这种效应在T < 1.2T(g)的粘性区域的局限性。

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