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限制在纳米多孔固体中的液晶的非均匀弛豫动力学和相行为。

Inhomogeneous relaxation dynamics and phase behaviour of a liquid crystal confined in a nanoporous solid.

作者信息

Całus Sylwia, Kityk Andriy V, Eich Manfred, Huber Patrick

机构信息

Faculty of Electrical Engineering, Czestochowa University of Technology, Al. Armii Krajowej 17, 42-200 Czestochowa, Poland.

出版信息

Soft Matter. 2015 Apr 28;11(16):3176-87. doi: 10.1039/c5sm00108k.

Abstract

We report filling-fraction dependent dielectric spectroscopy measurements on the relaxation dynamics of the rod-like nematogen 7CB condensed in 13 nm silica nanochannels. In the film-condensed regime, a slow interface relaxation dominates the dielectric spectra, whereas from the capillary-condensed state up to complete filling an additional, fast relaxation in the core of the channels is found. The temperature-dependence of the static capacitance, representative of the averaged, collective molecular orientational ordering, indicates a continuous, paranematic-to-nematic (P-N) transition, in contrast to the discontinuous bulk behaviour. It is well described by a Landau-de-Gennes free energy model for a phase transition in cylindrical confinement. The large tensile pressure of 10 MPa in the capillary-condensed state, resulting from the Young-Laplace pressure at highly curved liquid menisci, quantitatively accounts for a downward-shift of the P-N transition and an increased molecular mobility in comparison to the unstretched liquid state of the complete filling. The strengths of the slow and fast relaxations provide local information on the orientational order: the thermotropic behaviour in the core region is bulk-like, i.e. it is characterized by an abrupt onset of the nematic order at the P-N transition. By contrast, the interface ordering exhibits a continuous evolution at the P-N transition. Thus, the phase behaviour of the entirely filled liquid crystal-silica nanocomposite can be quantitatively described by a linear superposition of these distinct nematic order contributions.

摘要

我们报告了对凝聚在13纳米二氧化硅纳米通道中的棒状向列型液晶7CB的弛豫动力学进行的与填充分数相关的介电谱测量。在薄膜凝聚状态下,缓慢的界面弛豫主导介电谱,而从毛细管凝聚状态到完全填充,在通道核心发现了另一种快速弛豫。代表平均集体分子取向有序的静态电容的温度依赖性表明存在连续的顺向列相到向列相(P-N)转变,这与不连续的体相行为形成对比。它可以用朗道 - 德热纳自由能模型很好地描述圆柱形受限体系中的相变。毛细管凝聚状态下由高度弯曲的液体弯月面处的杨 - 拉普拉斯压力产生的10兆帕的大拉伸压力,定量地解释了P-N转变的向下移动以及与完全填充的未拉伸液态相比分子迁移率的增加。慢弛豫和快弛豫的强度提供了关于取向有序的局部信息:核心区域的热致行为类似体相,即其特征是在P-N转变处向列相有序突然出现。相比之下,界面有序在P-N转变处表现出连续演变。因此,完全填充的液晶 - 二氧化硅纳米复合材料的相行为可以通过这些不同向列相有序贡献的线性叠加来定量描述。

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