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Nematic liquid crystals at rough and fluctuating interfaces

机译:向列液晶在粗糙且波动的界面处

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Nematic liquid crystals at rough and fluctuating interfaces are analyzed within the Frank elastic theory and the Landau-de Gennes theory. We study specifically interfaces that locally favor planar anchoring. In the first part we reconsider the phenomenon of Berreman anchoring on fixed rough surfaces, and derive new simple expressions for the corresponding azimuthal anchoring energy. Surprisingly, we find that for strongly aligning surfaces, it depends only on the geometrical surface anisotropy and the bulk elastic constants, and not on the precise values of the chemical surface parameters. In the second part, we calculate the capillary waves at nematic-isotropic interfaces. If one neglects elastic interactions, the capillary wave spectrum is characterized by an anisotropic interfacial tension. With elastic interactions, the interfacial tension, i.e., the coefficient of the leading q(2) term of the capillary wave spectrum, becomes isotropic. However, the elastic interactions introduce a strongly anisotropic cubic q(3) term. The amplitudes of capillary waves are largest in the direction perpendicular to the director. These results are in agreement with previous molecular dynamics simulations.
机译:在弗兰克弹性理论和朗道·德·金尼斯理论中,分析了粗糙和波动界面处的向列液晶。我们专门研究了局部偏爱平面锚固的界面。在第一部分中,我们重新考虑了Berreman锚固在固定粗糙表面上的现象,并推导了相应方位角锚固能量的新简单表达式。出乎意料的是,我们发现对于高度对齐的表面,它仅取决于几何表面各向异性和整体弹性常数,而不取决于化学表面参数的精确值。在第二部分中,我们计算向列各向同性界面处的毛细管波。如果忽略弹性相互作用,则毛细管波谱的特征在于各向异性界面张力。通过弹性相互作用,界面张力,即毛细管波谱的前导q(2)项的系数变为各向同性。但是,弹性相互作用引入了强各向异性立方q(3)项。毛细管波的振幅在垂直于指向矢的方向上最大。这些结果与先前的分子动力学模拟一致。

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