Elgeti J, Schmid F
Theoretische Physik, Universität Bielefeld, 33501 Bielefeld, Germany.
Eur Phys J E Soft Matter. 2005 Dec;18(4):407-15. doi: 10.1140/epje/e2005-00051-8. Epub 2005 Dec 6.
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.
在弗兰克弹性理论和朗道-德热纳理论的框架内,对粗糙且起伏界面处的向列型液晶进行了分析。我们特别研究了局部有利于平面锚定的界面。在第一部分中,我们重新审视了在固定粗糙表面上的贝里曼锚定现象,并推导了相应方位角锚定能的新的简单表达式。令人惊讶的是,我们发现对于强取向表面,它仅取决于几何表面各向异性和体弹性常数,而不取决于化学表面参数的精确值。在第二部分中,我们计算了向列型-各向同性界面处的毛细波。如果忽略弹性相互作用,毛细波谱的特征是具有各向异性的界面张力。考虑弹性相互作用时,界面张力,即毛细波谱中主导的q(2)项的系数,变为各向同性。然而,弹性相互作用引入了一个强各向异性的三次方q(3)项。毛细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结果一致。