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偏振调制近晶相液晶相。

Polarization-modulated smectic liquid crystal phases.

作者信息

Coleman D A, Fernsler J, Chattham N, Nakata M, Takanishi Y, Körblova E, Link D R, Shao R-F, Jang W G, Maclennan J E, Mondainn-Monval O, Boyer C, Weissflog W, Pelzl G, Chien L-C, Zasadzinski J, Watanabe J, Walba D M, Takezoe H, Clark N A

机构信息

Department of Physics and Ferroelectric Liquid Crystal Materials Research Center, University of Colorado, Boulder, CO80309 - 0390, USA.

出版信息

Science. 2003 Aug 29;301(5637):1204-11. doi: 10.1126/science.1084956.

Abstract

Any polar-ordered material with a spatially uniform polarization field is internally frustrated: The symmetry-required local preference for polarization is to be nonuniform, i.e., to be locally bouquet-like or "splayed." However, it is impossible to achieve splay of a preferred sign everywhere in space unless appropriate defects are introduced into the field. Typically, in materials like ferroelectric crystals or liquid crystals, such defects are not thermally stable, so that the local preference is globally frustrated and the polarization field remains uniform. Here, we report a class of fluid polar smectic liquid crystals in which local splay prevails in the form of periodic supermolecular-scale polarization modulation stripes coupled to layer undulation waves. The polar domains are locally chiral, and organized into patterns of alternating handedness and polarity. The fluid-layer undulations enable an extraordinary menagerie of filament and planar structures that identify such phases.

摘要

任何具有空间均匀极化场的极性有序材料在内部都会受到阻碍

从对称性角度来看,极化场局部应具有非均匀性倾向,即呈局部花束状或“展开状”。然而,除非在该场中引入适当的缺陷,否则不可能在空间各处都实现具有特定方向的展开。通常,在铁电晶体或液晶等材料中,此类缺陷并非热稳定的,因此局部倾向在全局范围内受到阻碍,极化场保持均匀。在此,我们报道了一类流体极性近晶液晶,其中局部展开以周期性超分子尺度极化调制条纹的形式存在,这些条纹与层状起伏波相耦合。极性畴局部呈手性,并组织成交替的手性和极性图案。流体层状起伏使得这类相呈现出一系列独特的丝状和平板状结构。

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