Polar order in a fluid like ferroelectric with a tilted lamellar structure -- observation of a polar smectic C (SmC${_\textrm{P}}$) phase

Jordan Hobbs, Calum J. Gibb, Damian Pociecha, Jadwiga Szydłowska, Ewa Górecka, Richard. J. Mandle
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Abstract

The discovery of fluid states of matter with spontaneous bulk polar order is appreciated as a major discovery in the fields of soft matter and liquid crystals. Typically, this manifests as polar order superimposed atop conventional phase structures and is thus far limited to orthogonal phase types. Here we report a family of materials which exhibit a previously unseen state of matter which we conclude is a polar smectic C phase, and so we term it SmC${_\textrm{P}}$. The spontaneous polarisation of the SmC${_\textrm{P}}$ phase is over two orders of magnitude larger than that found in conventional ferroelectric SmC phase of chiral materials used in some LCD devices. Fully atomistic molecular dynamics simulations faithfully and spontaneously reproduce the proposed structure and associated bulk properties; comparison of experimental and simulated X-ray scattering patterns shows excellent agreement. The materials disclosed here have significantly smaller dipole moments than typical polar liquid crystals such as RM734 which suggests the role of molecular electrical polarity in generating polar order is perhaps overstated, a view supported by consideration of other molecular systems.
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具有倾斜片层结构的类流体铁电中的极性秩序--观察到极性 Smectic C (SmC${_\textrm{P}}$) 相
具有自发体极性阶的流态物质的发现是软物质和液晶领域的重大发现。通常情况下,这表现为叠加在传统相结构之上的极性有序,迄今为止仅限于正交相型。在这里,我们报告了一系列材料,它们展示了一种以前从未见过的物质状态,我们断定这是一种极性共晶 C 相,因此我们称之为 SmC${_textrm{P}}$。SmC${_textrm{P}}$相的自发极化比某些液晶显示设备中使用的手性材料的传统铁电SmC相的自发极化大两个数量级以上。完全原子分子动力学模拟忠实地、自发地再现了所提出的结构和相关的体质特性;实验和模拟 X 射线散射模式的比较显示出极好的一致性。本文所揭示的材料的偶极矩明显小于典型的极性液晶(如 RM734),这表明分子电极性在产生极性秩序中的作用可能被夸大了,而对其他分子系统的研究也支持这一观点。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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