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向列型液体中的反铁电序:挠曲电与静电学

Antiferroelectric Order in Nematic Liquids: Flexoelectricity Versus Electrostatics.

作者信息

Medle Rupnik Peter, Hanžel Ema, Lovšin Matija, Osterman Natan, Gibb Calum Jordan, Mandle Richard J, Sebastián Nerea, Mertelj Alenka

机构信息

Jožef Stefan Institute, Ljubljana, 1000, Slovenia.

Faculty of Mathematics and Physics, University of Ljubljana, Ljubljana, 1000, Slovenia.

出版信息

Adv Sci (Weinh). 2025 Mar;12(9):e2414818. doi: 10.1002/advs.202414818. Epub 2025 Jan 9.

Abstract

The recent discovery of ferroelectric nematic liquid crystalline phases marks a major breakthrough in soft matter research. An intermediate phase, often observed between the nonpolar and the ferroelectric nematic phase, shows a distinct antiferroelectric response to electric fields. However, its structure and formation mechanisms remain debated, with flexoelectric and electrostatics effects proposed as competing mechanisms. By controlling the magnitude of electrostatic forces through ion addition in two representative ferroelectric nematic materials, it is shown that the primary mechanism for the emergence of antiferroelectric order is the flexoelectric coupling between electric polarization and splay deformation of the nematic director. The addition of ions significantly expands the temperature range over which the antiferroelectric phase is observed, with this range increasing with increasing ion concentration. Polarizing optical microscopy studies and second harmonic generation (SHG) microscopy reveal the splayed structure modulated in 2D, while SHG interferometry confirms its antiferroelectric character. The model previously used to describe pretransitional behavior is extended by incorporating the electrostatic contribution of ions. The model shows qualitative agreement with the experiments, accurately reproducing the phase diagram and temperature-dependent evolution of the modulation period of the observed structure.

摘要

铁电向列相液晶相的近期发现标志着软物质研究的一项重大突破。在非极性相和铁电向列相之间经常观察到的一个中间相,对电场表现出明显的反铁电响应。然而,其结构和形成机制仍存在争议,挠曲电效应和静电效应被认为是相互竞争的机制。通过在两种代表性的铁电向列材料中添加离子来控制静电力的大小,结果表明反铁电有序出现的主要机制是极化与向列指向矢的展曲变形之间的挠曲电耦合。离子的添加显著拓宽了观察到反铁电相的温度范围,该范围随着离子浓度的增加而增大。偏振光学显微镜研究和二次谐波产生(SHG)显微镜揭示了二维调制的展曲结构,而SHG干涉测量证实了其反铁电特性。通过纳入离子的静电贡献,扩展了先前用于描述转变前行为的模型。该模型与实验结果在定性上一致,准确地再现了相图以及所观察结构的调制周期随温度的变化。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/00d1/11884549/211f8572c53f/ADVS-12-2414818-g010.jpg

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