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限制铁电向列相的介电常数的值。

Constraining the value of the dielectric constant of the ferroelectric nematic phase.

作者信息

Erkoreka Aitor, Martinez-Perdiguero Josu

机构信息

Department of Physics, Faculty of Science and Technology, <a href="https://ror.org/000xsnr85">University of the Basque Country</a> UPV/EHU, Bilbao, Spain.

出版信息

Phys Rev E. 2024 Aug;110(2):L022701. doi: 10.1103/PhysRevE.110.L022701.

DOI:10.1103/PhysRevE.110.L022701
PMID:39294943
Abstract

Ferroelectric nematic liquid crystals are currently being subject to a plethora of investigations since they are of great fundamental interest and could potentially foster promising applications. However, many basic aspects are still poorly understood, among which the problem of the dielectric constant stands out. Ferroelectric nematics have previously been reported to exhibit giant dielectric constants whose value depends on the thickness of the measurement cell, claims that have recently been shown to be the result of an incorrect interpretation of the experimental data. The intrinsic permittivity of these materials has not been determined yet. In this work, we tackle this problem by modeling the dielectric response of the liquid crystal filled cell through an equivalent circuit proposed by Clark et al. [Phys. Rev. Res. 6, 013195 (2024)2643-156410.1103/PhysRevResearch.6.013195] accounting for polarization reorientation and the effect of insulating interfacial layers. We arrive at the conclusion that the perpendicular component of the permittivity ɛ_{⊥} is of the order of 10 in the prototypical ferroelectric nematogen DIO, while the parallel component ɛ_{∥} is of the order of 150. In this way, the dielectric tensor of DIO has been fully determined.

摘要

铁电向列型液晶目前正受到大量研究,因为它们具有极大的基础研究价值,并且可能孕育出有前景的应用。然而,许多基本方面仍未得到充分理解,其中介电常数问题尤为突出。此前有报道称铁电向列型液晶表现出巨大的介电常数,其值取决于测量盒的厚度,但最近已证明这些说法是对实验数据错误解读的结果。这些材料的本征介电常数尚未确定。在这项工作中,我们通过采用Clark等人提出的等效电路[《物理评论研究》6, 013195 (2024)2643 - 156410.1103/PhysRevResearch.6.013195]对填充液晶的盒子的介电响应进行建模,该等效电路考虑了极化重新取向和绝缘界面层的影响,从而解决了这个问题。我们得出的结论是,在典型的铁电向列型液晶DIO中,介电常数的垂直分量ɛ⊥约为10,而平行分量ɛ∥约为150。通过这种方式,DIO的介电张量已被完全确定。

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