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铁电向列相材料RM734中的热致折返各向同性对称性和诱导近晶反铁电性

Thermotropic reentrant isotropic symmetry and induced smectic antiferroelectricity in the ferroelectric nematic material RM734.

作者信息

Chen Xi, Shuai Min, Zhong Bingchen, Martinez Vikina, Korblova Eva, Glaser Matthew A, Maclennan Joseph E, Walba David M, Clark Noel A

机构信息

Department of Physics and Soft Materials Research Center, University of Colorado, Boulder, CO 80309.

Department of Chemistry and Soft Materials Research Center, University of Colorado, Boulder, CO 80309.

出版信息

Proc Natl Acad Sci U S A. 2025 Apr 22;122(16):e2424917122. doi: 10.1073/pnas.2424917122. Epub 2025 Apr 18.

Abstract

We report a transition from the ferroelectric nematic liquid crystal (N) phase to a lower-temperature, apolar fluid phase having reentrant isotropic symmetry (I), in the liquid crystal compound RM734 doped with small concentrations of the ionic liquids 1-Butyl-3-methylimidazolium hexafluorophosphate (BMIM-PF) or 1-Ethyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide (EMIM-TFSI). Even a trace amount of ionic liquid dopant facilitates the kinetic pathway for the transition from the N to the I, enabling simple cooling to produce this isotropic fluid phase rather than resulting in immediate crystallization. The I was also obtained in the absence of specific ionic liquid doping by appropriate temperature cycling in three distinct, as-synthesized-and-purified batches of RM734, two commercial and one from our laboratory. Ionic liquid doping also stabilizes the smectic Z, an additional birefringent antiferroelectric phase having the director parallel to fluid smectic layers, significantly increasing its temperature range between the paraelectric and ferroelectric nematic phases with increasing BMIM concentration.

摘要

我们报道了在掺杂低浓度离子液体1-丁基-3-甲基咪唑六氟磷酸盐(BMIM-PF)或1-乙基-3-甲基咪唑双(三氟甲基磺酰)亚胺(EMIM-TFSI)的液晶化合物RM734中,从铁电向列相(N)到具有再入各向同性对称性(I)的低温非极性流体相的转变。即使是痕量的离子液体掺杂剂也有助于从N相到I相转变的动力学途径,使得简单冷却就能产生这种各向同性流体相,而不是立即结晶。在三个不同的、合成并纯化的RM734批次(两批市售的和一批我们实验室自制的)中,通过适当的温度循环,在没有特定离子液体掺杂的情况下也获得了I相。离子液体掺杂还稳定了近晶Z相,这是一种额外的双折射反铁电相,其指向矢平行于流体近晶层,随着BMIM浓度的增加,显著增加了其顺电相和铁电向列相之间的温度范围。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6156/12036992/45b8c836a404/pnas.2424917122fig01.jpg

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