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arXiv 2409.04019cond-mat.soft
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铁电向列领域中的自由悬浮向列相和近晶相薄膜及独立支撑近晶相丝

Freely Suspended Nematic and Smectic Films and Free-Standing Smectic Filaments in the Ferroelectric Nematic Realm

Keith G. Hedlund, Vikina Martinez, Xi Chen, Cheol S. Park, Joseph E. Maclennan, Matthew A. Glaser, Noel A. Clark

AI总结:

本研究发现铁电向列相及新型极性层状相可形成稳定自由悬浮薄膜与独立细丝,其独特织构由极化场静电自相互作用稳定,为受限流体结构研究提供新体系。

摘要:

我们证明,稳定的自由悬浮液晶薄膜可由铁电向列相($\text{N}_\text{F}$)以及最近发现的极性层状相$\text{SmZ}_\text{A}$和$\text{SmA}_\text{F}$制成。$\text{N}_\text{F}$薄膜呈现二维近晶状抛物焦锥织构,包含指向矢/极化弯曲,这是薄膜平面内指向矢展曲被静电抑制的体现。在$\text{SmZ}_\text{A}$和$\text{SmA}_\text{F}$相中,近晶层优先沿薄膜表面法线方向取向,这一状态在典型热致或溶致层状液晶相中从未发现;$\text{SmZ}_\text{A}$薄膜展现焦锥扇形织构,类似玻璃盒中近晶相层沿平板法线取向时的外观,而$\text{SmA}_\text{F}$薄膜呈现面内取向均匀的斑块织构(弯曲和展曲均被抑制),斑块间由晶界分隔。$\text{SmA}_\text{F}$相还可拉制成细丝,X射线散射显示其近晶层平面沿细丝轴法线方向。值得注意的是,这些细丝即使断裂仍机械稳定,形成仅一端支撑的独立流体细丝。这些薄膜和细丝的独特结构由液晶极化场的静电自相互作用稳定,从而能够形成受限流体结构,与使用已知液晶相制成的对应结构存在根本差异。

英文摘要:

We show that stable, freely suspended liquid crystal films can be made from the ferroelectric nematic ($\mathrm{N_F}$) phase and from the recently discovered polar, lamellar $\mathrm{SmZ_A}$ and $\mathrm{SmA_F}$ phases. The $\mathrm{N_F}$ films display two-dimensional, smectic-like parabolic focal conic textures comprising director/polarization bend that are a manifestation of the electrostatic suppression of director splay in the film plane. In the $\mathrm{SmZ_A}$ and $\mathrm{SmA_F}$ phases, the smectic layers orient preferentially normal to the film surfaces, a condition never found in typical thermotropic or lyotropic lamellar LC phases, with the $\mathrm{SmZ_A}$ films exhibiting focal-conic fan textures mimicking the appearance of typical smectics in glass cells when the layers are oriented normal to the plates, and the $\mathrm{SmA_F}$ films showing a texture of plaquettes of uniform in-plane orientation where both bend and splay are suppressed, separated by grain boundaries. The $\mathrm{SmA_F}$ phase can also be drawn into thin filaments, in which X-ray scattering reveals that the smectic layer planes are normal to the filament axis. Remarkably, the filaments are mechanically stable even if they break, forming free-standing, fluid filaments supported only at one end. The unique architectures of these films and filaments are stabilized by the electrostatic self-interaction of the liquid crystal polarization field, which enables the formation of confined, fluid structures that are fundamentally different from those of their counterparts made using previously known liquid crystal phases.

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