NT PNAS Plus: Nematic twist–bend phase in an external field
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PNAS Plus: Nematic twist–bend phase in an external field

机译:PNAS Plus:向列型向内弯曲-外部领域

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摘要

The response of the nematic twist–bend (NTB) phase to an applied field can provide important insight into the structure of this liquid and may bring us closer to understanding mechanisms generating mirror symmetry breaking in a fluid of achiral molecules. Here we investigate theoretically how an external uniform field can affect structural properties and the stability of NTB. Assuming that the driving force responsible for the formation of this phase is packing entropy, we show, within Landau–de Gennes theory, that NTB can undergo a rich sequence of structural changes with the field. For the systems with positive anisotropy of permittivity, we first observe a decrease of the tilt angle of NTB until it transforms through a field-induced phase transition to the ordinary prolate uniaxial nematic phase (N). Then, at very high fields, this nematic phase develops polarization perpendicular to the field (Np+). For systems with negative anisotropy of permittivity, the results reveal new modulated structures. Even an infinitesimally small field transforms NTB to its elliptical counterpart (NTBe), where the circular base of the cone of the main director becomes elliptic. With stronger fields, the ellipse degenerates to a line, giving rise to a nonchiral periodic structure, the nematic splay–bend (NSB), where the two nematic directors are restricted to a plane. The three structures—NTB, NTBe, and NSB—with a modulated polar order are globally nonpolar. But further increase of the field induces phase transitions into globally polar structures with nonvanishing polarization along the field’s direction. We found two such structures, one of which is a polar and chiral modification of NSB, where splay and bend deformations are accompanied by weak twist deformations (NSB*p). Further increase of the field unwinds this structure into a polar nematic (Np) of polarization parallel to the field.
机译:向列弯曲的响应( < mi> N T B N T B 。假设负责此阶段形成的驱动力是堆积熵,我们在Landau-de Gennes理论中证明, N T B 可以随场经历一系列丰富的结构变化。对于介电常数为正各向异性的系统,我们首先观察到 N T B ,直到它通过场致相变转变为普通的扁长单轴向列相( N )。然后,在非常高的磁场下,该向列相会垂直于磁场形成极化( N p + )。对于介电常数为负各向异性的系统,结果揭示了新的调制结构。甚至是一个无限小的字段也会转换 N T B 到它的椭圆形对应对象( N T B e ),其中主指向矢的圆锥体的圆形底部变为椭圆形。随着磁场的增强,椭圆会退化为一条线,从而产生非手性的周期性结构,即向列八字形弯曲( N S B ),其中两个向列导向器仅限于飞机。这三个结构-<数学xmlns:mml =“ http://www.w3.org/1998/Math/MathML” id =“ i10” overflow =“ scroll”> N T B N T B e ,和 N < / mrow> S B -具有调制的极性顺序在全球范围内是非极性的。但是,磁场的进一步增加会导致相转变为整体极性的结构,且沿电场方向极化不消失。我们发现了两个这样的结构,其中之一是 N S B ,其中展开和弯曲变形伴随着较弱的扭曲变形( N S B * p )。字段的进一步增加使该结构解散为极向列型( 极化平行的 N p - 到现场。

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