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Saddle-splay term induced orientational instability in nematic liquid crystal cells and director fluctuations at substrates

机译:马鞍形术语引起向列液体中的取向不稳定性   基板上的晶体和导向器波动

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摘要

We analyze stability of the planar orientational structure in a nematicliquid crystal (NLC) cell with planar anchoring conditions at both substrates.Specifically, we study the instabilities of the ground state caused by surfaceelasticity at large saddle-splay elastic constant, $K_{24}$. For relativelysmall $K_{24}$ violating the Ericksen inequalities the theory predicts that thecritical fluctuation mode of the wavelength, $\lambda_c$, will render thestructure unstable when the thickness of the cell is below its critical value,$d_c$. The parity of the critical mode changes as the twist-splay ratio$K_2/K_1$ is passing through the unity. Further increase of $K_{24}$ beyond thesecond threshold value, $4K_1K_2/(K_1+K_2)$, leads to the instability withrespect to the short wavelength fluctuations regardless of the cell thickness.We compute the critical thickness and the critical wavelength as functions of$K_{24}$, the twist-splay ratio and the azimuthal anchoring strength.
机译:我们分析了在两个基板上具有平面锚定条件的向列液晶(NLC)单元中平面取向结构的稳定性。特别是,我们研究了在大鞍展弹性常数$ K_ {24}下由表面弹性引起的基态不稳定性$。对于相对较小的$ K_ {24} $违反埃里克森不等式的理论,该理论预测,当单元的厚度低于其临界值$ d_c $时,波长的临界波动模式$ \ lambda_c $将使结构不稳定。临界模式的奇偶性随着扭曲比$ K_2 / K_1 $通过单位而改变。 $ K_ {24} $超过第二阈值$ 4K_1K_2 /(K_1 + K_2)$的进一步增加,导致与短波长波动无关的不稳定,无论单元厚度如何。我们将临界厚度和临界波长计算为$ K_ {24} $的功能,扭曲比和方位锚固强度。

著录项

  • 作者

    Kiselev, A. D.;

  • 作者单位
  • 年度 2003
  • 总页数
  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
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