First-order liquid crystal orientation transition on inhomogeneous substrates.

Phys Rev E Stat Nonlin Soft Matter Phys

Department of Physics and Institute of Nano Science and Technology, Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong.

Published: February 2004

AI Article Synopsis

  • Researchers discovered a unique transition in liquid crystal (LC) alignment when tested on microtextured substrates with alternating patterns, where the transition occurred as the period neared 1 micrometer.
  • This transition shifted the LC from a non-uniform planar state to a more uniform configuration with a notable pretilt angle of around 40 degrees.
  • A theoretical model based on elastic energy and surface potential effectively explained the transition, revealing it occurs in two steps and that the polar anchoring energy is significantly lower than usual, with specific terms found to play a dominant role.

Article Abstract

In a recent experiment, we uncovered an unconventional liquid crystal (LC) orientation transition on microtextured substrates consisting of alternating horizontal and vertical corrugations. When the period of alternation was decreased toward approximately 1 microm, the LC alignment underwent an abrupt transition from inhomogeneous planar to a more uniform configuration with a large pretilt angle ( approximately 40 degrees ). With the aid of a model based on the competition between the Frank-Oseen elastic energy and a phenomenological surface potential of the form W(theta,phi)=(1/2)W((2))(theta) sin(2) theta+(1/4)W((4))(theta) sin(4) theta+(1/2)W(phi) cos(2) theta sin(2) phi(x,y) (where theta and phi are, respectively, the pretilt and azimuthal angles of the LC director and W((2))(theta), W((4))(theta), and W(phi) are constants) that demonstrated good agreement with experiment, we investigated the microscopic origin of the observed transition. It was found that this transition comprises two steps. First, the LC director homogenizes toward the phi=45 degrees azimuthal direction in the plane to relax the elastic energy. The resulting rise in azimuthal anchoring energy subsequently drives the LC to adopt a finite pretilt. The values of the W's deduced from the model reveal that the polar anchoring energy is about approximately 1/10 of the typical values, with the sin(4) theta term dominating the sin(2) theta term. We present a possible explanation for this unexpected finding.

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http://dx.doi.org/10.1103/PhysRevE.69.021704DOI Listing

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