2004
DOI: 10.1080/15421400490440165
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Alignment of Nematic Liquid Crystal on the Surface with Spatial Distribution of Easy Axis and Anchoring Energy

Abstract: In this report we consider behaviour of nematic LC on randomly aligning surface. We solved the theoretical problem on spatial distribution of director on a tested surface where easy axis lies in the azimuthal plane and is randomly distributed over the surface. We found that in combined cell angular distribution of director on the tested surface strongly depends on anchoring parameter and its dispersion. For strong anchoring the director distribution practically coincides with the easy axis distribution. Weaker… Show more

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Cited by 9 publications
(10 citation statements)
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“…The HNF walls act on the director field of the guest as strongly anchoring, nanotextured sheets, with n(r) disordered on the nanoscale near the HNF sheets but annealing to order out to larger length scales with increasing distance from the HNFs, a scale comparable to the pore dimension in the middle of a pore. This results in an effective orientational anchoring that is much weaker than that on the HNF surface, in the same way that solid substrates having random orientations patterned on the nanoscale produce nearly-degenerate azimuthal alignment of a contacting bulk nematic [64][65][66][67] .…”
Section: δN<0 δN<0mentioning
confidence: 99%
“…The HNF walls act on the director field of the guest as strongly anchoring, nanotextured sheets, with n(r) disordered on the nanoscale near the HNF sheets but annealing to order out to larger length scales with increasing distance from the HNFs, a scale comparable to the pore dimension in the middle of a pore. This results in an effective orientational anchoring that is much weaker than that on the HNF surface, in the same way that solid substrates having random orientations patterned on the nanoscale produce nearly-degenerate azimuthal alignment of a contacting bulk nematic [64][65][66][67] .…”
Section: δN<0 δN<0mentioning
confidence: 99%
“…Placing the LC layer between two polarizers, one can obtain the interference oscillations with the light intensity maxima and minima by changing the phase difference between the ordinary and extraordinary beams using an external electric or magnetic field under the conditions of the Frederiks transition [2]. In the misoriented LC layers, the birefringence effects can be observed without polarizers [3][4][5]. In [3], the interference maxima and minima were found using the monochromatic light.…”
Section: Introductionmentioning
confidence: 99%
“…30 Surface randomness and resulting orientational quenched disorder also are important in liquid crystalline systems. [35][36][37][38] In their pioneering experiment Nespoulous, et al used a two-dimensional CCD array to image a 10 mm thick hybrid cell, planar alignment imposed by oblique evaporation of SiO x at one surface and vertical alignment at the other, which was arranged between crossed polarizers. Both theory and experiment are well represented, covering not only the nematic phase, but smectic phases as well.…”
Section: Introductionmentioning
confidence: 99%