Rayleigh-Gans theory of light scattering by liquid crystals filled with cylindrical particles
Rayleigh-Gans theory of light scattering by liquid crystals filled with cylindrical particles
Light scattering cross-sections by the director inhomogeneity near small cylindrical particles in a nematic cell are calculated in the Rayleigh-Gans approximation. We use the Percus-Yevick approximation to account for interference effects and study the influence of the boundary conditions on the particle surface as well as the effect of an external electric field on the angular dependence and on the magnitude of the light scattering cross-section.
139-146
Lednei, M.F.
172e077e-5880-4e55-a0cf-64a61e9250b4
Pinkevich, I.P.
3bc6385f-a71b-419c-9996-0cc566e9b687
Reshetnyak, V.Yu.
1443c2dd-2066-4dd6-ae18-f3b408dea98d
Sluckin, T.J.
8dbb6b08-7034-4ae2-aa65-6b80072202f6
2001
Lednei, M.F.
172e077e-5880-4e55-a0cf-64a61e9250b4
Pinkevich, I.P.
3bc6385f-a71b-419c-9996-0cc566e9b687
Reshetnyak, V.Yu.
1443c2dd-2066-4dd6-ae18-f3b408dea98d
Sluckin, T.J.
8dbb6b08-7034-4ae2-aa65-6b80072202f6
Lednei, M.F., Pinkevich, I.P., Reshetnyak, V.Yu. and Sluckin, T.J.
(2001)
Rayleigh-Gans theory of light scattering by liquid crystals filled with cylindrical particles.
Journal of Molecular Liquids, 92 (1-2), .
(doi:10.1016/S0167-7322(01)00186-6).
Abstract
Light scattering cross-sections by the director inhomogeneity near small cylindrical particles in a nematic cell are calculated in the Rayleigh-Gans approximation. We use the Percus-Yevick approximation to account for interference effects and study the influence of the boundary conditions on the particle surface as well as the effect of an external electric field on the angular dependence and on the magnitude of the light scattering cross-section.
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Published date: 2001
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Local EPrints ID: 39262
URI: http://eprints.soton.ac.uk/id/eprint/39262
PURE UUID: a6786980-ce6d-438e-8f05-c1cc8d644f1c
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Date deposited: 26 Jun 2006
Last modified: 16 Mar 2024 02:32
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Author:
M.F. Lednei
Author:
I.P. Pinkevich
Author:
V.Yu. Reshetnyak
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