Issue |
J. Phys. II France
Volume 2, Number 10, October 1992
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Page(s) | 1881 - 1888 | |
DOI | https://doi.org/10.1051/jp2:1992241 |
J. Phys. II France 2 (1992) 1881-1888
Saddle-splay and periodic instability in a hybrid aligned nematic layer subjected to a normal magnetic field
A. Sparavigna1, L. Komitov2, O. D. Lavrentovich3, 4 and A. Strigazzi11 Dipartimento di Fisica, Politecnico di Torino, CISM and INFM, Unità di Torino, C. so Duca degli Abruzzi 24, I-10129 Torino, Italy
2 Physics Department, Chalmers University of Technology, S-41296 Göteborg, Sweden
3 Laboratoire de Physique des Solides, associé au CNRS, Bât. 510, Université de Paris-Sud, F-91405 Orsay, France
4 Institute of Physics, Academy of Science of Ukraine, Kyïv-28, Ukraine
(Received 2 March 1992, accepted in final form 16 July 1992)
Abstract
A nematic layer with opposite boundary conditions (unidirectional planar and homeotropic) is considered, having strong anchoring
at the planar wall. It is known that a periodic deformation of splay-type can intervene between the aperiodic hybrid alignment
and undistorted planar state as one decreases the film thickness. This periodic state occurs due to the fact that the energetic
cost for a mixed twist-splay can be lower than the surface energetic cost at the homeotropic wall in the case of undistorted
planar alignment. Such a situation may also be achieved for nematics which have a bulk elastic isotropy. In this paper, the
saddle-splay elastic constant
K24 is shown to influence strongly the occurrence of the periodic pattern of splay-type, also in the presence of an external
magnetic field normal to the cell plates, and the role of the geometrical anchoring in wedge-shaped cells is discussed.
61.30 - 61.30G - 68.10C
© Les Editions de Physique 1992