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Smectic-A edge dislocations in a very thin cell
Authors:M Ambro?i?  S Kralj  S ?umer
Institution:(1) Condensed Matter Physics Department, Jožef Stefan Institute, Jamova 39, 1000 Ljubljana, Slovenia, SI;(2) Laboratory of Physics of Complex Systems, Faculty of Education, University of Maribor, Koroška 160, 2000 Maribor, Slovenia, SI;(3) Department of Physics, Faculty of Mathematics and Physics, University of Ljubljana, Jadranska 19, 1000 Ljubljana, Slovenia, SI
Abstract:We study stable “bookshelf” smectic-A structures within a very thin plane-parallel cell of thickness L in which the mismatch between surface preferred (d s) and intrinsic (d0) smectic layer thicknesses occurs. The Landau-Ginzburg approach based on a complex smectic order parameter is used. For a weak enough smectic positional anchoring strength W smectic layers adopt the modified bookshelf profile. In a thick enough cell with increasing W a lattice of edge dislocations is continuously formed at the confining surfaces and then depinned from them. The structure with dislocations is formed when the condition d 0/( d 0/d s - 1) ∼ 2 is fulfilled, where is the positional surface anchoring extrapolation length. If the cell is thin enough the dislocations formed at opposite cell plates annihilate and consequently the smectic layers adopt a locked bookshelf structure. This transition is discontinuous and takes place when d 0/(L d 0/d s - 1) ∼ 5 is realized. To observe these transitions in a cell of thickness L∼ 1μm the conditions W∼ 10-6 J/m 2 and d 0/d s - 1∼ 5 . 10-4 have to be fulfilled. All the three qualitatively different structures coexist at the triple point. Received 21 February 2002
Keywords:PACS  61  30  -v Liquid crystals –  61  30  Jf Defects in liquid crystals –  61  72  Bb Theories and models of crystal defects
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