2024 Impact factor 2.2
Soft Matter and Biological Physics
\n This email address is being protected from spambots. You need JavaScript enabled to view it. ), CBLU, University of Leeds * revised and updated by: Marcus Hennecke, Ross Moore, Herb Swan * with significant contributions from: Jens Lippmann, Marek Rouchal, Martin Wilck and others --> Eur. Phys. J. E 2, 47-57

Grain boundaries and the law of corresponding cones in smectics

M. Kléman1 - O.D. Lavrentovich2

1 Laboratoire de Minéralogie-Cristallographie (UMR 7590), Universités de Paris-VI & de Paris-VII, Case 115; 4 place Jussieu 75252 Paris cédex 05, France
2 Chemical Physics Interdisciplinary Program and Liquid Crystal Institute, Kent State University, Kent, Ohio 44242, USA
This email address is being protected from spambots. You need JavaScript enabled to view it.

Received 21 June 1999 and Received in final form 10 September 1999

Abstract
Focal Conic Domains (FCDs) in smectic phases often assemble according to a particular rule, experimentally discovered by G. Friedel, the law of corresponding cones (l.c.c.). This paper reports various results relating to this type of association. First we show that a l.c.c. contact between 2 focal conic domains has a vanishing energy, yielding metastable local equilibrium. Then we use some projective properties of conic sections to extend the celebrated Apollonian tiling, which describes a tilt grain boundary (TiGB) of vanishing disorientation $\omega=0$ made of toric focal conic domains, to any $\omega\not=0$ TiGB. Finally we present a realistic model of the energy of the $\omega\not=0$ TiGB, which we compare to the energy of a TiGB split into dislocations, and to the energy of a curvature wall. This model explains why FCD tilings show macroscopic zones not filled with FCDs.

PACS
61.30.Jf Defects in liquid crystals - 61.72.Lk Linear defects: dislocation disclinations - 61.72.Mm Grain and twin boundaries

Copyright EDP Sciences, Società Italiana di Fisica, Springer-Verlag