Thin nematic film on isotropic surface:
1-Dimensional periodicity

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The periodic stripe structure is a spectacular consequence of the confined nature of the film. It is a result of the competition between elastic inner forces and surface anchoring forces. The surface anchoring forces want to align the liquid crystals parallel to the bottom surface and perpendicular to the top surface of the film. The elastic forces work against the resulting "vertical" distortions of the director field. When the film is sufficiently thin, the lowest energy state is surprisingly achived by "horizontal" director deformations in the plane of the film. The current picture shows a 1-dimensional periodic pattern; 2-dimensional periodic patterns can also be observed (click on link below for next picture). Both periodic phases have similar energies such that they can coexist, as shown in the picture http://www.lci.kent.edu/deflat2.html.

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