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Spatially periodic structures in nematic liquid crystals usually appear as the initial response to a suddenly applied reorienting field. To account for the significant discrepancy between the measured periodicity and the periodicity calculated from a linear instability analysis we derived nonlinear equations of motion and solved them numerically. Our results agree well with the observed wavelength. We propose a novel mechanism responsible for the final wavelength selection.
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Srajer et al. (1989) studied this question.
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