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There is also a recent experiment of photopolymerization-induced phase separation in a deformed liquid crystal by Volcoschenko et al.(e-print cond-mat/0109473), which revealed the accumulation of polymer droplets into regions with high elastic energy of liquid crystals. This experimental situation is different from that in this paper because we deal with a system whose elastic energy density in the absence of particles is spatially uniform
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In this form of the Frank elastic energy we implicitly set the saddle-splay elastic constant as (Formula presented) The possible effect of the saddle-splay elasticity on the equilibrium director configuration in a hybrid nematic cell is discussed by A. Sparavigna, L. Komitov, O.D. Lavrentovich, and A. Strigazzi, J. Phys. II 2, 1881 (1992).
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Since the anchoring energy of a liquid crystal with glycerol is (Formula presented) and the Frank elastic constant K is of the order (Formula presented) the weak anchoring condition (Formula presented) is satisfied for micrometer-size droplets in the experiment of Ref. 28
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Since the anchoring energy of a liquid crystal with glycerol is (Formula presented) and the Frank elastic constant K is of the order (Formula presented) the weak anchoring condition (Formula presented) is satisfied for micrometer-size droplets in the experiment of Ref. 28.
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