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Hydrodynamics of polar liquid crystals

Abstract

Starting from a microscopic definition of an alignment vector proportional to the polarization, we discuss the hydrodynamics of polar liquid crystals with local C∞vC_{\infty v}-symmetry. The free energy for polar liquid crystals differs from that of nematic liquid crystals (D∞hD_{\infty h}) in that it contains terms violating the nβ†’βˆ’n{\bf{n}}\to -{\bf{n}} symmetry. First we show that these Z2\mathcal{Z}_2-odd terms induce a general splay instability of a uniform polarized state in a range of parameters. Next we use the general Poisson-bracket formalism to derive the hydrodynamic equations of the system in the polarized state. The structure of the linear hydrodynamic modes confirms the existence of the splay instability.Comment: 9 pages, corrected typos, added references, revised content, to appear in PR

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    Last time updated on 01/04/2019