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    • 7. 发明授权
    • Liquid crystal light modulation device and liquid crystal light
modulation apparatus
    • 液晶光调制装置及液晶光调制装置
    • US5061045A
    • 1991-10-29
    • US398541
    • 1989-08-25
    • Makoto YoneyaKatsumi KondoTetsuya OhashiMotomi OdamuraTeruo Kitamura
    • Makoto YoneyaKatsumi KondoTetsuya OhashiMotomi OdamuraTeruo Kitamura
    • G02F1/133C09K19/46G02F1/1337G02F1/137G02F1/141
    • C09K19/46G02F1/141
    • The present invention provides a liquid crystal light modulation device which has a cell comprising a pair of substrates at least one of which is transparent and which have electrodes and are opposed through a spacer, a ferroelectric liquid crystal layer which is enclosed in said cell and which has a phase series where a nematic phase (N*phase) or an isotropic phase (I phase) is shown on a just higher temperature side of a ferroelectric phase (smectic C* phase, Sc* phase) and two polarizing plates which sandwich the cell therebetween, liquid crystal molecules at one interface between the liquid crystal layer and the substrate being fixed to the substrate more weakly than liquid crystal molecules at the other interface between the liquid crystal and the substrate wherein the liquid crystal molecule weakly fixed is fixed to such an extent that inversion of spontaneous polarization of the liquid crystal molecule occurs upon application of an electrical field to the liquid crystal layer through the electrodes, orientation of the liquid crystal molecule at one interface and orientation of the liquid crystal molecule at the other interface can be either the state (a) of being nearly parallel to each other or the state (b) of crossing each other by the inversion of the spontaneous polarization and the two polarizing plates are arranged so that light transmittance is lower at the state (a) than at the state (b).
    • 本发明提供了一种液晶光调制装置,其具有包括一对基板的单元,其中至少一个基板是透明的并且具有电极并且通过间隔件相对,被包围在所述单元中的铁电液晶层和 具有列相(N *相)或各向同性相(I相)在铁电相(近晶C *相,Sc *相)的较高温度侧的相序,以及夹着 液晶层与基板之间的界面处的液晶分子固定在基板上的液晶分子与液晶分子弱固定的液晶分子之间的液晶分子比液晶分子弱, 在向液晶层施加电场时发生液晶分子的自发极化的反转的程度 使电极粗糙化,液晶分子在一个界面的取向和液晶分子在另一界面的取向可以是相互平行的状态(a)或相互交叉的状态(b) 自发极化的反转和两个偏振片的布置使得在状态(a)下的透光率比在状态(b)下更低。