“…It has been known since 1973 that a thin film of nematic liquid crystal (NLC ), when placed upon a ferroelectric crystal, is able to delineate the domain structure of the underlying crystal substrate. [1][2][3][4][5][6][7][8][9][10] This phenomenon was first demonstrated by Furuhata and Toriyama for the ferroelectric crystal triglycine sulfate (TGS ) and the NLC p-N-( p-methoxybenzylidene)amino-n-butylbenzene.1 They proposed a model whereby the spontaneous polarisation of a ferroelectric domain couples Bi 2 Br 11 .7 More the direct surface interactions. Further, the well defined device recently the coupling mechanism between the domains of geometry allows the interaction of the NLC layer with the ferroelectric crystals with NLC has been described in terms of OFE to be quantified, as will be discussed.…”
The technique of domain visualisation, revealed by a film of nematic liquid crystal (NLC ) on a ferroelectric crystal substrate, is demonstrated for the first time to be applicable to thin films of lead zirconate-lead titanate (PZT ) ferroelectric ceramics. PZT film thicknesses <1 mm were deposited on indium tin oxide coated glass substrates. Commercially available NLC materials with positive dielectric anisotropy were employed. The electro-optic properties of devices incorporating the ferroelectric ceramic and NLC are reported. The poled PZT grains induce a local Fre ´edericksz transition in the NLC and it is proposed that the ferroelectric-NLC interaction is primarily due to the depolarisation field due to the ferroelectric remanent polarisation.
“…It has been known since 1973 that a thin film of nematic liquid crystal (NLC ), when placed upon a ferroelectric crystal, is able to delineate the domain structure of the underlying crystal substrate. [1][2][3][4][5][6][7][8][9][10] This phenomenon was first demonstrated by Furuhata and Toriyama for the ferroelectric crystal triglycine sulfate (TGS ) and the NLC p-N-( p-methoxybenzylidene)amino-n-butylbenzene.1 They proposed a model whereby the spontaneous polarisation of a ferroelectric domain couples Bi 2 Br 11 .7 More the direct surface interactions. Further, the well defined device recently the coupling mechanism between the domains of geometry allows the interaction of the NLC layer with the ferroelectric crystals with NLC has been described in terms of OFE to be quantified, as will be discussed.…”
The technique of domain visualisation, revealed by a film of nematic liquid crystal (NLC ) on a ferroelectric crystal substrate, is demonstrated for the first time to be applicable to thin films of lead zirconate-lead titanate (PZT ) ferroelectric ceramics. PZT film thicknesses <1 mm were deposited on indium tin oxide coated glass substrates. Commercially available NLC materials with positive dielectric anisotropy were employed. The electro-optic properties of devices incorporating the ferroelectric ceramic and NLC are reported. The poled PZT grains induce a local Fre ´edericksz transition in the NLC and it is proposed that the ferroelectric-NLC interaction is primarily due to the depolarisation field due to the ferroelectric remanent polarisation.
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