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Antiferroelectric liquid crystal alignment

Thermal polarized light microscopy of liquid crystal systems still primarily involves the identification of phase types. Recently, however, a number of novel phases with complex structures have been discovered and detailed examinations of the configurations of their defects are required in order to provide a basis for future phase classification. Thermal microscopy is also used extensively in examination of the alignment processes of liquid crystals, and, in a related context, electric-field studies on meso-phases are carried out in aligned cells. Electric-field studies are now used as adjuncts to phase classification, e.g., antiferroelectric phases are sometimes identified in the microscope with the aid of electric-field studies. [Pg.3106]

Figure 9.30. Polar plots of the absorbances of the phenyl ring (1605 cm ) stretching mode versus the polarizer rotation angle in a homogeneously aligned liquid crystal cell (a) SmA (b) SmX without applied field (c) SmX with F = +5 V/pm and (d) antiferroelectric without applied field [92]. Figure 9.30. Polar plots of the absorbances of the phenyl ring (1605 cm ) stretching mode versus the polarizer rotation angle in a homogeneously aligned liquid crystal cell (a) SmA (b) SmX without applied field (c) SmX with F = +5 V/pm and (d) antiferroelectric without applied field [92].
Liquid crystal molecules usually tilt in the same direction over the smectic layers (synclinic [212]) in the smectic C (SmC) phase. However, in one of the smectic A (SmA) phases, called de-Vries phase [213,214], molecules tilt but the tile direction is random so that the overall molecular tilt cannot be recognized optically. Frustration can be produced between aligning and random orders [215]. There is another style of tilt, in which the tilting direction is aligning in one direction in each smectic layer however, tilting direction alternates between the adjacent layers (anticlinic [212]). It has been well known that the introduction of chirality into the synclinic and anticlinic stmctures produces the ferroelectric and antiferroelectric properties, respectively. Frustration between the ferroelectric and antiferroelectric properties produces the ferroelectric structure in which the spontaneous polarization is partially canceled by the different magnitude between plus and minus polarization directions [216, 217]. The anticlinic order, NOT the antiferroelectric order, has been reported to be created by achiral systems [218, 219], indicating that the frustration between synclinic and anticlinic structures occurs, without any polar effects. The clinicity is determined by the style of the molecular order between the adjacent smectic layers, and therefore, the molecular structures at the peripheral... [Pg.293]


See other pages where Antiferroelectric liquid crystal alignment is mentioned: [Pg.155]    [Pg.19]    [Pg.256]    [Pg.317]    [Pg.396]    [Pg.410]    [Pg.491]    [Pg.524]    [Pg.63]    [Pg.252]    [Pg.222]   


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