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Electrooptics of the Twist Cell for Oblique Incidence

FIGURE 4.15. The twist cell for oblique light incidence at the angles ie, i ). The angle ie is measured from the normal to the substates, while the angle is from the symmetric plane of the twist structure. [Pg.164]

The most crucial partoieter that affects the uniformity of transmission is the Mauguin number [87]. For low And/ values the anisotropy of transmission is weak [87, 88]. According to this, liquid crystal mixtures with low An values and the first Mauguin minimum And/X = f%j2 as a working point are preferable. We do not consider the influence of the parameters ATaa/ifTii and Aef on the transmission characteristics of the twist cell, as their effect now is very small compared with the case of normal incidence [74, 95]. [Pg.164]

Let us note that coloration, i.e., dependence of the light transmission on the wavelength, and the stronger temperature dependence of 6n make the operation in the first Mauguin s minimum less attractive. Sometimes it seems more convenient to choose y/S/2 And/X a/5/2 (between the first and second minima) even at the cost of the partial loss of the contrast [95]. [Pg.164]

FIGURE 4.17. Isocontrast curves for the normally white mode [98] (twist cell between crossed polarizers in white light). The first polarizer is (a) perpendicular and (b) parallel to the director on the input substrate. [Pg.166]

4 Matrix Addressed Displays and Multiplexing Capability of Twist-Effect Materials [Pg.166]


See other pages where Electrooptics of the Twist Cell for Oblique Incidence is mentioned: [Pg.163]   


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