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2.7 Orientation oj Liquid Ci:i,stals Under Mechanicul Forces 69<br />

a<br />

b<br />

solid symbol 1st writing cycle, open symbol 6th wntlng cycle<br />

1 ' 1 9 I , I I I ' I<br />

0 200 400 600 800 1000 30 35 40 45 50 55 60 65 70 75 80<br />

Irradiation time Is Temperature I "C<br />

Figure 2-38. Reversibility of repeated write/erase-cycles demonstrated in time-resolved FTIR<br />

polarization measurements by the order parameter for the different segments of PSal?: (a) As a<br />

function of irradiation time (488 nm line of an argon-ion laser, at 30"C, SOOmW/cm') in the 1st<br />

and 6th cycle; and (b) Versus temperature during thermal erasure with a heating rate of 30 "C/niin.<br />

2.7.1 Shear-Induced Orientation in Side-Chain Liquid-Crystalline<br />

Copolysiloxanes<br />

As pointed out already in Section 2.5.5, low-molecular weight ferroelectric liquid<br />

crystals (FLCs) and FLCPs are attracting a lot of interest because of their potential<br />

for electro-optical applications. The polymers offer new possibilities, e.g., as elastomers<br />

for piezoelectric elements or by copolymerization [77, 78, 1051 due to the<br />

formation of intrinsic mixtures between SniCY' mesogenic units and other coinonomers.<br />

This leads to FLCPs combining several material properties which might be<br />

utilized for colored displays in the case of comonomers containing chi-omophores.<br />

For the differentiated evaluation of such copolymers with reference to the possible<br />

exploitation of nonlinear optical (NLO) properties, the interplay of the different orientation<br />

tendencies of the side-chain functionalities is of crucial importance [36, 1061.<br />

2.7.1.1 Materials<br />

The copolymers presented here are copolysiloxanes whose liquid-crystalline phase<br />

behavior is characterized by the formation of a SmC* phase. By the additional

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