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40 2 Segnwital Mobility of Liquid Crystuls aid Liquidcrystalline Polymevs<br />

6CPe<br />

0<br />

C H 3 - ( C H z ) e C - O D C = N<br />

5<br />

44.5°C 48.5OC<br />

K - N - I<br />

NLCP<br />

- 0<br />

2, H -&-O-(CHZ)~$$C O a C - N<br />

-.<br />

CH2<br />

-n 3S°C 130°C<br />

G - N - I<br />

Figure 2-6. Sti ucture aiid transition temperatures<br />

of the investigated low- aiid highmolecular<br />

weight LC systems I6CPB and<br />

NLCP).<br />

polymers and liquid-crystalline guest-host system) in switch-on/switch-off experiments,<br />

and on the other hand we will describe the structural consequences incurred<br />

by a ferroelectric side-chain polymer in a poled electric field.<br />

Nematic liquid-crystalline molecules, which consist of a rigid inesogenic unit with<br />

an attached flexible part (sequence of methylene units, for example) (Figure 2-6),<br />

are among the most characteristic thermotropic systems. FTIR spectroscopy has<br />

been applied to study the mechanisiii of orientation of the liquid crystals in an<br />

electric field; however, at present the experimental data are not always unequivocal,<br />

and conclusions obtained are not in complete agreement with each other. T~us,<br />

some authors did not detect any differences in orientational rates of the rigid and<br />

the flexible part of the LC molecule [16, 51-54], which is in accordance with the<br />

commonly accepted mechanism of the orientation of an LC as a cooperative<br />

motion of a molecular ensemble [l, 2, 381. Other authors reported, that the motion<br />

of the flexible part precedes that of the inesogen in both orientation and relaxation<br />

[29, 55-57], and some investigators suggested that the motion of the mesogen precedes<br />

the motion of the flexible part [58, 591. With respect to a more detailed exploitation<br />

of the spectroscopic data in terms of the synchronization of the segmental<br />

motions of different functionalities of the investigated liquid-crystalline systems,<br />

2D-correlation analysis [ 16, 30, 60, 611 has proved an extremely valuable tool. In<br />

view of the detailed discussion of this mathematical technique in Chapter 1 of this<br />

book; however, this topic will not be treated here, although several results extracted<br />

from the presented spectroscopic data are based on the application of the 2Dcorrelation<br />

formalism.<br />

2.5.1 Materials<br />

To study the addressed phenomena, a commercial sample of p-cyanophenyl p-nhexylbenzoate<br />

(hereafter abbreviated as 6CPB) (Figure 2-6) was obtained from<br />

Roche (Basel, Switzerland), and used without further purification [53, 541. The<br />

transition temperatures of this LC are also presented in Figure 2-6. It should be<br />

mentioned, that the nematic phase will be retained during cooling down to 7 "C<br />

below the crystal-nematic transition point. To demonstrate the reduction of

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