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Figure 2-12. Stack-plot of spectra measured during the electric field-induced orirnration and duriiip<br />

part of the relaxation of thc 6CPB molecules (41 -C'.<br />

Figure 2-13. Relative absorbance/time-plot during orientation and relaxation of 6CPB (41 C!<br />

for selected absorption bands: (0) 2929 cni-'. (7) 2858 cm-', (012230 cin-l. I + ) 1605 cm-'. I x<br />

1503 cm-'. (+) 757 cni.~'.<br />

approximately 1.5 Vpp. In the homeotropic type of orientation, the long axis of the<br />

LC molecule is normal to the electrode surface and parallel to the IR beam propagation.<br />

According to geometrical considerations [62] a reorientation to this honieotropic<br />

state thus leads to intensity changes of the Ail-component only. This component<br />

asymptotically approaches the Al intensity value at sufficiently high fields.<br />

For this reason, all time-resolved measurements have been performed with light<br />

polarized parallel to the polyimide-layer rubbing direction.<br />

A stack-plot of time-resolved spectra recorded during the honiogeneous-homeotropic<br />

transition and part of the relaxation process is presented in Figure 2-12. A<br />

good signal-to-noise-ratio is observed for all spectral regions (except when the<br />

absorbance exceeds a value of 2). Relative absorbance changes A, for selected<br />

absorption bands were calculated from:<br />

where A, is the absorbance at time t and A0 is the absorbance just before reorientation.<br />

These relative intensity changes of selected absorption bands are presented<br />

in Figure 2-13 and remarkable changes are observed only after a definite induction

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