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Modern Polymer Spect..

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-3.6 Aligmient OJ' Side- Clinin Liyuicl- Cv!~stnlline Poljwstevs 61<br />

161<br />

WAVENUMBER I cmd<br />

14 -<br />

12 -<br />

10 -<br />

c<br />

c<br />

zi<br />

(0 8-<br />

6-<br />

Figure 2-29. Comparison of the reference (top)<br />

and power (bottom) spectra intensities of the<br />

FLCP for the reorientation process during<br />

poling the external electric field.<br />

4r<br />

1500 2000 2500 3000<br />

WAVENUMBER /at-'<br />

Figure 2-30. Schematic representation of the<br />

segmental motions of the FLCP during poling<br />

the electric field.<br />

POLARITY SWITCH<br />

RESPONSE<br />

of novel SCLC-polyesters [ 151 are presented. In unoriented polyester films with a<br />

dodecamethylene spacing of the ester groups in the main chain, holograms with a<br />

resolution of 6000 linesjmm can be recorded by the interference of an Argon-ion<br />

laser beam [95]. The thermal erasure and rewriting of the laser-induced alignment in<br />

the SCLC polyesters is the basis for such storage processes. In order to investigate<br />

the mechanism of the involved processes in more detail, a variable-temperature,<br />

computer-controlled sampling system for on-line polarization FTIR nieasurements<br />

during laser irradiation as well as thermal erasure has been designed and<br />

constructed.

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