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~ polyester<br />

2.6 Alignnient qf Side-Chaiii Liquid- Crystalline Polyrsters 63<br />

film<br />

polarization direction<br />

Figure 2-32. Simplified picture of the experimental<br />

set-up for laser-irradiation and symbolic<br />

representation of the motivation for the<br />

FTIR-spectroscopic detemiinatioii of the order argon.ion laser ,R beam<br />

parameters of the polyester functionalities.<br />

(488 nin)<br />

been studied, but no obvious iinproveinent of the data storage capability 1991 could<br />

be observed.<br />

Thin film of the polyesters were obtained by casting a chloroform solution<br />

(3mg/200 pl) of the polymer onto KBr plates with a 1.5 x 1Oinm' area. After<br />

evaporation of the solvent, the films were dried at room temperature under vacuum<br />

for 2 h. The film thickness obtained by this preparation procedure was approximately<br />

5 pni.<br />

2.6.2 Experimental<br />

Figure 2-32 provides a simplified picture of a laser irradiation/FTIR measurement<br />

experiment symbolizing the inherent problem to determine the laser-induced orientation<br />

of the different polymer segments. The detailed instrumental design of the<br />

apparatus used for these on-line ineasurements is given in Figure 2-33 and shows<br />

that the following experimental parameters can be varied:<br />

0 Based on an internally calibrated photo-diode, the laser intensity can be reduced<br />

from 800 mW/cin2 in a controlled fashion with a neutral-glass filter wheel.<br />

The irradiation time is adjusted by the shutter.<br />

The temperature of the sample is controlled by a Peltier element.<br />

The acquisition of the FTIR polarization spectra is performed by using the<br />

dedicated computer of the spectrometer, which is synchronized with the different<br />

devices. The laser beam passes through the shutter and the filter wheel and is<br />

directed via two mirrors onto the film sample, which is mounted on the Peltier<br />

heater/cooler arrangement. This set-up was used to follow the photo-induced<br />

anisotropy during and after irradiation as a function of time and temperature, as<br />

well as its thermal stability during erasing cycles. Time-resolved spectra with a<br />

resolution of 4 cin-' were taken with radiation polarized alternately parallel and

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