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Modern Polymer Spect..

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70 2 Segrnentrrl Mobility of Liquid Crystals and Liquirl-Ci.vstalliiit1 Po1jwiei.r<br />

r-<br />

-45 % -47 70 -8 %<br />

- [ .I-[ 7- f - .}<br />

4H2 41<br />

C=O<br />

c=o<br />

I<br />

?.<br />

H 3C-FH<br />

C=O<br />

I<br />

9<br />

CH2 -CH3<br />

chiral mesogen<br />

phase transition<br />

main chain + mesogen<br />

copolymer<br />

98<br />

(- 8”h) Figure 2-39. Chemical structure, coiiiposition<br />

and phase-transition temperatures of the<br />

different investigated copolymers.<br />

+ ChreNphore n<br />

introduction of chromophores with extended n-conjugation it was attempted to<br />

combine the ferroelectric properties of the mesomorphic phase with the NLOproperties<br />

of the chromophore. The synthesis has been described in detail 11061, and<br />

Figure 2-39 shows the structure and composition of the investigated homopolymer<br />

(containing no chromophore) and the modified copolymers alongside their corresponding<br />

phase-transition temperatures.<br />

2.7.1.2 Experimental<br />

Oriented polymeric films were obtained in a mechanical force field by applying<br />

a shear stress. The NaCl plates used as sample supports were coated with a thin<br />

polyiinide layer to improve the surface properties. The shearing process along a<br />

defined direction was first performed in the isotropic state above the clearing temperature<br />

and then at the isotropic/SmC*-transition. Afterwards, the temperature<br />

was gradually decreased to room temperature. The mechanical process was simultaneously<br />

analyzed using polarization optical microscopy. The experimental set-up<br />

is shown in Figure 2-40. For the subsequent dichroic measurements the samples<br />

were mounted in the spectrometer so that the shearing direction and the polarization<br />

direction of the incoming radiation were initially parallel. By rotating the

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