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mail1 chain<br />

Figure 2-1. Schematic structure of a side-chain liquid-crystalline<br />

polymer.<br />

. orientation mechanism of a liquid single crystal elastomer during cyclic deformation<br />

and recovery.<br />

Static and time-resolved spectroscopic data acquired both, by the conventional<br />

rapid-scan and by the novel step-scan technique will be presented and interpreted in<br />

terms of their individual applications.<br />

2.2 Measurement Techniques and Instrumentation<br />

Since the mid-l970s, FTIR spectroscopy has been widely used for polymer analytical<br />

applications and for studies of time-dependent phenomena in chemical and<br />

physical processes [ 141. With the current iinproveinent in electronics and data<br />

acquisition procedures, the time resolution for such investigations with an acceptable<br />

signal/noise-ratio is presently about 20 111s. Time resolutions far beyond this<br />

value are not accessible by the conventional rapid-scan technique with continuous<br />

mirror moveinelit without additional interferogram data manipulation. Thus, for<br />

time-resolved, rapid-scan measurements, generally, the retardation time of the<br />

moving mirror has to be considerably shorter than the time duration of the investigated<br />

event (Figure 2-2a). In search of new approaches, stroboscopic techniques<br />

have been proposed, where interferograms taken in the rapid-scan mode are subsequently<br />

subjected to a sampling of reordered interferograin segments and have<br />

thus led to an improvement in time resolution by a factor of about 500 [24, 251.<br />

A further improvement in time resolution to the submicrosecond level has been<br />

achieved with the step-scan technique 116, 26, 271. Here, the mirror is moved stepwise<br />

and the optical retardation is held constant during sampling of the individual<br />

interferogram elements. Thus, the time resolution is only limited by the response of

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