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Modern Polymer Spect..

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1'<br />

1656<br />

1661<br />

1669<br />

1679<br />

I I I I I I I I I 1 1788<br />

BE 1650 1608<br />

Wavenumber, u,<br />

Figure 1-26. An asynchronous ZD IR spectrum in the amide I vibration region of a film made of<br />

solubilized human hair keratin 1441.<br />

1.6 Further Extension of 2D Correlation Technique<br />

The basic concept of 2D IR spectroscopy based on the correlation analysis of<br />

perturbation-induced time-dependent fluctuations of IR intensities could be readily<br />

extended to other areas of polymers spectroscopy. The 2D correlation analysis has<br />

been successfully applied to the time-dependent variations of small angle X-ray<br />

scattering intensity measurement [4]. In this study, a small amplitude dynamic<br />

strain is applied a sheet of microphase-separated styrene-butadiene-styrene triblock<br />

copolymer sample. Intensity variation of scattered X-ray beam due to the<br />

strain-induced changes in the interdomain Bragg distances coupled with the reorientation<br />

of microdomain structures is analyzed by using the 2D correlation map.<br />

Similarly, the formal approach of 2D correlation analysis to time-dependent spectral<br />

intensity fluctuations has been extended to UV, Raman [63), and near-IR<br />

spectroscopy (641. There seems no intrinsic limitation to the application of this<br />

versatile technique in polymer spectroscopy.<br />

The introduction of the generalized 2D correlation method [8] has made it possible<br />

to further extend the utility of 2D correlation analysis beyond the study of<br />

simple sinusoidally varying dynamic spectral signals as originally described in Eqs.<br />

(1-2) and (1-3). By utilizing the time-domain Fourier transform of spectral intensity<br />

variations, a formal definition of 2D correlation spectra resembling Eq. (1-9) can be

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