## I51 sive wrinkling and corrugation. A disclination model seems to apply to the core of round filaments, the transitions from round to cracked structures imply disclination interactions along the length of the filament. 236. The textile prestretching of PAN-fibres as a controlling parameter for
The lineshape of motion-averaged isotropic Raman spectra
β Scribed by A.I. Burshtein; S.G. Fedorenko; A.Yu. Pusep
- Publisher
- Elsevier Science
- Year
- 1983
- Tongue
- English
- Weight
- 337 KB
- Volume
- 100
- Category
- Article
- ISSN
- 0009-2614
No coin nor oath required. For personal study only.
β¦ Synopsis
The conventional Kubo model can be used to describe the spectrum modulation by slow to fast motion, i.e. even in the range of applicability of perturbation theory. However, the Kubo model assumes the gaussian shape of static spectra. A model free of this assumption has been used to show that experbnental data can be interpreted provided the initial static spectrum has nongaussian wings. 1_ introduction 2. Nongaussian static spectra Adiabatic perturbations of vibrational levels affect essentially the shape of vibrational spectra. These perturbations, caused by interactions of the medium molecules, lead to a random modulation of the vibrational transition frequency 6+,ib = w. + Am(t), where o. is the average transition frequency, and Am(t) is the centred random process. Lately this phenomenon was termed vibrational dephasing [I]. It is often described in terms of the stochastic theory of lineshape (the Kubo model) [Z-S], while in the case of fast modulation the perturbation theory is used [9-13]_
π SIMILAR VOLUMES
## Abstract The characteristics of the generalized Van VleckβWeisskopfβFrΓΆhlich type susceptibility (GVWF) are discussed. It is shown that the GVWF can represent both an oscillator type and a relaxational (Debye) type of phonon mode, usually adopted in the analysis of Raman spectra of soft modes in
Important motional narrowing has been previo%sIy experimentally observed by Dion and May in the isotropic Raman Q branch of pure gaseous HD in rhe fundamental vibrational band. A recent theoretical calculation of the present authors, in good agreement with these e.xperiments, has shown thar for pure