Magnetic field induced resonance Ramdn circular intensity differentId spectra arc rcportcd for the two argon ian 1~s~ wavelengths (514.5 and 501.7 nm) that fall withm the p electronic absorption band of fcrrocytochrome c. The Ggna and magnitudes of the effects arc completely different in the t&o set
Magnetic resonance-Raman optical activity of ferrocytochrome c theory and experiment
โ Scribed by L. D. Barron; C. Meehan; J. Vrbancich
- Publisher
- John Wiley and Sons
- Year
- 1982
- Tongue
- English
- Weight
- 959 KB
- Volume
- 12
- Category
- Article
- ISSN
- 0377-0486
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โฆ Synopsis
Abstract
The theory of magnetic resonance Raman optical activity in metal porphyrins is developed. Irreducible tensor methods are used to calculate the transition polarizabilities (involving both symmetric and antisymmetric contributions) which are formulated in terms of a vibronic development of the Raman transition tensors. The circular intensity difference for the vibrations of symmetry species A~1~, A~2~, B~1~ and B~2~ is explicitly evaluated for excitation within the 0โ0 and 0โ1 visible absorption bands. Polarized, depolarized and unpolarized magnetic resonance Raman optical activity spectra of ferrocytochrome c within the 0โ0 and 0โ1 bands are presented. Good qualitative agreement is found between theory and experiment.
๐ SIMILAR VOLUMES
M~gnc~c optic31 xtwity in resonance Raman spuctra of IrB$ are reported. Couplets are observed In alI three Ramsn fundamentals (Alg, Eg and Tzg) at 514.5 nm, but only m i%lg 31577.5 nm.Thcsc ongm~~c m ~nnnuons bcrwxn Zerman levels of the Knmersdcpeneratc ground SIUC. From the absolurc sifn in the AQ
The molecular theory of the scattering of polarized light is applied to the problem of the artefacts that frequently arise in Raman circular intensity difference measurements. By including the effect of the finite solid angle in the cone of collected light, a detailed understanding of the major sour
## Abstract An apparatus is described for measuring Raman backscattering with both linearly and circularly polarized light. All four polarization components, parallel, perpendicular, corotating and contrarotating, can be directly compared and used to determine the relative magnitudes of the three i