No abstract

The resonance coherent anti-Stokes Raman technique was used to obtain vibrational spectra of flavin in flavodoxins from Desulfovibrio gigas and Desulfovibrio vulgaris and of the simpler 6,7-dimethyl-8-ribityllumazine chromophore in the blue fluorescence lumazine protein from the bioluminescent bacterium Photobacterium phosphoreum. In the region examined, 1100-1700 cm-1, the Raman spectrum of the lumazine is less crowded than that of the flavin and this facilitates assignment of observed frequencies to particular vibrational modes. Certain modes are not affected by chromophore binding to the protein, but others are changed in frequency or intensity in a way that can be rationalized by expected interactions of the chromophore with the amino acid residues of the binding site. For example, a tentative assignment of change in hydrogen bonding at N(5) is suggested as the cause of the frequency shift for the chromophore in both flavodoxins (free-bound, 1582-1572 cm-1) and for C(4)=O in glucose oxidase (1359-1364 cm-1) and lumazine protein (1359-1362 cm-1). Shifts of the C(2)-N(3) mode in D2O may arise from hydrogen-bonding changes at C(2)=O in lumazine protein (1284-1291 cm-1), flavodoxin (1300-1280 cm-1), and glucose oxidase (1297-1287 cm-1). Bonding at N(3)-H may be the origin of changes in the frequency or intensity of the amide III mode in riboflavin binding protein and glucose oxidase. A stacking interaction is suggested for the change in a pyrimidine ring mode in FAD (1508 cm-1) since this mode is found at 1504 cm-1 in 30% Me2SO/H2O, where the adenine and pyrimidine are unstacked. The results clearly indicate different interactions in the binding sites of those proteins studied to date.

Our previously published infrared and Raman spectra of 1,3-disilacyclobutane (13DSCB) and its 1,1,3,3-d4 isotopomer have been reexamined and partially reassigned on the basis of DFT and ab initio calculations. The calculations confirm previous microwave work that the CSiC angles in the ring are unexpectedly larger than the SiCSi angles. This may arise from the partial charges on the ring atoms. The calculations are in excellent agreement with the observed spectra in both frequency and intensity. They also demonstrate that this molecule has CH2 wagging and twisting vibrations with frequencies below 1000 cm-1, about 200 cm-1 lower than expected. These unprecedented low values can be explained by the decreased slope in the potential energy curves for these vibrations as the sideways motions of the CH2 groups result in attractive forces between the positively charged hydrogens on the carbon atoms and the negatively charged hydrogens on the silicon atoms. The theoretical calculations also confirm the previous conclusions that the individual molecules (vapor) have C2v symmetry whereas in the solid the molecules become planar with D2h symmetry. The vibrational coupling between the ring-angle bending mode and the SiH2 in-phase rocking, which is present for the C2v structure, is forbidden for D2h and hence disappears.

The term "hydrophobicity" as used in this paper refers to the sum total of all such environmental effects on fluorescence. For a more complete discussion on hydrophobicity and solvent polarity the reader is referred to the recent review of Brand and Gohlke (1972).

A detailed analysis of the vibrational spectra of 1,3-disilacyclobutane and 1,3-disilacyclobutane-l,1,3,3-d4 in vapor, liquid, and solid phases shows that the molecules have puckered ring conformations in the former two phases but become planar in the solid state. This is reflected by the frequency shifts of the ring deformation and SiH2 (or SiD2) rocking modes which are uncoupled for the planar conformation but interact strongly for the puckered structure. Frequency differences between gas and solid phases for these two modes range from 27 to 42 cirf1. Force constant calculations confirm that these shifts are due to the different amounts of vibrational mixing for different conformations in the two phases.