Of. Nielsen et al., USE OF ISOTOPE EFFECTS IN STUDIES OF INTERMOLECULAR INTERACTIONS BY RAMAN-SPECTROSCOPY, Journal of molecular structure, 378(1), 1996, pp. 1-9
A very brief introduction to vibrational spectroscopy is given with a
particular emphasis on the effect of isotopic substitution. A few key
references to studies of both the gaseous and the crystalline states a
re cited. Intermolecular interactions in liquids are studied by (i) Re
sonance Energy Transfer giving rise to a non-coincidence effect betwee
n the anisotropic and the isotropic Raman components, (ii) Coalescence
of Bands in Mixtures of Isotopomers, giving rise to an observation of
fewer bands than expected from a simple addition of bands from the in
dividual isotopomers in the mixture, and finally (iii) low-frequency R
aman spectroscopy, for which the R(<(nu)over bar>) representation is u
sed in order to get rid of the intense Rayleigh line appearing in the
Raman spectra of liquids. Experimental data include results for isotop
ically substituted liquid formamides and a solution of HCOND2 in D2O.
The results show that intermolecular interactions via transfer of vibr
ational energy occur for the carbonyl stretching vibration at around 1
650 cm(-1) (amide-I band). A band in the low-frequency spectrum at aro
und 100 cm(-1) is assigned to a mode involving displacements of atoms
in the intermolecular hydrogen bonds. Similar interactions might be of
importance for the fast dynamics of biological macromolecules like pr
oteins and nucleic acids.