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Band assignments Fermi resonance

From an energetic point of view, the bands at higher wavenumbers can be assigned to the Ss rings. However, the intensities were found as ca. 0.65 1 (pure infected) instead of 2.8 1 which would be expected from the natural abundance of the isotopomers. These discrepancies were solved by applying the mathematical formalism utilized in the treatment of intramolecular Fermi resonance (see, e.g., [132]). Accordingly, in the natural crystal we have to deal with vibrational coupling between isotopomers in the primitive cell of the crystal [109]. [Pg.61]

In. a number of cases sub-maxima associated with vXH bands have been interpreted in this fashion and in the case of the carboxylic acid dimers this question has been investigated in some detail [4]. A prominent satellite band accompanying the main vOH bands has been assigned to an overtone of the <5QH vibration, and it has been possible to explain formally most of the multiplicity of peaks in the rOH band of formic acid in Fermi resonance terms. Although it is possible that some of these peaks correspond to Stepanov-type sub-bands, no convincing series of this type can be picked out. There seems little doubt that in many cases a considerable number of sub-bands in the rXH region are to be interpreted in terms of Fermi resonance [5, 43,... [Pg.96]

The fundamental vibrations have been assigned for the M-H-M backbone of HM COho, M = Cr, Mo, and W. When it is observable, the asymmetric M-H-M stretch occurs around 1700 cm-1 in low temperature ir spectra. One or possibly two deformation modes occur around 850 cm l in conjunction with overtones that are enhanced in intensity by Fermi resonance. The symmetric stretch, which involves predominantly metal motion, is expected below 150 cm l. For the molybdenum and tungsten compounds, this band is obscured by other low frequency features. Vibrational spectroscopic evidence is presented for a bent Cr-H-Cr array in [PPN][(OC)5Cr-H-Cr(CO)5], This structural inference is a good example of the way in which vibrational data can supplement diffraction data in the structural analysis of disordered systems. Implications of the bent Cr-H-Cr array are discussed in terms of a simple bonding model which involves a balance between nuclear repulsion, M-M overlap, and M-H overlap. The literature on M-H -M frequencies is summarized. [Pg.239]

A comprehensive publication by Heise et al. (1981) demonstrates the value of medium resolution work for the assignment of fundamentals of a larger, nine-atom molecule like CH3CH2CN and its isotopic species. In this case, complete consideration of combination bands is of great assistance. In order to calculate a valence force field, the wavenumbers of the fundamentals have, as in most cases, not been corrected for anharmonicities and evident Fermi resonance effects. This gains an added degree of complexity as the molecular size increases. [Pg.276]

All of the preceding discussions have dealt with bands that are associated with the excitation of individual normal modes, i.e., the fundamental frequencies. Although only such transitions are permitted for a harmonic oscillator, the vibrations of real molecules are anharmonic, and in such cases double excitations of a normal mode (resulting in overtone bands) and single excitations of two different normal modes (resulting in combination bands) are allowed. Analysis of such bands often leads to information on the assignments of the fundamentals, and is therefore of importance. In this connection, we need to know not only the rules for the appearance of such bands, but we must understand that they often are perturbed by an interaction known as Fermi resonance. [Pg.228]

Every chemical compound has its own characteristic IR spectrum. The IR spectrum contains the entire information about the molecular structure of the investigated sample. The main problem is the assignment of experimental spectral bands. In addition to fundamental vibration bands, very often so-called combination and overtone bands are present. Fermi resonance can cause intensity changes and frequency shifts of the bands involved. Intermolecular interactions (such as hydrogen bonding) can cause additional bands. Furthermore, the influences of solvents, tern-... [Pg.98]


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Assigning resonances

Band assignments

Fermi resonance

Resonance assignment

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