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Analysis of vibronic intensities in the phosphorescence spectrum of dimethylbenzaldehydes in durene
Authors:A. Després  V. Lejeune  E. Migirdicyan  C. Mijoule  G. Marconi  G. Orlandi  W. Siebrand  M.Z. Zgierski
Affiliation:Laboratoire de Photophysique Moléculaire du CNRS, Université de Paris-Sud, 91405 Orsay, France;Laboratoire de Physique Thèorique des Particules, Université de Picardie, 80039 Amiens, France;Istituto FRAE del CNR, 40126 Bologna, Italy;Istitut Chimico “G. Ciamician” dell''Università, Bologna, Italy
Abstract:An attempt is reported to explain the main intensity patterns in the phosphorescence spectra of 2,4-, 2,5- and 3,4-dimethyl-benzaldehyde-1h1 and -1d1, observed previously. The analysis is based on CNDO and MINDO calculations of (transition) dipole moments, spin-orbit couplings, vibronic couplings, state energies, normal coordinates and vibrational frequencies. Where possible these quantities are empirically checked and corrected. Additional information, especially about the separation of the closely spaced T1(3ππ*) and T2(3*) states, is obtained from phosphorescence excitation spectra reported here for all six isomers. The phosphorescence spectra consist of two components, an “allowed” component of 3ππ* and a “forbidden” component of 3* symmetry. It is concluded that the allowed component is partly induced by the crystal field. The forbidden component is vibronically induced by out-of-plane vibrations among which the aldehydic CH(CD)-wag mode is the most active. The observed intensity patterns for this component are ascribed to interference between two mechanisms, one involving vibronic coupling between S0 and S1(1*) and spin-orbit coupling between S1 and T1, the other involving vibronic coupling between T1 and T2 and spin-orbit coupling between S0 and T2. Within the groups of either 1h1 or 1d1 isomers, the main changes in the spectrum are shown to be due to the change in T1–T2 energy separation. The changes observed upon deuterium substitution in the aldehyde group involve, in addition to changes in the T1–T2 gap, changes in vibronic coupling due to normal-coordinate mixing. All these spectral changes are reproduced by calculations based on a mixture of theoretical and empirical input parameters, derived from, or at least consistent with, other observations, including excitation spectra, dipole moments and zero-field splittings. It is concluded that the mechanisms underlying these calculations offer a satisfactory explanation of the observed intensity patterns in the phosphorescence spectra of dimethylbenzaldehydes.
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