It is sho)vn that the changes in the non-mdiativc decay rate of dilute aromatic vapors, following excitation of higher-lying singlet states, can be related to the dependence of vibrational level distribution (in St) upon the initially excited singlet states. The excitation energy dependence of radia
Energy dependence of radiative rates in isolated molecules
โ Scribed by G.R. Fleming; O.L.J. Gijzeman; S.H. Lin
- Publisher
- Elsevier Science
- Year
- 1973
- Tongue
- English
- Weight
- 386 KB
- Volume
- 21
- Category
- Article
- ISSN
- 0009-2614
No coin nor oath required. For personal study only.
๐ SIMILAR VOLUMES
A thermodynamic Green's function technique is successfully applied to the calculation of IVR rates of polyatonfic molecul, The energy dependence of IVR rates has interesting threshold features: rates are zero below some critical energy Ec, aJ non-zero for higher energies. This dependence can be unde
A method for determination of rates of non radiative energy transfer in assemblies of identicai tluorophorcs, ic described. The method is npplic;lble to systems in which migration of energy by twnst'er is much f'astrr than by difcusion. rcgardlcss of the mechanism of transfer or the type ot' order i
Absolute rate constants for radiative and for nonradiative decay from three single vibronic levels of isolated 1B2u benzene molecules are derived from experimental data. Both rate constants show sensitivity to the' vibrational state of the excited molecule. Their correspondence with the theory of vi
A theory of intramolecular non-radiative transitions is proposed for gaseous small molecules. The theory explains three experimental features: the linearity of the Stern-Volmer equation, the Douglas effect, and the fact that the non-radiative rate is faster in a gas than in condensed media.
The radiative decay rates of the 3rr,\* states of coumarin, piperonal and 4-methoxybenzaldehyde were determined at the O-O, and different vibronic bands involving both totally and non-totally symmetric vibrations. The emission from the z and x sublevels is primarily due to the mixing of the 3nrr\*