Nonadiabatic radiative lifetimes and fluorescence spectra of NO2

Citation
F. Santoro et C. Petrongolo, Nonadiabatic radiative lifetimes and fluorescence spectra of NO2, J CHEM PHYS, 111(21), 1999, pp. 9651-9657
Citations number
27
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
JOURNAL OF CHEMICAL PHYSICS
ISSN journal
00219606 → ACNP
Volume
111
Issue
21
Year of publication
1999
Pages
9651 - 9657
Database
ISI
SICI code
0021-9606(199912)111:21<9651:NRLAFS>2.0.ZU;2-H
Abstract
We have computed the radiative lifetimes and fluorescence spectra of the B- 2 nonadiabatic states of NO2 up to 18 735 cm(-1), employing ab initio MRD-C I potentials refined with respect to the experimental lines up to 10 000 cm (-1). The effects of the conical intersection (X) over tilde(2)A'/(A) over tilde(2)A' between the first two adiabatic surfaces on the radiative lifeti mes have been investigated by comparing the lifetimes of the nonadiabatic s tates with those of vibrational states of the excited electronic species. B y this way we have confirmed that the anomalous long lifetimes observed for NO2 are caused by the nonadiabatic couplings, suggesting furthermore that the lifetimes of some weak absorbing states are on the contrary lowered by the conical intersection. We have compared our lifetimes with the published experimental measurements, showing that we are able to well reproduce and explain the general experimental trends and that the computed results agree with the experimental ones within a factor two or three. These differences are similar to those found among the observed lifetimes. Moreover, we have computed laser induced fluorescence spectra and compared them with the exp erimental ones, showing a fair agreement in the low-energy range 11 600-13 900 cm(-1) and a rough agreement in the high-energy range 16 000-18 735 cm( -1), and suggesting the assignments for the main 1(2)B(2) characters of som e strongest bands. Finally, we have computed dispersed fluorescence spectra for some initial states, by pointing out that they can be very different b ecause of the difference of the wave functions of the initial states. (C) 1 999 American Institute of Physics. [S0021-9606(99)30541-9].