RESONANT INTERSYSTEM CROSSING IN PENTACENE

Citation
A. Corval et al., RESONANT INTERSYSTEM CROSSING IN PENTACENE, Journal of physical chemistry, 98(30), 1994, pp. 7376-7381
Citations number
22
Categorie Soggetti
Chemistry Physical
ISSN journal
00223654
Volume
98
Issue
30
Year of publication
1994
Pages
7376 - 7381
Database
ISI
SICI code
0022-3654(1994)98:30<7376:RICIP>2.0.ZU;2-X
Abstract
Intersystem crossing (ISC) in pentacene dissolved in a single-crystal matrix of benzoic acid is shown to be dominated by near-resonant trans fer of the excitation between the pure electronic SI state and vibrati onal levels of a higher triplet state. According to CNDOM calculations the triplet state is T-3, with the same symmetry as S-1 (pi pi B-2u) . The vibrational levels are assigned to fundamentals of out-of-plane modes involving motions of the hydrogen atoms, so that large changes i n the ISC rates are observed when the vibrational frequencies are shif ted by partial deuteration of pentacene. Normal mode calculations for different isotopic species of pentacene locate the fundamental frequen cies of these out-of-plane vibrations in the range of 300-1100 cm(-1). The separation of the pure electronic S-1 and T-3 states must therefo re lie in the same range, in agreement with the CNDOM calculations. Fo r small energy separations of the singlet S-1 state and the vibronic t riplet level, crossings between them can be induced by applying a magn etic field. These level crossings produce changes of the ISC rates and , as a consequence, changes of the fluorescence emission quantum yield . Well-defined level crossing signals have been observed at 1.6 K by m onitoring the fluorescence intensity as a function of the Strength of the applied field. A quantitative analysis of these signals leads to a determination of the spin-orbit coupling matrix elements between the singlet and the triplet sublevels (in the range of 0.1 cm(-1)). The wi dth of the resonances reflects the width of the triplet vibronic level , which at 1.6 K, is aetermined by its decay time of about 1.7 ps. Whe n, at higher temperatures, pure dephasing dominates the population dec ay rates, the resonance effects are predicted to be diminished. In the experimentally accessible range of T < 15 K the onset of this evoluti on can be observed.