Fw. Langkilde et al., MOLECULAR-STRUCTURE OF STILBENE IN THE T-1 STATE - TRANSIENT RESONANCE RAMAN-SPECTRA OF STILBENE ISOTOPOMERS AND QUANTUM-CHEMICAL CALCULATIONS, Journal of physical chemistry, 98(9), 1994, pp. 2254-2265
Time-resolved resonance Raman spectra are reported for the lowest exci
ted triplet state of stilbene and three of its isotopomers. The-spectr
a were obtained using a two-laser pump-and-probe arrangement under var
ious experimental conditions. The spectrum of trans-stilbene after dir
ect excitation in a glassy medium at low temperature (glycerol at 203
K) is compared with that of cis-stilbene under sensitized excitation i
n solution at room and low temperature. The dependence of resonance Ra
man spectra on excitation wavelength in both cases is investigated. Th
e observed spectra and isotopic shifts are discussed and interpreted o
n the basis of quantum chemical molecular orbital calculations. Optimi
zed geometries and vibrational frequencies in the T-1 state are calcul
ated by a semiempirical QCFF/PI Hamiltonian and by means of ROHF ab in
itio methods using the 6-31G basis set. T-1 -> T-n transition energies
and moments are calculated using QCFF/PI and CNDO/S methods, and the
triplet-triplet transition responsible for the observed T-1 -> T-n abs
orption and resonance Raman spectra is identified as the T-1 -> T-10 t
ransition. Corresponding resonance Raman intensities are calculated by
QCFF/PI. It is concluded that trans- and cis-stilbene adopt a common
equilibrium geometry in the T-1 state, with the ethylenic C=C bond of
the ground state being weakened to a bond with essentially single-bond
character in the T-1 state. The observed spectra in the glass are ass
igned to a planar geometry, implying that a relative minimum is found
at a planar trans geometry (C-2h point group) on the potential energy
surface of the T-1 state. A number of observed non-totally symmetric v
ibrational modes are tentatively assigned to combinations of either a(
u) or b(g) modes, deriving their intensities from relatively large fre
quency changes upon T-1 -> T-10 excitation.