PROBE-WAVELENGTH DEPENDENCE OF PICOSECOND TIME-RESOLVED ANTI-STOKES-RAMAN SPECTRUM OF CANTHAXANTHIN - DETERMINATION OF ENERGY-STATES OF VIBRATIONALLY EXCITED MOLECULES GENERATED VIA INTERNAL-CONVERSION FROM THE LOWEST EXCITED SINGLET-STATE
T. Nakabayashi et al., PROBE-WAVELENGTH DEPENDENCE OF PICOSECOND TIME-RESOLVED ANTI-STOKES-RAMAN SPECTRUM OF CANTHAXANTHIN - DETERMINATION OF ENERGY-STATES OF VIBRATIONALLY EXCITED MOLECULES GENERATED VIA INTERNAL-CONVERSION FROM THE LOWEST EXCITED SINGLET-STATE, The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory, 101(19), 1997, pp. 3494-3500
The vibrational relaxation process in the ground electronic state (S-0
) of canthaxanthin after internal conversion from the lowest excited e
lectronic state (S-1) to the S-0 state is studied by picosecond time-r
esolved anti-Stokes Raman spectroscopy. The pump-induced intensities o
f two strong anti-Stokes Raman bands reach their maxima at delay time
similar to 12 ps from the pump pulse, and decay with a time constant o
f 15-20 ps. The peak position of the transient ''in-phase'' C=C stretc
hing anti-Stokes Raman band shows a small shift to a lower frequency f
rom that observed in the stationary (cw) spectrum. In order to determi
ne the energy levels on which the observed vibrationally excited molec
ules are populated, the probe-wavelength dependence of the pump-induce
d anti-Stokes Raman intensities are analyzed. Most of the vibrationall
y excited transients giving rise to the transient 1520 cm(-1) band at
delay time 12 ps are on the first excited vibrational level of the C=C
stretching mode in the So state. This result suggests that the intram
olecular vibrational redistribution (IVR) process is very fast and con
tributes only to the rise part of the time dependence of the anti-Stok
es Raman intensity. The observed shift of the C=C stretching band is c
onsidered to arise from anharmonic coupling with various other vibrati
onal modes which are excited through the IVR process, rather than from
contributions of molecules on highly excited levels of the C=C stretc
hing mode generated immediately after the internal conversion from the
S-1 state.