Thermalization process after the relaxation of electronically excited states: Intramolecular proton transfer systems studied by the transient gratingmethod
T. Okazaki et al., Thermalization process after the relaxation of electronically excited states: Intramolecular proton transfer systems studied by the transient gratingmethod, J CHEM PHYS, 110(23), 1999, pp. 11399-11410
Photophysical and thermalization processes after photoexcitation of 2-(2'-h
ydroxy-5'-methylphenyl)benzotriazole (HMPB) in cyclohexane and 2-hydroxyben
zophenone (HBP) in various solvents were investigated by the transient grat
ing (TG) method. From the time profiles of the population grating (PG) sign
als, two distinct kinetics were observed for HMPB and HBP. For HMPB, the fa
ster (600 fs) kinetics is attributed to the back proton transfer reaction i
n the ground state, and the faster process of HBP (400 fs) is attributed to
the vibrational cooling in the S-1 state. The slower one (similar to 30 ps
) of both compounds is assigned to the vibrational cooling in the S-0 state
. In ethanol (hydrogen bonding solvent), the PG signal originated from the
T-1 state of HBP is apparent. However, the thermal energy from the T-1 stat
e is negligibly small and the triplet quantum yield was found to be less th
an 0.05. The photoexcited HBP relaxes to the ground state by the internal c
onversion dominantly even in ethanol. The thermalization rates of these mol
ecules were measured from a point of view of the translational energy of so
lvents by the acoustic peak delay method of the TG signal. The results show
that in the early step of the thermalization, there is a very fast cooling
process (less than a few ps) which is due to the energy transfer from the
photoexcited solute to (several) effectively coupled solvent molecule(s), a
nd then the heated solvent molecule becomes cool by the thermal diffusion t
o the bulk solvents. The thermalization processes depend on both of the sol
ute and solvent properties. The time development of the temperature calcula
ted based on this thermalization model explains the experimental observatio
ns. (C) 1999 American Institute of Physics. [S0021-9606(99)00723-0].