I. Suzuki et al., Absorption spectra of C-60-excited states in various solvents: Their dependence on the ionization potential of solvent molecules, B CHEM S J, 73(3), 2000, pp. 589-598
Using a picosecond laser photolysis system, the absorption spectra of excit
ed states of C-60 in twelve solvents were measured in the 590-1190 nm wavel
ength range. The absorption spectra observed immediately after a 532 nm pic
osecond laser excitation and those in the late-time region depended upon th
e solvents. In particular, the former dependence was much larger than the l
atter one. Their spectral shapes did not correlate with either dielectric c
onstant of the solvents or their refractive index, but with their ionizatio
n potential (I-p). The early-gated absorption spectra of C-60 in solvents w
ith a small I-P were extraordinary broad compared with those in solvents wi
th a large I-P. In addition, the absorption changed to those observed in th
e late-time region both with a decay time constant of 1.2+/-0.05 ns and wit
h keeping the isosbestic points. This time constant was the same as the lif
etime of the C-60-singlet excited state (C-1(60)*) reported previously, and
the presence of the isosbestic points was also the same as that observed d
uring spectral evolution from S-n<--S-1 absorption of Csa to its T-n<--T-1
one. Combining the results of the resonance Raman spectra by Gallagher et a
l. with the present ones suggested that the solvent-dependent early-gated a
bsorption spectra of the C-60-excited state are ascribed to C-1(60)* with a
distortion induced by specific interactions with solvents molecules throug
h the donation of their pi-electron density without forming obviously excit
ed-state complexes. The transient absorption spectra observed immediately a
fter the direct excitation of ground-state charge-transfer complexes formed
between C-60 and solvent molecules with a small I-P were not due to ionic
species, but to C-1(60)*, suggesting that the photogenerated ionic species
undergo a very rapid charge-recombination reaction to result in C-1(60)* an
d the ground-state solvent molecule. The absorption spectra in the late-tim
e region, which showed a slight dependence on I-P of the solvent molecules,
as aforementioned, were assigned to the T-n<--T-1 absorption of C-60; the
dependence was considered to be also ascribed to the same reason as that fo
r C-1(60)*.