Time-resolved spectroscopic techniques are used to determine the primary ph
otoprocesses of A2E in solution. Comparison of the absorption and excitatio
n spectrum of A2E in methanol solution indicates excitation 400 nm populate
s the S-2 excited state. Transient absorption signals decaying with a time
constant of 0.9 ps were observed probing around 800 nm. These signals are a
ttributed to the S-2-->S-n transition and reveal the S-2-->S-1 relaxation o
ccurs on the subpicosecond time scale. Transient absorption data probing at
shorter wavelengths (480 and 550 nm) are attributed to the S-1-->S-n absor
ption. These signals exhibit an exponential decay with a time constant of 1
1 and 13 ps, respectively. Time-resolved emission measurements of the corre
sponding S-0<--S-1 decay reveal a nonexponential decay; however, > 95 % of
the signal amplitude is described by an exponential decay with a time const
ant of 12.4 ps. Both time-resolved emission and absorpti.on experiments the
refore indicate repopulation of the ground electronic state occurs with a t
ime constant of similar to 12 ps. A weak transient absorption probing in th
e blue (400 nm) persists onto the nanosecond time scale and is attributed t
o the T-1-->T-n absorption of A2E. Photoacoustic spectroscopy establishes t
he quantum yield for intersystem crossing of A2E in methanol solution is at
most 0.03. The emission quantum yield of A2E in ethanol is determined to b
e 0.01, and so, nonradiative relaxation is the dominant primary event. The
quantum yield for the generation of singlet molecular oxygen following 355
mn excitation of A2E in acetonitrile was determined to be 0.02, consistent
with a low production of the excited triplet state. These results establish
A2E is not an efficient photogenerator of reaction oxygen species in solut
ion.