We have investigated the kinetics of excitation and lasing of the free
radical SO by rotationally-resolved optical pumping near 250 nm with
a continuously-tunable, narrow-line width KrF laser. Longitudinal phot
odissociation of SO2 by a 193-nm ArF excimer laser produced SO(X(3) Si
gma(-)) concentrations close to 10(16) cm(-3) over a 50-cm length. Pum
ping of SO(B-3 Sigma(-)) by the KrF laser occurred from the v''=2 grou
nd state cm vibrational level which was preferentially produced by pho
todissociation. The fraction of ground state population that could be
excited to SO(B) was determined by measuring the saturation fluence fo
r excitation as a function of buffer gas pressure and comparing with a
simple model. Addition of a buffer gas increased excitation by nearly
30 times due to increased rotational mixing in the ground electronic
state. Lasing was demonstrated on six new vibrational bands of fully-a
llowed SO(B-X) band in the region 262-315 nm. A small-signal gain coef
ficient of 0.11 cm(-1) and pulse energy of 11 mu J were achieved on th
e 270-nm SO-(B,v'=2-->X,v''=5) laser transition. A full computational
rate equation model of the excitation and lasing dynamics, including c
ollisional rotational mixing, was developed. The A(3) Pi electronic st
ate of SO was also investigated as a possible ultraviolet energy stora
ge laser medium. Excitation of SO(A(3) Pi,v'=5,6) near 250 nm was achi
eved after a time delay from photodissociation to allow for vibrationa
l relaxation into SO(X,v''=0). Measurements of the radiative lifetime,
deactivation rate, and saturation fluence, along with computation mod
eling, indicate that a storage laser based on the weak SO(A,v'=0-->X,v
''=4) transition is not feasible with our production and excitation ca
pabilities. Lasing on a direct-pumped single rotational transition of
the SO(A,v'=5-->X,v''=1) band may be possible, but with very limited c
apacity to store energy.