OCS was photodissociated near 217 and 230 nm, and the resulting CO was
probed by 2 + 1 resonant multiphoton ionization (REMPI) using the B-1
Sigma(+), C-1 Sigma(+) <--<-- X(1) Sigma(+) transitions. The CO+ was
detected by the ion imaging technique of Chandler and Houston. The nas
cent CO was found only in the v = 0 state, and its rotational state po
pulation distribution was bimodal. It is remarkable that this CO rotat
ional distribution has no tail extending to states of lower J. beta va
lues rise monotonically with J. Recent potential energy surface calcul
ations by Rokutan et al. provide reasonable explanations for the resul
ts: (1) dissociation can take place from near degenerate A '' and A' s
tates, each of which generates a different CO product distribution; (2
) a molecule excited by the initial absorption to an A' state can cros
s over in linear geometry at two different C-S distances to dissociati
ng states.