Rotational and vibrational energy transfer rate constants have been me
asured for excited rovibrational levels of I-2(X). Stimulated emission
pumping was used to excite the levels upsilon = 23, J = 57, and upsil
on = 38, J = 49 via the B-X transition. Laser induced fluorescence fro
m the D-X system was used to follow the collision dynamics. Energy tra
nsfer processes induced by collisions with He,Ar,N-2,O-2,Cl-2,I-2, and
H2O were investigated. Rotational energy transfer was found to be eff
icient for all collision partners. In accordance with classical models
, the total rotational transfer rate constants were proportional to th
e collision momentum (except for H2O). The total transfer rate constan
ts and the distributions of rotational levels populated by collisions
were not dependent on the initial vibrational state. For colliders tha
t are not good quenchers of I-2(B), the rotational energy transfer dyn
amics of the X and B states were found to be very similar. For collide
rs that are good quenchers, comparisons of the X and B state dynamics
show that quenching competes with rotational energy transfer in the B
state. Vibrational energy transfer was characterized for all collision
partners with the exception of I-2, which appears to have a low vibra
tional transfer efficiency. Vibrational transfer was dominated by Delt
a upsilon = - 1 steps. Multiquantum vibrational transfer was not obser
ved. The dependence of the vibrational transfer rate constants on the
initial vibrational state appeared to be weaker than the linear scalin
g predicted by the Landau-Teller model. Vibrational deactivation of I-
2(X) plays an important role in chemically driven oxygen-iodine lasers
. Effective deactivation late constants have been derived from the vib
rational transfer rate constants. Estimates for the deactivation rate
constants for O-2 and H2O differ from those currently in use by almost
an order of magnitude. (C) 1997 American Institute of Physics.