The nascent quantum state distributions of the RbH product resulting from t
he reaction of Rb(5(2)D(3/2,5/2), 7(2)S(1/2)) with H-2 are determined using
a laser pump-probe technique. For the three investigated reactions, the na
scent RbH product molecules are found to populate the lowest three vibratio
nal (upsilon = 0, 1, and 2) levels of the ground electronic state. The rela
tive vibrational populations an determined to be (0.42, 0.31, 0.27) for the
Rb(5(2)D(3/2)) + H-2 reaction, (0.42, 0.33, 0.25) for the Rb(5(2)D(5/2)) H-2 reaction, and (0.45, 0.32, 0.23) for the Rb(7(2)S(1/2)) + H-2 reaction
, each corresponding to a high vibrational temperature. The nascent RbH rot
ational temperatures are found to be slightly below the cell temperature. B
y comparing the spectral intensities of the RbH action spectra with those o
f pertinent Rb atomic fluorescence excitation spectra, the relative reactiv
ity with H-2 for the three studied atoms is in an order of Rb(7(2)S(1/2)) >
Rb(5(2)D(3/2)) > Rb(5(2)D(5/2)). The relative fractions ([fv], [f(R)], [f(
T)]) of average energy disposal are derived as (0.17, 0.04, 0.79) for the R
b(5(2)D(5/2)) case, (0.17, 0.04, 0.79) for the Rb(5(2)D(5/2)) case, and (0.
14, 0.03, 0.83) for the Rb(7(2)S(1/2)) case, all having a major translation
al energy release and a minor rotational energy release. All of the above r
esults support the assumption that the Rb*-H-2 reaction occurs primarily in
a collinear C-infinity upsilon collision geometry by a harpoon mechanism,
in which the crossing between the ionic Rb+H2- energy surface and the neutr
al Rb*-H-2 energy surfaces plays a very crucial role. A further comparison
with two previous results reveals that the average vibrational disposal [f(
v)] in MH changes dramatically as the excited alkali atom M* is varied from
K* to Rb* and to Cs*. The [f(v)] value for the (K* + H-2) system is close
to the prior distribution limit, but it becomes smaller and smaller for the
(Rb* + H-2) system and for the (Cs* + H-2) system.