We present a crossed beam study of the title reaction over the
collision energy range from 0.47 to 1.20 eV,
over which the dynamics of particle transfer are direct. The data
include vibrational state populations and
vibrational-state dependent angular distributions. Over the entire
collision energy range, the product vibrational
state distributions are inverted, and the extent of that inversion as
measured by the vibrational surprisal increases
with increasing collision energy. The energy dependence of the
product vibrational state distributions is
partially consistent with mixed energy release in the Heavy +
Light−Light mass combination, but it more
closely resembles the behavior of proton transfer in the
O- + HF system at low energies, where the
attractive
well induces corner cutting trajectories, leading to partitioning of
increased reagent translation into product
vibration. The most probable rotational energy is approximately
constant as a function of vibrational quantum
number and is effectively independent of collision energy. This
saturation effect is consistent with the softening
of the low energy repulsive wall as the collision geometry changes from
collinear to bent. Several features
of the data can be rationalized with extant ab initio
calculations, but other features, especially the
vibrational
state populations, require additional theoretical insight for complete
understanding.