It is a generally held belief that inelastic transition probabilities and c
ross sections in slow, nearly adiabatic atomic collisions decrease exponent
ially with the inverse of the collision velocity v [i.e., sigma (alpha)exp(
-const/v)]. This notion is supported by the Landau-Zener approximation and
the hidden crossings approximation. We revisit the adiabatic limit of inn-a
tom collisions and show that for eely slow collisions radial transitions ar
e dominated by the topology of the branch points of the radial velocity rat
her than the branch points of the energy eigensurface. This can lead to a d
ominant power-law dependence of inelastic cross sections, sigma alphav(n).
We illustrate the interplay between different contributions to the transiti
on probabilities in a one-dimensional collision system for which the exact
probabilities can be obtained from a direct numerical solution of the time-
dependent Schodinger equation.