The widely used assumption that transitions induced by slowly changing pert
urbations are completely described by the topology of adiabatic energy surf
aces in the plane of a complex perturbation parameter is reexamined. This a
ssumption is the basis for the hidden crossings theory and most two-state m
odels and yields an exponential decrease of transition probabilities and cr
oss sections with decreasing speed of the perturbation v. We show that for
a large class of problems, these approximations do not describe correctly t
ransitions in the adiabatic limit. Contributions neglected lead, instead, t
o dominant power-law dependences in inelastic collisional cross sections, s
igma infinityv(4). We illustrate the interplay between different contributi
ons for a collisional model system for which exact transition probabilities
can be determined.