A quantitative comparison of the results from quantum and classical co
mputations of the dissociation of H-2 on the ab initio Cu(111) surface
is presented. In order to initiate a detailed comparison of the class
ical and quantum methods, we chose to investigate motion on the vibrat
ionally adiabatic ground state. This subtracts from the problem the la
rgest quantum degree of freedom with the consequence that broadly spea
king, quantum and classical results for the dissociation as a function
of initial rotational state and incidence angle agree well. One featu
re arising from the calculations is that for the first time we have sh
own how the quantized nature of motion near the transition state affec
ts experimental observables. We demonstrate that hitherto neglected st
ructure in dissociation probabilities may be traced to quantized hinde
red rotational and translational motion. An additional consequence of
the quantization is a pronounced J-dependent broadening in the dissoci
ation probabilities when plotted as a function of the translational en
ergy which should be experimentally observable.