We present results of six-dimensional (6D) quantum wave-packet calculations
for the dissociative adsorption of (v = 0,j = 4,m(j)) H-2 on Cu(100). The
potential-energy surface is a fit to points calculated using density-functi
onal theory (DFT), with the generalized gradient approximation (GGA), and a
slab representation for the surface. New aspects of the methodology we use
to adapt the wave function to the symmetry of the surface, which relate to
calculations for initial rotational states with odd m(j) (the magnetic qua
ntum number), are explained. Invoking detailed balance, we calculate the qu
adrupole alignment for H-2 as it would be measured in an associative desorp
tion experiment. The reaction of the helicopter (v = O,j = 4,m(j) = 4) stat
e is preferred over that of the ( v = 0,j = 4,m(j) = 0) cartwheel state for
all but the lowest collision energies considered here. The energy dependen
ce of the quadrupole alignment that we predict for (v = 0,j =4) H-2 desorbi
ng from Cu(100) is in good qualitative agreement with velocity-resolved ass
ociative desorption experiments for D-2 + Cu(111). The vibrational excitati
on probability P(v = 0,j --> v = 1) is much larger for j = 4 than for j = 0
, and the m(j)-dependence of P(v = 0,j = 4,m(j) --> v = 1) is markedly diff
erent from that of the initial-state-resolved reaction probability. For all
but the highest collision energies, vibrational excitation from the (v = 0
,j = 4) state is accompanied by loss of rotational energy, in agreement wit
h results of molecular beam experiments on scattering of H-2 and D-2 from C
u(111). (C) 1999 American Institute of Physics.