COMPARING QUANTUM AND CLASSICAL DYNAMICS - H-2 DISSOCIATION ON W(100)

Citation
M. Kay et al., COMPARING QUANTUM AND CLASSICAL DYNAMICS - H-2 DISSOCIATION ON W(100), The Journal of chemical physics, 108(11), 1998, pp. 4614-4627
Citations number
72
Categorie Soggetti
Physics, Atomic, Molecular & Chemical
ISSN journal
00219606
Volume
108
Issue
11
Year of publication
1998
Pages
4614 - 4627
Database
ISI
SICI code
0021-9606(1998)108:11<4614:CQACD->2.0.ZU;2-4
Abstract
A quantitative comparison of the dissociation probabilities of H-2 On the W(100) surface obtained from quantum and classical dynamical simul ations is presented. Four dimensions are employed, and the vibrational ly adiabatic approximation is used to circumvent problems in classical mechanics associated with nonconservation of zero-point energy. For n ormal incidence, we find good agreement between the classical and quan tum dissociation probabilities. Both are dominated by strong steering into geometries favorable for dissociation. Exciting either initial ro tations or parallel translations reduces the effectiveness of steering , thus reducing the dissociation probability. For the former, the good agreement between classical and quantum still holds, however. for the latter this is not so, and the disagreement becomes progressively gre ater as the initial parallel momentum is increased. To understand this , we employ two new visualization techniques. For the classical dynami cs, we use swarms of color-coded trajectories to illustrate the detail ed motion of an ensemble. While for the quantum system, we project tim e-dependent wave packets onto a local basis set, adiabatic in the inte rnal (rotational and parallel translational) degrees of freedom, plott ing the results on the correlation diagram. Examination of these shows that the behavior of adiabatic states populated for normal incidence is dominated by a combination of steering and orientational hindering, both classical phenomena. In contrast, there are very large avoided c rossings in the states populated at off-normal incidence, leading to m otion which cannot be reproduced by a classical system. (C) 1998 Ameri can Institute of Physics.