Ab initio ground potential energy surface and quasiclassical trajectory study of the O(D-1)+CH4(X (1)A(1))-> OH(X (2)Pi)+CH3(X (2)A(2)'') reaction dynamics

Citation
M. Gonzalez et al., Ab initio ground potential energy surface and quasiclassical trajectory study of the O(D-1)+CH4(X (1)A(1))-> OH(X (2)Pi)+CH3(X (2)A(2)'') reaction dynamics, J CHEM PHYS, 111(19), 1999, pp. 8913-8924
Citations number
53
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
JOURNAL OF CHEMICAL PHYSICS
ISSN journal
00219606 → ACNP
Volume
111
Issue
19
Year of publication
1999
Pages
8913 - 8924
Database
ISI
SICI code
0021-9606(19991115)111:19<8913:AIGPES>2.0.ZU;2-Z
Abstract
An ab initio study of the ground potential energy surface (PES) of the O(D- 1)+CH4--> OH+CH3 reaction has been performed using the second and fourth or der Moller-Plesset methods with a large basis set. From the ab initio data a triatomic analytical ground PES with the methyl group treated as an atom of 15.0 amu has been derived. This PES has been employed to study the dynam ics of the reaction by means of the quasiclassical trajectory (QCT) method. A good agreement between the experimental and QCT OH rovibrational distrib utions at a collision energy of 0.212 eV with the methane molecule at 298 K has been obtained. The analysis of the microscopic reaction mechanism show s that the reaction takes place almost exclusively through the insertion of the O(D-1) atom into a C-H bond, due to the presence of the deep (CH3)OH m inimum, and the resulting trajectories may be direct or nondirect (short-li ved collision complexes mainly) with about the same probability. The OH vib rational distribution arising from the direct mechanism is inverted, while the nondirect mechanism leads to a noninverted one. There is some tendency to give broader OH rotational distributions peaking at higher N-' values, p articularly for the vibrational levels v'=0-1, in the case of the nondirect trajectories. The PES derived here may be used in dynamics studies under c onditions where the methyl group motions are not strongly coupled to the mo tions leading to reaction. (C) 1999 American Institute of Physics. [S0021-9 606(99)30442-6].