Regularity in chaotic reaction paths. I. Ar-6

Citation
T. Komatsuzaki et Rs. Berry, Regularity in chaotic reaction paths. I. Ar-6, J CHEM PHYS, 110(18), 1999, pp. 9160-9173
Citations number
51
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
JOURNAL OF CHEMICAL PHYSICS
ISSN journal
00219606 → ACNP
Volume
110
Issue
18
Year of publication
1999
Pages
9160 - 9173
Database
ISI
SICI code
0021-9606(19990508)110:18<9160:RICRPI>2.0.ZU;2-V
Abstract
We scrutinize the saddle crossings of a simple cluster of six atoms to show (a) that it is possible to choose a coordinate system in which the transmi ssion coefficient for the classical reaction path is unity at all energies up to a moderately high energy, above which the transition state is chaotic ; (b) that at energies just more than sufficient to allow passage across th e saddle, all or almost all the degrees of freedom of the system are essent ially regular in the region of the transition state; and (c) that the degre e of freedom associated with the reaction coordinate remains essentially re gular through the region of the transition state, even to moderately high e nergies. Microcanonical molecular dynamics simulation of Ar-6 bound by pair wise Lennard-Jones potentials reveals the mechanics of passage. We use Lie canonical perturbation theory to construct the nonlinear transformation to a hyperbolic coordinate system which reveals these regularities. This trans form "rotates away'' the recrossings and nonregular behavior, especially of the motion along the reaction coordinate, leaving a coordinate and a corre sponding dividing surface in phase space which minimize recrossings and mod e-mode mixing in the transition state region. The action associated with th e reactive mode tends to be an approximate invariant of motion through the saddle crossings throughout a relatively wide range of energy. Only at very low energies just above the saddle could any other approximate invariants of motion be found for the other, nonreactive modes. No such local invarian ts appeared at energies at which the modes are all chaotic and coupled to o ne another. (C) 1999 American Institute of Physics. [S0021-9606(99)50918-5] .