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]
.