INSTITUTE OF PHYSICS PUBLISHING NONLINEARITY
Nonlinearity 15 (2002) 957–992 PII: S0951-7715(02)27575-1
The geometry of reaction dynamics
T Uzer
1
, Charles Jaff´ e
2
, Jes ´ us Palaci´ an
3
, Patricia Yanguas
3
and
Stephen Wiggins
4
1
Center for Nonlinear Sciences, School of Physics, Georgia Institute of Technology, Atlanta,
GA 30332-0430, USA
2
Department of Chemistry, West Virginia University, Morgantown, WV 26506-6045, USA
3
Departamento de Matem´ atica e Inform´ atica, Universidad P´ ublica de Navarra,
31006 Pamplona, Spain
4
School of Mathematics, University of Bristol, Bristol, BS8 1TW, UK
Received 30 July 2001, in final form 15 February 2002
Published 22 April 2002
Online at stacks.iop.org/Non/15/957
Recommended by P Cvitanovi´ c
Abstract
The geometrical structures which regulate transformations in dynamical
systems with three or more degrees of freedom (DOFs) form the subject of
this paper. Our treatment focuses on the (2n - 3)-dimensional normally
hyperbolic invariant manifold (NHIM) in nDOF systems associated with a
centre ×···× centre × saddle in the phase space flow in the (2n - 1)-
dimensional energy surface. The NHIM bounds a (2n - 2)-dimensional
surface, called a ‘transition state’ (TS) in chemical reaction dynamics, which
partitions the energy surface into volumes characterized as ‘before’ and ‘after’
the transformation. This surface is the long-sought momentum-dependent TS
beyond two DOFs. The (2n - 2)-dimensional stable and unstable manifolds
associated with the (2n - 3)-dimensional NHIM are impenetrable barriers with
the topology of multidimensional spherical cylinders. The phase flow interior
to these spherical cylinders passes through the TS as the system undergoes its
transformation. The phase flow exterior to these spherical cylinders is directed
away from the TS and, consequently, will never undergo the transition. The
explicit forms of these phase space barriers can be evaluated using normal form
theory. Our treatment has the advantage of supplying a practical algorithm,
and we demonstrate its use on a strongly coupled nonlinear Hamiltonian, the
hydrogen atom in crossed electric and magnetic fields.
Mathematics Subject Classification: 37C75, 37D10, 37J40, 70H09, 81V45,
78A35
1. Introduction
In this paper we develop a general formulation of the nonlinear dynamics and geometry
of classical reaction dynamics. Our formalism hinges on finding, for the first time, the
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