Dynamical Hierarchy in Transition States: Why and How does a System Climb over the Mountain?

How a reacting system climbs through a transition state during the course of a reaction has been an intriguing subject for decades. Here we present and quantify a technique to identify and characterize local invariances about the transition state of an N-particle Hamiltonian system, using Lie canoni...

Full description

Saved in:
Bibliographic Details
Published inProceedings of the National Academy of Sciences - PNAS Vol. 98; no. 14; pp. 7666 - 7671
Main Authors Komatsuzaki, Tamiki, Berry, R. Stephen
Format Journal Article
LanguageEnglish
Published United States National Academy of Sciences 03.07.2001
National Acad Sciences
The National Academy of Sciences
Subjects
Online AccessGet full text

Cover

Loading…
More Information
Summary:How a reacting system climbs through a transition state during the course of a reaction has been an intriguing subject for decades. Here we present and quantify a technique to identify and characterize local invariances about the transition state of an N-particle Hamiltonian system, using Lie canonical perturbation theory combined with microcanonical molecular dynamics simulation. We show that at least three distinct energy regimes of dynamical behavior occur in the region of the transition state, distinguished by the extent of their local dynamical invariance and regularity. Isomerization of a six-atom Lennard-Jones cluster illustrates this: up to energies high enough to make the system manifestly chaotic, approximate invariants of motion associated with a reaction coordinate in phase space imply a many-body dividing hypersurface in phase space that is free of recrossings even in a sea of chaos. The method makes it possible to visualize the stable and unstable invariant manifolds leading to and from the transition state, i.e., the reaction path in phase space, and how this regularity turns to chaos with increasing total energy of the system. This, in turn, illuminates a new type of phase space bottleneck in the region of a transition state that emerges as the total energy and mode coupling increase, which keeps a reacting system increasingly trapped in that region.
Bibliography:SourceType-Scholarly Journals-1
ObjectType-Feature-1
content type line 14
ObjectType-Article-1
ObjectType-Feature-2
content type line 23
To whom reprint requests should be addressed. E-mail: berry@chicago.edu.
Edited by Rudolph A. Marcus, California Institute of Technology, Pasadena, CA, and approved April 12, 2001
ISSN:0027-8424
1091-6490
DOI:10.1073/pnas.131627698