Transition states, trapped trajectories, and classical bound states embedded in the continuum

We show that the best choice of transition state, for the atom exchange reaction in a classical collinear collision of an atom with a diatomic, is a classical bound state embedded in the continuum: a periodic vibration of the triatomic system across the interaction region of the potential surface. These unstable bound states also serve as limit sets of the trapped trajectories that form the boundary of reactivity bands in molecular collisions, and we comment on the implications of this result for calculation of product state distributions. Numerical calculations of transition states are presented for the collinear H+H2 and F+H2 reactions.

[1]  W. J. Chesnavich On the threshold behavior of collinear bimolecular exchange reactions , 1978 .

[2]  E. Pollak,et al.  Trapped trajectories at the boundary of reactivity bands in molecular collisions , 1977 .

[3]  K. Laidler,et al.  Reactivity bands in atom–molecule collisions. III. The coplanar (H, H2) reaction , 1977 .

[4]  Michael E. Coltrin,et al.  A new tunneling path for reactions such as H+H2→H2+H , 1977 .

[5]  Rudolph A. Marcus,et al.  Semiclassical calculation of bound states in a multidimensional system for nearly 1:1 degenerate systems , 1977 .

[6]  L. L. Lohr,et al.  On the exactness of classical transition state theory for collinear collisions , 1977 .

[7]  James S. Wright,et al.  Reactivity bands in atom--molecule collisions. II. X+HX on the collinear SSMK surface. [Total reactivity maps, probability, threshold energies, skewed coordinate axes, single and multiple collisions] , 1977 .

[8]  W. Miller Unified statistical model for ’’complex’’ and ’’direct’’ reaction mechanisms , 1976 .

[9]  D. Truhlar,et al.  Classical S matrix: Application of the Bessel uniform approximation to a chemical reaction☆ , 1976 .

[10]  J. Murrell,et al.  The behaviour of long-lived classical trajectories through saddle points and their contribution to the semi-classical S-matrix , 1976 .

[11]  K. Laidler,et al.  Energy bands in reactive collisions. I. H+H2 on the collinear SSMK surface , 1976 .

[12]  G. Schatz,et al.  Exact quantum, quasiclassical, and semiclassical reaction probabilities for the collinear F+H2 → FH+H reaction , 1975 .

[13]  D. W. Noid,et al.  Semiclassical calculation of bound states in a multidimensional system. Use of Poincaré’s surface of section , 1975 .

[14]  W. Miller,et al.  Accuracy of transition state theory for the threshold of chemical reactions with activation energy. Collinear and three-dimensional atomic hydrogen + molecular hydrogen , 1975 .

[15]  P. Pechukas,et al.  Quantum transition state theory , 1974 .

[16]  D. Truhlar,et al.  Classical S matrix: numerical applications to classically allowed chemical reactions , 1974 .

[17]  P. Pechukas,et al.  On transition‐state theory and the classical mechanics of collinear collisions , 1973 .

[18]  P. Pechukas Semiclassical Approximation of Multidimensional Bound States , 1972 .

[19]  M. Karplus,et al.  Collision Dynamics and the Statistical Theories of Chemical Reactions. II. Comparison of Reaction Probabilities , 1971 .

[20]  M. Karplus,et al.  Potential Energy Surface for H3 , 1964 .

[21]  E. Coddington,et al.  Theory of Ordinary Differential Equations , 1955 .

[22]  Eugene P. Wigner,et al.  The transition state method , 1938 .

[23]  Juro Horiuti,et al.  On the Statistical Mechanical Treatment of the Absolute Rate of Chemical Reaction , 1938 .

[24]  Eugene P. Wigner,et al.  Calculation of the Rate of Elementary Association Reactions , 1937 .