Improved potential energy surfaces for the reaction O(3P)+H2→OH+H

We present global 3A’ and 3A‘ potential energy surfaces for the reaction O(3P)+H2→OH+H and its isotopic analogs. The new surfaces are based in part on the surface of Lee et al. [J. Chem. Phys. 76, 3563 (1982)] for collinear O–H–H, which is modified to give accurate properties for reactants and products. The potentials for noncollinear O–H–H geometries are based on bending energies of Bowman et al. [J. Chem. Phys. 81, 1739 (1984)] as fit previously and called surface set M2 by two of the authors [B. C. Garrett and D. G. Truhlar, Int. J. Quantum Chem. 29, 1463 (1986)], and the potentials for H–O–H geometries are based on a new interpolation scheme. The new surfaces treat the approach of an O to either end of H2 equivalently. We used improved canonical variational transition state theory calculations with the least‐action ground‐state tunneling approximation (ICVT/LAG) to recalibrate the classical barrier height to 13.0 kcal/mol. The ICVT/LAG rate constants calculated using the new surfaces are in excellent ...

[1]  P. Marshall,et al.  HTP kinetics studies of the reactions of O(2 3PJ) atoms with H2 and D2 over wide temperature ranges , 1987 .

[2]  I. Paidarová,et al.  Diatomics‐in‐molecules models for H2O and H2O−. II. A self‐consistent description of the 1A′, 1A″, 3A′, and 3A″ states of H2O , 1987 .

[3]  P. Pacey,et al.  Effective bending frequencies, energies, and tunneling parameters of transition states from thermal rate data and semiempirical internuclear distances: DHH, HDD, OHH, ODD , 1987 .

[4]  S. Walch Extended active space CASSCF/MRSD CI calculations of the barrier height for the reaction O+H2→OH+H , 1987 .

[5]  T. Kitsopoulos,et al.  Evidence for tunneling in the reaction O(3P)+HD , 1987 .

[6]  J. Bowman,et al.  Reaction dynamics for O(3P)+HD. V. Reduced dimensionality quantum and quasiclassical reaction probabilities and rate constants with an adiabatic incorporation of the bending motion , 1987 .

[7]  J. Bowman,et al.  Reaction dynamics for O(3P)+H2, D2, and HD. VI. Comparison of TST and reduced dimensionality quantum and quasiclassical isotope effects with experiment , 1987 .

[8]  B. C. Garrett,et al.  Reaction rates for O + HD OH + D and O + HD OD + H , 1987 .

[9]  Wing Tsang,et al.  Chemical Kinetic Data Base for Combustion Chemistry. Part I. Methane and Related Compounds , 1986 .

[10]  B. C. Garrett,et al.  Thermal and state‐selected rate constant calculations for O(3p) + H2 → OH + H and isotopic analogs , 1986 .

[11]  B. C. Garrett,et al.  Ab Initio Predictions and Experimental Confirmation of Large Tunneling Contributions to Rate Constants and Kinetic Isotope Effects for Hydrogen Atom Transfer Reactions , 1986 .

[12]  J. Bowman,et al.  Inclusion and assessment of Renner–Teller coupling in transition state theory for Π states: Application to O(3P)+H2 , 1985 .

[13]  R. Gordon,et al.  The kinetic isotope effect in the reaction of O(3P) with H2, D2, and HD , 1985 .

[14]  Michael Baer,et al.  Theory of chemical reaction dynamics , 1985 .

[15]  J. Bowman,et al.  Reaction dynamics for O(3P)+H2 and D2. IV. Reduced dimensionality quantum and quasiclassical rate constants with an adiabatic incorporation of the bending motion , 1984 .

[16]  B. C. Garrett,et al.  WKB approximation for the reaction‐path Hamiltonian: Application to variational transition state theory, vibrationally adiabatic excited‐state barrier heights, and resonance calculations , 1984 .

[17]  K. Westberg,et al.  Chemical Kinetic Data Sheets for High‐Temperature Chemical Reactions , 1983 .

[18]  B. C. Garrett,et al.  A least‐action variational method for calculating multidimensional tunneling probabilities for chemical reactions , 1983 .

[19]  G. Schatz,et al.  A comparative study of the reaction dynamics of several potential energy surfaces for O(3P)+H2 → OH+H. II. Collinear exact quantum and quasiclassical reaction probabilities , 1982 .

[20]  G. B. Skinner,et al.  Resonance absorption measurements of atom concentrations in reacting gas mixtures. VIII. Rate constants for O+H2→OH+H and O+D2→OD+D from measurements of O atoms in oxidation of H2 and D2 by N2O , 1982 .

[21]  R. Jaquet,et al.  Cepa calculations of potential energy surfaces for open-shell systems. I. The reaction of O(3P) with H2(1Σg+) , 1981 .

[22]  D. Truhlar Potential Energy Surfaces and Dynamics Calculations , 1981 .

[23]  B. C. Garrett,et al.  Variational Transition State Theory , 1980 .

[24]  Donald G. Truhlar,et al.  Improved treatment of threshold contributions in variational transition-state theory , 1980 .

[25]  George C. Schatz,et al.  Theoretical studies of the O+H2 reaction , 1980 .

[26]  R. Raffenetti,et al.  A theoretical study of the potential energy surface for O(3P)+H2 , 1980 .

[27]  A. D. McLean,et al.  Extended basis first‐order CI study of the 1A′, 3A″, 1A″, and B̃ 1A′ potential energy surfaces of the O(3P,1D)+H2(1Σg+) reaction , 1979 .

[28]  B. C. Garrett,et al.  Generalized transition state theory. Classical mechanical theory and applications to collinear reactions of hydrogen molecules , 1979 .

[29]  Donald G. Truhlar,et al.  Importance of quartic anharmonicity for bending partition functions in transition-state theory , 1979 .

[30]  D. D. Drysdale,et al.  Evaluated kinetic data for high temperature reactions , 1972 .

[31]  R. Bader,et al.  Theoretical investigations of the chemistry of singlet and triplet species. I. Insertion and abstraction reactions , 1971 .

[32]  A. A. Westenberg,et al.  Atom—Molecule Kinetics Using ESR Detection. III. Results for O+D2→OD+D and Theoretical Comparison with O+H2→OH+H , 1967 .