Dynamics calculations of kinetic isotope effects for the reactions of muonium atoms with F2 and Cl2
暂无分享,去创建一个
[1] M. Baer. Analytical fitting of potential energy surfaces for the Hxy systems , 1986 .
[2] B. C. Garrett,et al. Test of Variational Transition State Theory and Multidimensional Semiclassical Transmission Coefficient Methods against Accurate Quantal Rate Constants for H + H2/HD, D + H2, and O + H2/D2/HD, Including Intra- and Intermolecular Kinetic Isotope Effects , 1986 .
[3] D. Truhlar,et al. Diffusion of hydrogen, deuterium, and tritium on the (100) plane of copper: Reaction-path formulation, variational transition state theory, and tunneling calculations , 1985 .
[4] D. Truhlar,et al. Large tunneling effects in the migration of chemisorbed hydrogen on a metal , 1985 .
[5] B. C. Garrett,et al. Test of variational transition state theory and the least-action approximation for multidimensional tunneling probabilities against accurate quantal rate constants for a collinear reaction involving tunneling into an excited state , 1985 .
[6] D. Walker. Leptons in chemistry , 1985 .
[7] B. C. Garrett,et al. Variational transition state theory with least‐action tunneling calculations for the kinetic isotope effects in the Cl+H2 reaction: Tests of extended‐LEPS, information‐theoretic, and diatomics‐in‐molecules potential energy surfaces , 1985 .
[8] W. Jakubetz. A two-mechanism model of the H + F2 reaction , 1985 .
[9] F. B. Brown,et al. Semiclassical reaction‐path methods applied to calculate the tunneling splitting in ammonia , 1985 .
[10] B. C. Garrett,et al. Characterization of exit‐channel barriers for chemical reactions producing specific vibrational states , 1984 .
[11] B. C. Garrett,et al. Test of variational transition state theory against accurate quantal results for a reaction with very large reaction‐path curvature and a low barrier , 1984 .
[12] 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 .
[13] M. Baer. Three‐dimensional DIM‐3C potential energy surfaces for the reactions H+XY and X+HY (X,Y=F, Cl, Br, I) , 1984 .
[14] D. Bondi,et al. Exact quantum and vibrationally adiabatic quantum, semiclassical and quasiclassical study of the collinear reactions Cl + MuCl, Cl + HCl, Cl + DCl , 1983 .
[15] Donald G. Truhlar,et al. Additions and Corrections - Incorporation of Quantum Effects in Generalized-Transition-State Theory , 1983 .
[16] K. Westberg,et al. Chemical Kinetic Data Sheets for High‐Temperature Chemical Reactions , 1983 .
[17] B. C. Garrett,et al. Test of variational transition state theory with a large‐curvature tunneling approximation against accurate quantal reaction probabilities and rate coefficients for three collinear reactions with large reaction‐path curvature: Cl+HCl, Cl+DCl, and Cl+MuCl , 1983 .
[18] B. C. Garrett,et al. Variational transition state theory and tunneling for a heavy–light–heavy reaction using an ab initio potential energy surface. 37Cl+H(D) 35Cl→H(D) 37Cl+35Cl , 1983 .
[19] B. C. Garrett,et al. Comparison of variational transition state theory and quantum sudden calculations of three‐dimensional rate coefficients for the reactions D(H)+BrH → DBr(HBr)+H , 1983 .
[20] B. C. Garrett,et al. A least‐action variational method for calculating multidimensional tunneling probabilities for chemical reactions , 1983 .
[21] B. C. Garrett,et al. Vibrationally adiabatic models for reactive tunneling , 1982 .
[22] B. C. Garrett,et al. Kinetic isotope effects in the Mu+H2 and Mu+D2 reactions: Accurate quantum calculations for the collinear reactions and variational transition state theory predictions for one and three dimensions , 1982 .
[23] B. C. Garrett,et al. Incorporation of quantum effects in generalized-transition-state theory , 1982 .
[24] D. Walker. Muonium. A light isotope of hydrogen , 1981 .
[25] B. C. Garrett,et al. A general small-curvature approximation for transition-state-theory transmission coefficients , 1981 .
[26] D. Dixon,et al. Location and energetics of transition states for the reactions H+ClF, H+FCl, H+F2, and H+Cl2 , 1981 .
[27] J. Connor. Isotope effects and chemical reaction dynamics of muonium in the gas phase , 1981 .
[28] D. M. Garner,et al. Temperature dependence of muonium reaction rates in the gas phase , 1981 .
[29] B. C. Garrett,et al. Reaction probabilities, resonances, and thermal rate constants for the collinear reactions H + FH and D + FD on a low-barrier surface. Close-coupling and tunneling calculations, variational transition-state theory, and the unified statistical model , 1981 .
[30] Donald G. Truhlar,et al. Comparison of variational transition state theory and the unified statistical model with vibrationally adiabatic transmission coefficients to accurate collinear rate constants for T+HD→TH+D , 1980 .
[31] Donald G. Truhlar,et al. Improved treatment of threshold contributions in variational transition-state theory , 1980 .
[32] B. C. Garrett,et al. Variational transition state theory, vibrationally adiabatic transmission coefficients, and the unified statistical model tested against accurate quantal rate constants for collinear F+H2, H+F2, and isotopic analogs , 1980 .
[33] B. C. Garrett,et al. Application of variational transition-state theory and the unified statistical model to H + Cl/sub 2/. -->. HCl + Cl , 1980 .
[34] B. C. Garrett,et al. Reliable ab initio calculation of a chemical reaction rate and a kinetic isotope effect: H + H(2) and H + H(2). , 1979, Proceedings of the National Academy of Sciences of the United States of America.
[35] W. Jakubetz. Gas-phase muonium chemistry, isotope effects, and collision theory: Theoretical investigations of the Mu+F2 and Mu+Cl2 reactions and their isotopic counterparts , 1979 .
[36] W. Jakubetz. Tunneling in collinear light-heavy-heavy reactions , 1979 .
[37] J. Brewer,et al. Reaction dynamics of the Mu atom using surface muons in the gas phase , 1979 .
[38] B. C. Garrett,et al. Accuracy of tunneling corrections to transition state theory for thermal rate constants of atom transfer reactions , 1979 .
[39] J. Brewer,et al. Muonium chemistry: kinetics of the gas phase reaction Mu + F2 → MuF + F from 300 to 400 K , 1978 .
[40] J. Manz,et al. Isotope effects in the reaction X + F2 → XF + F(X = Mu, H, D, T): A quantum mechanical and information theoretic investigation , 1978 .
[41] J. Warnatz,et al. Rate Measurements for the Reaction of H-Atoms with F2 , 1977 .
[42] R. T. Watson. Rate constants for reactions of ClOx of atmospheric interest , 1977 .
[43] G. Marshall,et al. The chemical reaction of muonium with Cl2 in the gas phase , 1977 .
[44] J. Brewer,et al. Muonium Chemistry in the Gas Phase , 1977 .
[45] J. Manz,et al. Muonium chemistry: quantum mechanical calculations for the collinear reaction Mu + F2(ν = 0) → MuF(ν′ ⩽ 3) + F , 1977 .
[46] M. Clyne,et al. Atomic resonance fluorescence for rate constants of rapid bimolecular reactions. Part 6.—Hydrogen atom reactions: H + Cl2 from 300 to 730 K and H + NO2 at 298 K , 1977 .
[47] H. Wagner,et al. Rate Measurements for the Reaction H + Cl2 HCl + Cl by Lyman-α Fluorescence , 1976 .
[48] J. Polanyi,et al. Distribution of reaction products (theory). XI. H + F2 , 1975 .
[49] C. Bender,et al. Saddle point geometry and barrier height for H + F2 → HF + F , 1974 .
[50] D. S. Perry,et al. Effect of changing reagent energy on reaction probability and product energy-distribution , 1973 .
[51] D. H. Slater,et al. Initial vibrational energy distributions determined by infra-red chemiluminescence. I. The reaction of fluorine atoms with hydrogen and methane , 1972 .
[52] Donald G. Truhlar,et al. EXACT TUNNELING CALCULATIONS. , 1971 .
[53] A. Dodonov,et al. Mass‐Spectrometric Determination of Rate Constants for H‐Atom Reactions with Cl2 and F2 , 1969 .
[54] C. E. Young,et al. Energy Distribution Among Products of Exothermic Reactions. II. Repulsive, Mixed, and Attractive Energy Release , 1966 .