The lifetimes of gas phase CO2˙− and N2O˙− calculated from the transition probability of the autodetachment process A− → A + e−

A procedure to calculate the quantum mechanical transition probability of a unimolecular primary chemical process, A− A + e− is investigated for the circumstance where A− and A have different numbers of vibrational and rotational degrees of freedom (one is linear, the other not). A procedure is introduced to deal with the coupling between the vibrational and rotational motions. The proposed method was applied to calculating the lifetimes of CO2˙− and N2O˙− in the gas phase. The geometry optimizations and frequency calculations for CO2, CO2˙−, N2O, and N2O˙− are performed at HF, MP2, and QCISD(T) levels with 6-31G* or 6–31+G* basis sets, in order to obtain reliable geometric and spectroscopic information on these systems. Lifetimes are calculated for several of the lower vibrational–rotational states of the anions, as well as for the Boltzmann distribution of states at 298 K. The lifetime of the lowest vibrational–rotational state of CO2˙−, is 1.03 × 10−4 s, and of the lowest vibrational state with rotational levels weighted by Boltzmann distribution at 298 K, 1.50 × 10−4 s. These values are in good agreement with the experimental number, 9.0 ± 2.0 × 10−5 s, and support the experimental evidence that CO2˙− was formed in its ground vibrational level by the techniques used. The lifetime of CO2˙− calculated with Boltzmann distribution over its vibrational and rotational levels at 298 K, is 1.51 × 10−5 s. There are no direct measurements of the lifetime of N2O˙−, but it was estimated to be greater than 10−4 s from experimental evidence. The predicted lifetimes of N2O˙−, at its lowest vibrational–rotational state (0 K) and lowest vibrational state with rotational levels weighted by the Boltzmann distribution at 298 K, are 238 and 19.1 s, respectively. The lifetime of N2O˙− at thermal equilibrium at 298 K is 6.66 × 10−2 s, indicating that electron loss from the excited vibrational states of N2O˙− is significant. This study represents the first theoretical investigation of CO2˙− and N2O˙− lifetimes. © 1994 John Wiley & Sons, Inc.

[1]  A. Rauk,et al.  The transition probability of electron loss from anions in the gas phase: The lifetime of O2 ⋅− , 1992 .

[2]  A. Rauk,et al.  Electron affinities and thermodynamic properties of some triatomic species , 1992 .

[3]  Krishnan Raghavachari,et al.  Gaussian-2 theory for molecular energies of first- and second-row compounds , 1991 .

[4]  C. Schöneich,et al.  Reactions of CO2˙– radicals with pterin and pterin-6-carboxylate ions , 1991 .

[5]  Henry F. Schaefer,et al.  A systematic study of molecular vibrational anharmonicity and vibration-rotation interaction by self-consistent-field higher-derivative methods. Linear polyatomic molecules , 1990 .

[6]  M. Jacox,et al.  The vibrational spectra of molecular ions isolated in solid neon. I. CO+2 and CO−2 , 1989 .

[7]  C. Freidhoff,et al.  Negative ion photoelectron spectroscopy of N2O− and (N2O)−2 , 1986 .

[8]  Y. Hatano,et al.  Thermal electron attachment to van der Waals molecules (O2⋅N2) , 1983 .

[9]  D. Yarkony On the reaction Mg+N2O→MgO+N2 , 1983 .

[10]  H. Schaefer,et al.  Theoretical investigation of the electron affinity of CO2 , 1981 .

[11]  W. England Accurate ab initio scf energy curves for the lowest electronic states of co2/co−2 , 1981 .

[12]  R. W. Fessenden,et al.  Thermal electron attachment to oxygen and van der Waals molecules containing oxygen , 1981 .

[13]  K. Jordan,et al.  Ab initio study of bis(nitrogen dioxide)(1+) and bis(carbon dioxide)(1-) ions , 1980 .

[14]  R. Compton,et al.  Electron attachment to carbon dioxide clusters in a supersonic beam , 1977 .

[15]  Y. Hatano,et al.  Thermal electron attachment to O2 in the presence of various compounds as studied by a microwave cavity technique combined with pulse radiolysis , 1977 .

[16]  D. G. Hopper,et al.  Theoretical and experimental studies of the N2O− and N2O ground state potential energy surfaces. Implications for the O−+N2→N2O+e and other processes , 1976 .

[17]  P. J. Fortune,et al.  Abinitio vertical spectra and linear bent correlation diagrams for the valence states of CO2 and its singly charged ions , 1976 .

[18]  F. Koike Low Energy Resonant Electron Scattering by O 2 and NO , 1975 .

[19]  P. W. Reinhardt,et al.  Collisional ionization of Na, K, and Cs by CO2, COS, and CS2: Molecular electron affinities , 1975 .

[20]  P. Bagus,et al.  SCF ab‐initio ground state energy surfaces for CO2 and CO2− , 1975 .

[21]  A. O. Allen,et al.  Chemical reaction rates of quasi-free electrons in non-polar liquids. The equilibrium CO2 + e− CO2− , 1975 .

[22]  G. Schulz,et al.  Vibrational excitation in CO2via the 3.8-eV resonance , 1974 .

[23]  L. Christophorou,et al.  Attachment of slow (<1 eV) electrons to O2 in very high pressures of nitrogen, ethylene, and ethane , 1974 .

[24]  F. Koike Resonant Vibrational Excitation of O2 by Slow Electron Impact , 1973 .

[25]  R. Compton,et al.  Molecular electron affinities from collisional ionization of cesium. I. NO, NO2, and N2O , 1973 .

[26]  F. Koike,et al.  On the Mechanism of Electron Attachment by O2 , 1973 .

[27]  L. Christophorou INTERMEDIATE PHASE STUDIES FOR UNDERSTANDING RADIATION INTERACTION WITH CONDENSED MEDIA. THE ELECTRON ATTACHMENT PROCESS. , 1972 .

[28]  R. Compton,et al.  Metastable anions of CO2 , 1972 .

[29]  D. Neumann,et al.  Energy curves of CO−2 , 1972 .

[30]  J. Bardsley Negative Ions of N2O and CO2 , 1969 .

[31]  島内 みどり,et al.  G. Herzberg: Molecular Spectra and Molecular Structure. III. Electronic Spectra and Electronic Structure of Polyatomic Molecules, D. Van Nostrand, Prinston 1966, 745頁, 16.5×24cm, 8,000円. , 1968 .

[32]  I. Hisatsune,et al.  Infrared Spectrum of Carbon Dioxide Anion Radical , 1966 .

[33]  T. E. Sharp,et al.  Franck—Condon Factors for Polyatomic Molecules , 1964 .

[34]  D. W. Ovenall,et al.  Electron spin resonance and structure of the CO-2radical ion , 1961 .