Ab initio studies of the structures and energies of the H−(H2O) and H−(H2O)2 complexes

Accurate calculations for the H−(H2O) complex with extended basis sets are reported at the restricted Hartree–Fock (RHF) through the fourth‐order Mo/ller–Plesset (MP) perturbation levels of theory. In the equilibrium geometry of the H−(H2O) complex the H− anion is found to lie almost along one of the H–O bond directions. The H–H− distance proved to be very sensitive to electron correlation effects: it is 1.8 and 1.4 A at the RHF and MP2 levels, respectively. The interaction energy between H− and H2O at the MP4 level including conterpoise corrections for basis set superposition error, depending upon the basis set used, is found to range from 16.2 to 16.9 kcal/mol, and the electron correlation is responsible for one‐third of this value. The enthalpy of formation of H−(H2O) is estimated to be from −15.2 to −16.0 kcal/mol compared with the experimental value of −17.3±1.2 kcal/mol. The vibrational frequencies of H−(H2O) are also reported. The H−(H2O)2 complex is also studied by using a polarized double zeta ba...

[1]  Timothy Clark,et al.  Efficient diffuse function‐augmented basis sets for anion calculations. III. The 3‐21+G basis set for first‐row elements, Li–F , 1983 .

[2]  Michael J. Frisch,et al.  Contribution of triple substitutions to the electron correlation energy in fourth order perturbation theory , 1980 .

[3]  Kimihiko Hirao,et al.  The calculation of higher-order energies in the many-body perturbation theory series , 1985 .

[4]  D. Cremer,et al.  Theoretical determination of molecular structure and conformation. 17. On the existence of FH2-, OH3-, NH4-, and CH5- in the gas phase , 1986 .

[5]  M. Newton,et al.  The water dimer: Theory versus experiment , 1983 .

[6]  M. Ferreira Ionic processes in the gas phase , 1983 .

[7]  G. Diercksen,et al.  Finite-field many-body perturbation theory. VII. A complete fourth-order MBPT study of multipole moments of the CO molecule , 1985 .

[8]  M. Arshadi,et al.  Hydration of the halide negative ions in the gas phase. II. Comparison of hydration energies for the alkali positive and halide negative ions , 1970 .

[9]  R. Ahlrichs,et al.  The impact of higher polarization basis functions on molecular ab initio results. I. The ground state of F2 , 1985 .

[10]  Ab initio study of structures and binding energies for anion-water complexes , 1986 .

[11]  Stephen Wilson,et al.  van der Waals interaction potentials: Many-body basis set superposition effects☆ , 1983 .

[12]  H. Haberland,et al.  Negatively Charged Water Clusters, or the First Observation of Free Hydrated Electrons , 1981 .

[13]  G. Diercksen,et al.  The ground state potential energy. Curve of Be2: Is the MBPT approach capable of predicting it? , 1985 .

[14]  A. Sapse,et al.  Ab initio studies of F−(H2O)n and Cl−(H2O)n clusters for n = 1, 2 , 1985 .

[15]  G. Diercksen,et al.  Finite-field many-body perturbation theory IV. Basis set optimization in MBPT calculations of molecular properties. Molecular quadrupole moments , 1983 .

[16]  M. Gutowski,et al.  THE BASIS SET SUPERPOSITION ERROR IN CORRELATED ELECTRONIC STRUCTURE CALCULATIONS , 1986 .

[17]  L. Curtiss,et al.  Theoretical studies of O2−:(H2O)n clusters , 1986 .

[18]  P. Dacre The interaction of a water molecule with an ion at a distance , 1984 .

[19]  E. E. Muschlitz Formation of Negative Ions in Gases by Secondary Collision Processes , 1957 .

[20]  N. Nibbering,et al.  The long-lived H3O− ion in the gas phase: Its formation, structure and reactions , 1983 .

[21]  P. C. Hariharan,et al.  The influence of polarization functions on molecular orbital hydrogenation energies , 1973 .

[22]  C. Glidewell Ligands of low electronegativity in the vsepr model: electron-rich hydrides MH3E2, MH4E, MH5E, and MH6E , 1980 .

[23]  J. Rayez,et al.  Theoretical study of the H3− cluster , 1981 .

[24]  E. Clementi,et al.  Study of the Structure of Molecular Complexes. I. Energy Surface of a Water Molecule in the Field of a Lithium Positive Ion , 1972 .

[25]  J. V. Lenthe,et al.  Ab initio calculations on weakly bonded systems , 1984 .

[26]  S. J. Cole,et al.  Correlated calculation of the interaction in the nitromethane dimer , 1986 .

[27]  Enrico Clementi,et al.  Study of the electronic structure of molecules. XXI. Correlation energy corrections as a functional of the Hartree‐Fock density and its application to the hydrides of the second row atoms , 1974 .

[28]  M. Frisch,et al.  Ab initio computation of the enthalpies of some gas-phase hydration reactions , 1983 .

[29]  J. V. Lenthe,et al.  An analysis of the partial wave expansion of the dispersion energy for Ne2 , 1984 .

[30]  P. H. Smit,et al.  On the role of the distortion energy in the ab initio calculated dimerization energy of formic acid , 1978 .

[31]  K. Hirao,et al.  Theoretical study on the structure and stability of X−(CH3CN)n (X = F and Cl, n = 1,2,3,4) clusters , 1981 .

[32]  S. F. Boys,et al.  The calculation of small molecular interactions by the differences of separate total energies. Some procedures with reduced errors , 1970 .

[33]  G. Diercksen,et al.  Finite-field many-body perturbation theory. IX: Electric properties of ammonia , 1986 .

[34]  M. Bulski SCF non-additivity of the interaction energy in the neon trimer , 1981 .