Abstract

The binding energy, equilibrium geometry, and electronic structure of molecular hydrogen and helium atoms interacting with Ni, Cu, Co, and Al atoms and cations have been calculated using self-consistent-field linear combination of the atomic-orbitals--molecular-orbital method. The exchange interaction between the electrons is treated using the unrestricted Hartree-Fock theory. Correlation is included using M\oller-Plesset perturbation theory up to the fourth order. The accuracy of the calculation is tested by comparing the results of the ground-state spin and binding energy with available experiments on dimers. While a neutral metal atom is found to dissociate the ${\mathrm{H}}_{2}$ molecule, the metal cations bind the ${\mathrm{H}}_{2}$ molecule associatively and with rather large binding energy. The binding of the He atom to a metal cation is found to be analogous to that of a ${\mathrm{H}}_{2}$ molecule since both possess closed electronic shells. The number of hydrogen molecules and He atoms that can be bound to a metal cation at a given temperature and gas density is studied using the effective-medium approximation and density-functional theory. The results are compared with recent experiments.

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