The chemisorption of a hydrogen atom on a transition-metal surface is treated theoretically on the basis of the Anderson Hamiltonian in Hartree-Fock approximation, which includes the interelectronic interaction within the $1s$ orbital. One-electron theory is shown to be inadequate for this problem. The localized states which may occur are discussed. A simple expression for the chemisorption energy $\Delta E$ is obtained, and a variational method is given for obtaining its self-consistent value. The metal eigenfunctions enter $\Delta E$ only through a function $\Delta \left(\epsilon \right)$, and the foregoing results are exemplified and applied when this function is semielliptical. When the band is half-filled, a single analytic formula for the one-electron part of $\Delta E$ is obtained, in accord with the Kohn-Majumdar theorem. With some further assumptions, $\Delta E$ and the charge on the atom are calculated for adsorption on Ti, Cr, Ni, and Cu. The values of the hopping integral between the $1s$ orbital and a neighboring metal $d$ orbital required to fit the experimental $\Delta E$ are found to be similar and are reasonable. The correct prediction that ${\left|\Delta E\right|}_{\mathrm{Ni}}>{\left|\Delta E\right|}_{\mathrm{Cu}}$ is believed to be significant. A suggestive correlation is found between observations of catalytic ortho-para hydrogen interconversion on Pd-Au alloys and a rigidband calculation of $\Delta E$.

• Received 15 July 1968

DOI:https://doi.org/10.1103/PhysRev.178.1123