Abstract
Atomic orbitais and an atomic approximation to the potential are used in the chemical pseudopotential secular equation to calculate the covalent binding energy of an adsorbed monolayer on a transition metal slab. After showing that the method provides a realistic description of the bulk metal band structure we examine the changes which accompany adsorption in various surface arrangements. For H on W(001), maximum coverage is found to correspond to occupation of all bridge sites (β 1 phase). Bridge sites also provide maximum covalent binding at lower coverage but energy differences between alternative sites are small (~0.2 eV per H atom) and ionic effects may stabilise adsorption above atoms in the β 2 phase. On Ni and Pt(001) both adsorbates bind most strongly above 4-fold hole sites, but for hydrogen energy differences between alternative sites are particularly small (~0.1 eV on Pt). Surface densities of states are presented and discussed in relation to photoemission spectra and the mechanism of the chemisorptive bond.
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