Abstract

The K/sup +/-W ion-atom scattering potential is calculated with the Hartree-Fock-Slater linear combination of atomic orbitals (HFS-LCAO) method. For hyperthermal (10--100 eV) K/sup +/ scattering from a W(110) surface, classical-trajectory calculations are performed, where the K/sup +/-W(110) ion-surface potential is represented by a sum of pairwise-calculated (HFS-LCAO) K/sup +/-W potentials. The results of these classical-trajectory calculations are compared with experiment and with the results of similar trajectory calculations using a sum of Ziegler-Biersack-Littmarck ''universal'' pair potentials. From these comparisons, it turns out that the HFS-LCAO pair potential is able to reproduce well on-top-site hyperthermal K/sup +/ scattering from a W(110) surface, contrary to the Ziegler-Biersack-Littmarck potential, which clearly does not work very well in this low-energy range. The inability of the HFS-LCAO pair potential to give a proper description of K/sup +/ scattering from the hollow site of the W(110) surface unit cell can be ascribed to the breakdown of a summation of pair potentials. This is clear from the difference between the sum of the calculated K/sup +/-W ion-atom potentials and a calculated K/sup +/-W/sub 5/ ion-cluster potential, the cluster representing the W(110) surface. The ion-cluster calculations indicate an extra repulsion of about 10% at the center of themore » W(110) surface unit cell. This extra hollow-site repulsion can be explained by analyzing the properties of the exchange (Pauli, Born) repulsions between the K/sup +/ ion and (i) one W atom and (ii) the W(110) surface (W/sub 5/ cluster) at the hollow site.« less

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