Abstract

Angular distributions and surface-phonon dispersion curves have been measured by He-atom scattering for clean Pt between T=160 and 373 K and for Pt-H(1\ifmmode\times\else\texttimes\fi{}1) at 160 K along the 〈110〉 and 〈112〉 azimuths. Inelastic-scattering intensities over a wide range of wave vectors are also reported for the clean surface. The results are analyzed with use of the distorted-wave Born approximation for a model potential describing the He-atom--Pt-surface potential. A set of 14 force constants adjusted to the bulk-phonon dispersion data cannot explain the measured time-of-flight spectra and the observed first-layer relaxation. However, by modifying at the surface the nearest-neighbor tangential force constants (${\ensuremath{\alpha}}_{1}^{\mathcal{'}\mathcal{'}}$=1.7${\ensuremath{\alpha}}_{1}^{b}$, and ${\ensuremath{\alpha}}_{1}^{\mathcal{'}}$=1.3${\ensuremath{\alpha}}_{1}^{b}$), the radial force constants (${\ensuremath{\beta}}_{1}^{\mathcal{'}\mathcal{'}}$=0.39${\ensuremath{\beta}}_{1}^{b}$), and the three-body force constant (${\ensuremath{\gamma}}_{1}^{\mathcal{'}\mathcal{'}}$=0.037${\ensuremath{\gamma}}_{1}^{b}$)--- where the superscripts \ensuremath{\parallel} and \ensuremath{\perp} denote forces within the surface plane and between the first and second planes, respectively---a good fit to all the data is achieved. The new surface force constants are discussed in terms of electronic-charge redistribution within the first layer.

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