Helium Atom Scattering from Surfaces by E. Hulpke (auth.), Dr. E. Hulpke (eds.) PDF

By E. Hulpke (auth.), Dr. E. Hulpke (eds.)

High answer helium atom scattering could be utilized to check a few fascinating houses of strong surfaces with nice sensitivity and accuracy. This ebook treats intimately experimental and theoretical facets ofthis procedure in addition to all present functions in floor technological know-how. the person chapters - all written through specialists within the box - are dedicated to the research of floor constitution, disorder shapes and concentrations, the interplay power, collective and localized floor vibrations at low energies, section transitions and floor diffusion. during the last decade helium atom scattering has won frequent recognitionwithin the outside technology group. issues in its favour are comprehensiveunderstanding of the scattering concept and the provision of well-tested approximation to the rigorous concept. This ebook may be worthy to floor scientists wishing to make an educated judgement at the real and power features of this method and its results.

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However, this simple replacement does not account for the fact that the Fourier components VG(z) decay more rapidly with z than V0 (z), as displayed in Eqs. 29-31) below for a sum of pairwise potentials. More accurately, the G Fourier component of ((R) should be multiplied by exp((/3- f3G)z]. A potential of this type has been constructed, for instance, by Kirsten et al. 59] for the reconstructed surface of Pt(111)(1 x 2). For insulators, a better semi-empirical form of the potential may be given by a pairwise sum, with most of the parameters determined from a knowledge of the He-atom (or He-ion) pair potentials.

The use of resonant enhancement places additional demands on both the apparatus and the process of data-taking. The apparatus must provide sufficient kinematic variability - in the form of a continuously variable total scattering angle and/ or a continuously variable beam energy - to track the resonances through L1E(L1K)-space. The bound state energies must either be known or they must be measured prior to undertaking the inelastic scattering measurements. Data- 19 <110> LiF (001) 9i =50. ci ...

123, 338 (1982) U. C. Levi, R. E. Tommei: Surf. Sci. C. Levi, H. Suhl: Surf. Sci. 88, 221 (1979) G. R. Manson: Surf. Sci. 80, 532 (1979) G. Benedek, N. Garcia: Surf. Sci. 80, 543 (1979) G. Boato, P. Cantini, R. Tartarek: Phys. Rev. Lett. 5 See T. Engel, K. H. 6 lar Beam Diffraction, Springer Tracts in Modern Physics, Vol. 91 (Springer, Berlin, Heidelberg 1981) C. Chiroli, A. C. Levi: Surf. Sci. 7 N. R. Hill, V. Celli: Surf. Sci. 8 C. E. H. Weare: Solid State Commun. 10 N. Garcia, F. 0. Goodman, V.

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