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Extra info for Dynamical Phenomena at Surfaces, Interfaces and Superlattices: Proceedings of an International Summer School at the Ettore Majorana Centre, Erice, Italy, July 1–13, 1984

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P. W. Q. B. E. Hilliard: J. of Magnetism and Mag. S. K. R. P. Halperin: Physica 108B, 953 (1981) 1 5 1. K. S c h u lIe ran d C. M. ~= 1979, ed. U. L. R. K. Schuller: Phys. Rev. Lett. P. W. Barbee, Jr. B. McWhan: Phys. Rev. B24, 6193 (1981) 1 8 C. M. Fal co and 1. K. l i!!. 9. = Band Metals, ed. by W. Buckel and W. Weber (KernsforschungsanslageKarlsruhe, Germany, 1982) p. 283 19 J. Geerk, M. B. M. M. E. F. P. Flynn: J. Phys. F - Metal Phys. M. E. P. Flynn: J. Phys. F - Metal Phys. 12, L75 (1982) 22 G.

Fenter, priv. comm. M. G. R. K. W. T. Bl, 803 (1983) T. J. Chen,T. Sci. o. Hahn, M. Phys. T. O. Hahn, S. Yokohama, M. Sci. (1984) in press M. Henzler, P. T. G. -C. M. Lu in"Ordering in two dimensions" ed. K. Sinha (North Holland, New York 1980) p 113 andin"Chemistry and Physics of Solid Surfaces" ed. R. Vanselow (CRC Press, Boca Raton, Florida 1979), Vol. 2, p. -C. M. Lett. H. T. G. Lett. M. Fiz. Phys. M. -Cahn, Acta Metall. 27, 1085 (1979) H. Froitzheim, in "Electron Spectroscopy for Surface Analysis" ed.

If the overlayer has a superstructure, then only the over layer col umns are contributing to the extra spot. Their shape is therefore completely described within kinematic approximation given above (11,12). For overlayers without superstructure,the normal spots have to be used for 25 analysis. Here,at least two. lumns have to. be used, which have to. rding to. n. rder. nly few .. ne-. r example Au(llO) 2xl in ref. 10). n II (Kx'O) or 12 (K x ) =~I (Kx,Ky) dKy The two. nto. n. n). re to. n is meant.

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