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H.L. Davis, J.B. Hannon, K.B. Ray, and E.W. Plummer, Phys. Rev. Lett. 68, 2632 (1992).
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Ph. Hofmann, K. Pohl, R. Stumpf, and E.W. Plummer, Phys. Rev. B 53, 13 715 (1996).
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S. Lizzit, K. Pohl, A. Baraldi, G. Comelli, V. Fritzsche, E.W. Plummer, R. Stumpf, and Ph. Hofmann, Phys. Rev. Lett. 81, 3271 (1998).
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0009040354
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A.M. Begley, R.G. Jordan, W.M. Temmerman, and P.J. Durham, Phys. Rev. B 41, 11 780 (1990).
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23
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0001300239
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These different bonding characters between (Formula presented) and (Formula presented) would provide the different driving force for the oscillatory multilayer relaxation observed in both surfaces. In (Formula presented) the “chemical” concept based on a bond-order bond-length consideration [see Ref. 22).
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Feibelman, P.1
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24
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0001303056
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The origin of the anisotropic bonding in Be was explained by the absence of core p orbitals which results in the compactness of the valence p orbitals and the relative effectiveness of the s-p hybridization. See M.Y. Chou, P.K. Lam, and M.L. Cohen, Phys. Rev. B 28, 4179 (1983).
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R. Stumpf, J. B. Hannon, P. J. Feibelman, and E. W. Plummer, in Electronic Surface and Interface States on Metallic Systems, edited by E. Bertel and M. Donath (World Scientific, Singapore, 1995), pp. 151-170.
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27
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0001041806
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Such different bonding characters between (Formula presented) and Be(0001) are consistent with the conclusion from the electron energy loss spectroscopy data of the surface phonon dispersions of both surfaces, i.e., the bonding at (Formula presented) is more complicated than the free-electron-like bonding at Be(0001). See J.B. Hannon, E.J. Mele, and E.W. Plummer, Phys. Rev. B 53, 2090 (1996).
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0031124908
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Ph. Hofmann and E.W. Plummer, Surf. Sci. 377, 330 (1997).
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Plummer, E.1
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