Towards an understanding of surfactant action in the epitaxial growth of metals: The case of Sb on Ag (111)

Vincenzo Fiorentini1, Sabrina Oppo1, Matthias Scheffler2
1Dipartimento di Scienze, Fisiche dell' Università, Cagliari, Italy
2Theory, Fritz Haber Institute, Max Planck Society

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R. Kunkel, B. Poelsema, L.K. Verheij, G. Comsa: Phys. Rev. Lett.65, 733 (1990) M. Bott, T. Michely, G. Comsa: Surf. Sci.272, 161 (1992)

H. A. van der Vegt, H.M. van Pinxteren, M. Lohmeier, E. Vlieg, J.M.C. Thornton: Phys. Rev. Lett.68, 3335 (1992)

G. Rosenfeld, R. Servaty, C. Teichert, B. Poelsema, G. Comsa: Phys. Rev. Lett.71, 895 (1993)

S. Esch, M. Hohage, T. Michely, G. Comsa: Phys. Rev. Lett.72, 518 (1994)

S. Oppo, V. fiorentini, M. Scheffler, Phys. Rev. Lett.71, 2437 (1993)

S. Oppo, V. Fiorentini, M. Scheffler: MRS Proc.317 (1994) (in press)

J. Tersoff, A.W. Denier van der Gon, R. Tromp: Phys. Rev. Lett.72, 266 (1994)

M. Scheffler, V. Fiorentini, S. Oppo: InSurface Science II, ed. by R. MacDonald, E. Taglauer, K. Wandelt, Springer Proc. Phys. (Springer, Berlin, Heidelberg 1994) (in press)

Z. Zhang, M. Lagally: Phys. Rev. Lett.72, 693 (1994) We note that the description of surfactant action given in that paper does not apply to the present case. Such description of surfactant action is based on the inequalityV A-A>V A-S?V s-s connecting the adatom-adatom, adatom-surfactant, and surfactant-surfactant bond strengths (A=Ag, S=Sb). Surface-substitutional Sb repels Ag adatoms, which contradicts the assumptions of ZL. As a consequence of its surface-substitutional geometry, the surfactant will diffuse on the surface at a very much slower rate than the deposited Ag adatoms, which is reverse to the ZL suggestion. Thus, due to the substitutional adsorption of Sb, the general mechanism envisaged by ZL seems of limited relevance for this system

J. Vrijmoeth, H.A. van der Vegt, J.A. Meyer, E. Vlieg, R.J. Behm: Phys. Rev. Lett.72, 3842 (1994)

K. Meinel, M. Klaua, H. Bethge: Phys. Stat. Sol.110, 189 (1988)

H. Bethge: InKinetics of Ordering and Growth at Surfaces, ed. by M.G. Lagally (Plenum, New York 1990) p. 125

Oxford Dictionary of Physics (Oxford Univ. Press, Oxford 1988)

D.J. Eaglesham, F.C. Unterwald, D.C. Jacobson: Phys. Rev. Lett.70, 966 (1993)

G. Ehrlich, F.G. Hudda: J. Chem. Phys.44, 1039 (1966)

R.L. Schwöbel: J. Appl. Phys.40, 614 (1969)

R. Stumpf, M. Scheffler: Phys. Rev. Lett.72, 254 (1994)

R.Q. Hwang, J. Schröder, R. Günther, R.J. Behm: Phys. Rev. Lett.67, 3279 (1991)

R. Dreizler, E. Gross:Density Functional Theory, (Springer, Berlin, Heidelberg 1990)

Exchange-correlation energy by D.M. Ceperley, B.J. Alder: Phys. Rev. Lett.45, 566 (1980)

Parametrized by S. Wosko, L. Wilk, M. Nusair: J. Phys.58, 1200 (1980)

M. Methfessel: Phys. Rev. B38, 1537 (1988)

M. Methfessel, C. O. Rodriguez, O.K. Andersen: Phys. Rev. B40, 2009 (1989)

For surface studies see M. Methfessel, D. Hennig, M. Scheffler: Phys. Rev. B46, 4816 (1992)

V. Fiorentini, M. Methfessel, M. Scheffler: Phys. Rev. Lett.71, 1051 (1993)

J. Neugebauer, M. Scheffler: Phys. Rev.46, 16067 (1992)

Sb gains only about 0.2 eV by being lifted to the upper layer by exchange with asingle Ag from the upper layer. One thus expects that to create on-surface Sb at an appreciable rate from substitutional Sb, more upper-layer Ag neighbors are needed to provide sufficient coordination to the Sb atom being lifted

Indeed, recent STM results indicate the presence of Sb not only on the substrate, but also on the growing islands ([10], and private communication by J. Meyer)