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Phys. Rev. B 79, 115417 (2009) [7 pages]

Surface structure of liquid Bi and Sn: An x-ray reflectivity study

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P. S. Pershan1, S. E. Stoltz1, Oleg G. Shpyrko2, Moshe Deutsch3, Venkatachalapathy S. K. Balagurusamy1, Mati Meron4, Binhua Lin4, and Reinhard Streitel1
1Department of Physics and SEAS, Harvard University, Cambridge, Massachusetts 02138, USA
2Department of Physics, University of California–San Diego, San Diego, La Jolla, California 92093, USA
3Department of Physics and Institute of Nanotechnology and Advanced Materials, Bar-Ilan University, Ramat-Gan 52900, Israel
4CARS, University of Chicago, Chicago, Illinois 60637, USA

Received 10 November 2008; revised 12 January 2009; published 13 March 2009

X-ray reflectivity measurements of the liquid Bi surface are presented and analyzed together with previous liquid Sn results. Published measurements on liquid Ga, In, and K all exhibit a single strong maximum at a wave-vector transfer of the order of the reciprocal of an atomic-diameter, due to surface-induced layering. In contrast, both Sn and Bi exhibit—in addition—a weak broad peak at much smaller wave-vector transfers. This feature is an unambiguous signature of an enhanced electron density in the near-surface region. Possible ways of modeling this enhancement are presented. Once the different surface-roughening effects of thermal capillary waves are accounted for, the surface structure factors of Sn and Bi are remarkably similar. The principal difference between the two is that the depth of the layering below the surface is more than ∼40% larger for Bi than for Sn. This is considerably larger than the ratio of their covalent radii which is only ∼10%. No theoretical explanation can be offered at this time for the surface structure difference between Sn and Bi and other elemental liquid metals studied to date: Ga, In, and K.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.79.115417
DOI:
10.1103/PhysRevB.79.115417
PACS:
68.03.−g, 68.35.Ct, 61.25.Mv