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Phys. Rev. B 52, 16796–16802 (1995)

p(n×1) superstructures of Pb on Cu(110)

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C. Nagl, M. Pinczolits, M. Schmid, and P. Varga
Institut für Allgemeine Physik, Technische Universität Wien, A-1040 Wien, Austria

I. K. Robinson
Department of Physics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801

Received 28 June 1995; published in the issue dated 15 December 1995

The structures of the p(n×1) superstructures (n=4, 5, and 9) of Pb on Cu(110) in the coverage range between FTHETA=0.75 and 0.8 are revealed by atomically resolved scanning tunneling microscopy. All three superstructures are formed by substitution of every nth row of Cu atoms (n=4, 5, and 9) in the [001] direction by Pb atoms. The Pb atoms in between are lined up in the [1¯10] direction. The p(4×1) structure appears in two different modifications: one with substitutional rows of Pb atoms and one with a simple overlayer structure without substituted rows of Cu atoms. Alternating succession of these two modifications results in p(12×1) domains. It is further shown that the p(9×1) structure is not a succession of p(4×1) and p(5×1) but a superstructure on its own. The p(5×1) structure proposed here agrees with previous x-ray-diffraction data at least as well as the quasihexagonal model proposed earlier. We have, in addition, identified the nature of the phase that has been described incommensurate obtained by desorption of Pb upon annealing above 600 K.

© 1995 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.52.16796
DOI:
10.1103/PhysRevB.52.16796
PACS:
68.55.Jk, 61.16.Ch, 68.35.Bs