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Structure of the quasi-one-dimensional Si(553)-Au surface: Gold dimer row and silicon honeycomb chain

Source: Phys. Rev. B 82, 075426 (2010); doi:10.1103/PhysRevB.82.075426

Published 26 August 2010

PACS
  • 68.35.bg
    Surface structure of semiconductors
  • 68.47.Fg
    Semiconductor surfaces
  • 61.05.cp
    X-ray diffraction (condensed matter structure determination)
  • YEAR: 2010
PUBLICATION DATA
ISSN:
1553-9644 (online)
Publisher:
AIP is a member of CrossRef APS
Wolfgang Voegeli, Toru Takayama, Tetsuroh Shirasawa, Makoto Abe, Kimitaka Kubo, and Toshio Takahashi
Institute for Solid State Physics, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa 277-8581, Japan

Koichi Akimoto
Department of Quantum Engineering, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan

Hiroshi Sugiyama
Photon Factory, High Energy Accelerator Research Organization, Tsukuba 305-0801, Japan
The Si(553)-Au surface consists of a periodic array of single steps and (111) terraces with a quasi-one-dimensional electronic structure. In this paper, the determination of the atomic structure of this surface with x-ray diffraction is reported. The gold coverage of the surface was measured to be 0.5 monolayer using x-ray fluorescence spectroscopy, i.e., two gold atoms per primitive unit cell. A structural model was constructed directly from the x-ray diffraction intensities with a step-by-step approach. First, the relative positions of the gold atoms were obtained from the Patterson map. Using the positions of the gold atoms, the deconvolution of the Patterson map was calculated and the positions of the gold atoms relative to the substrate were determined. Finally, the positions of the silicon atoms at the surface were obtained from a reconstruction of the electron density with an iterative phase and amplitude recovery algorithm. The main features of the structural model obtained in this way are a row of gold dimers on the (111) terraces in the topmost layer of the surface, and a honeycomb chain of silicon atoms near the step edge. Structural refinement of this model with the experimental diffraction data gave reasonable atomic positions and a chi2 value of 3.35, better than previous models. The model is related to the ×2  m1 model recently proposed by Krawiec [Phys. Rev. B 81, 115436 (2010)] but without the strong ×2 modulation. ©2010 The American Physical Society
History: Received 30 April 2010; published 26 August 2010
Permalink: http://link.aps.org/abstract/PRB/v82/e075426
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