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The structure of the CoS2 (100)-(1 × 1) surface

Z X Yu et al 2007 J. Phys.: Condens. Matter 19 156223 (9pp)   doi: 10.1088/0953-8984/19/15/156223  Help

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Z X Yu1,2, M A Van Hove2, S Y Tong2, David Wisbey3, Ya B Losovyj3,4, Ning Wu5, M Manno5, L Wang5, C Leighton5, W N Mei3,6 and P A Dowben3,7
1 School of Physics and Engineering, Zhongshan University, Guangzhou 510275, People's Republic of China
2 Department of Physics and Materials Science, City University of Hong Kong, Kowloon, Hong Kong SAR
3 Department of Physics and Astronomy and the Nebraska Center for Materials and Nanoscience, University of Nebraska-Lincoln, Lincoln, NE 68588-0111, USA
4 Center for Advanced Microstructures and Devices, Louisiana State University, 6980 Jefferson Highway, Baton Rouge, LA 70806, USA
5 Department of Chemical Engineering and Materials Science, University of Minnesota, Minneapolis, MN 55455, USA
6 Department of Physics, University of Nebraska at Omaha, Omaha, NE 68182-0266, USA
7 Author to whom any correspondence should be addressed
E-mail: pdowben@unl.edu

Abstract. Quantitative low-energy electron diffraction (LEED) has been used to determine the structure of the cubic CoS2 (100)-(1 × 1) surface. The clearly favoured structural model from the LEED analysis is the 1S-terminated (1 × 1) surface, in which the S–S dimer is intact and the terminal surface layer retains a complete S–Co–S sandwich structure. The surface S atoms move outwards towards the vacuum while the subsurface Co atoms move towards the bulk, by approximately 0.03 and 0.11 Å, respectively. In addition, the S atoms in the third sublayer relax outwards by about 0.12 Å, thus providing an indication of a stronger S–S dimer bond and a denser surface region. The complete atomic coordinates of the S–Co–S surface layers are determined in this analysis.

A corrigendum for this article has been published in 2007 J. Phys.: Condens. Matter 19 249001

Print publication: Issue 15 (16 April 2007)
Received 8 January 2007, in final form 23 January 2007
Published 26 March 2007

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