Au enrichment and vertical relaxation of the Cu3Au(111) surface studied by normal-incidence x-ray standing waves

被引:9
作者
Bauer, O. [1 ]
Schmitz, C. H. [1 ]
Ikonomov, J. [1 ]
Willenbockel, M. [2 ]
Soubatch, S. [2 ]
Tautz, F. S. [2 ,3 ]
Sokolowski, M. [1 ]
机构
[1] Univ Bonn, Inst Phys & Theoret Chem, Wegelerstr 12, D-53115 Bonn, Germany
[2] Forschungszentrum Julich, Peter Grunberg Inst PGI 3, D-52425 Julich, Germany
[3] JARA, Fundamentals Future Informat Technol, D-52425 Julich, Germany
关键词
SCANNING-TUNNELING-MICROSCOPY; RECONSTRUCTED AU(111) SURFACE; SCATTERING MEASUREMENTS; GROWTH; RANGE; IDENTIFICATION; SPECTROSCOPY; COPPER; PTCDA; ORDER;
D O I
10.1103/PhysRevB.93.235429
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We have investigated the Cu3Au(111) surface, prepared under ultrahigh vacuum conditions by sputtering and annealing, by low energy electron diffraction (LEED), scanning tunneling microscopy (STM), x-ray photoelectron spectroscopy, and normal incidence x-ray standing waves (NIXSW). We find the surface to be depleted with Cu and enriched with Au at the same time, yielding a nominal Cu: Au ratio of 0.61:0.39 in the topmost layer. The STM images reveal that the first layer is nearly closely filled with atoms and contains a small amount of vacancies with an area concentration of about 5%. Together with the Au enrichment, these cause local short-range disorder of the Au p(2 x 2) reconstruction. From this data, the average stoichiometry of the p(2 x 2) surface unit cell is estimated at Cu2.22Au1.44 square(0.20) (instead of Cu3.00Au1.00 square(0.00) of the ideal surface; square denotes an atomic vacancy site). From NIXSW we find a significant outward relaxation of both the Cu and Au atoms of the topmost layer by 0.28 angstrom and 0.33 angstrom, which corresponds to 13% and 15% of the (111) bulk layer spacing of Cu3Au. We suggest that this originates from a widening of the first/second layer spacing, by 6.8% and 8.8% for the Cu and Au atoms, respectively, plus an additional rigid increase in the second/third layer spacing by 6.2%. We explain this by steric repulsions between Au atoms of the topmost layer, replacing smaller Cu atoms, and Au atoms in the second layer in combination with disorder. Finally, a lateral reconstruction, similar to that on the Au(111) surface, but with a much larger periodicity of 290 angstrom, is identified from LEED.
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页数:8
相关论文
共 36 条
[1]  
[Anonymous], 1987, J PHASE EQUILIB, DOI DOI 10.1007/BF02893155
[2]   SCANNING TUNNELING MICROSCOPY OBSERVATIONS ON THE RECONSTRUCTED AU(111) SURFACE - ATOMIC-STRUCTURE, LONG-RANGE SUPERSTRUCTURE, ROTATIONAL DOMAINS, AND SURFACE-DEFECTS [J].
BARTH, JV ;
BRUNE, H ;
ERTL, G ;
BEHM, RJ .
PHYSICAL REVIEW B, 1990, 42 (15) :9307-9318
[3]  
Bauer O., PHYS REV B UNPUB
[4]  
Bauer O., 2015, THESIS
[5]   Role of functional groups in surface bonding of planar π-conjugated molecules [J].
Bauer, Oliver ;
Mercurio, Giuseppe ;
Willenbockel, Martin ;
Reckien, Werner ;
Schmitz, Christoph Heinrich ;
Fiedler, Benjamin ;
Soubatch, Serguei ;
Bredow, Thomas ;
Tautz, Frank Stefan ;
Sokolowski, Moritz .
PHYSICAL REVIEW B, 2012, 86 (23)
[6]   Au(111)-Based Nanotemplates by Gd Alloying [J].
Corso, Martina ;
Fernandez, Laura ;
Schiller, Frederik ;
Enrique Ortega, Jose .
ACS NANO, 2010, 4 (03) :1603-1611
[7]   Chemical identification in the CU3Au(100) surface using scanning tunneling microscopy and first-principles calculations [J].
Dias, L. G. ;
Leitao, A. A. ;
Achete, C. A. ;
Blum, R. -P. ;
Niehus, H. ;
Capaz, Rodrigo B. .
SURFACE SCIENCE, 2007, 601 (23) :5540-5545
[8]   LONG-RANGE ORDER NEAR THE CU3AU(001) SURFACE BY EVANESCENT X-RAY-SCATTERING [J].
DOSCH, H ;
MAILANDER, L ;
REICHERT, H ;
PEISL, J ;
JOHNSON, RL .
PHYSICAL REVIEW B, 1991, 43 (16) :13172-13186
[9]  
Duvernay J., 2011, COMMUNICATION
[10]   RECONSTRUCTION OF THE PT(111) SURFACE - X-RAY-SCATTERING MEASUREMENTS [J].
GRUBEL, G ;
HUANG, KG ;
GIBBS, D ;
ZEHNER, DM ;
SANDY, AR ;
MOCHRIE, SGJ .
PHYSICAL REVIEW B, 1993, 48 (24) :18119-18139