Submonolayer growth of Pd on Cu(111) studied by scanning tunneling microscopy

被引:78
作者
Aaen, AB
Laegsgaard, E
Ruban, AV
Stensgaard, I [1 ]
机构
[1] Univ Aarhus, Ctr Atom Scale Mat Phys, DK-8000 Aarhus C, Denmark
[2] Univ Aarhus, Inst Phys & Astron, DK-8000 Aarhus, Denmark
[3] Tech Univ Denmark, Ctr Atom Scale Mat Phys, DK-2800 Lyngby, Denmark
[4] Tech Univ Denmark, Dept Phys, DK-2800 Lyngby, Denmark
关键词
copper; epitaxy; growth; scanning tunneling microscopy; single crystal surfaces;
D O I
10.1016/S0039-6028(98)00124-1
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The growth mode of sub-monolayer amounts of Pd on Cu(111) in the temperature range - 80-300 degrees C has been investigated by scanning tunneling microscopy (STM), Rutherford backscattering spectroscopy (RBS) and Auger electron spectroscopy (AES). Below approximate to 100 degrees C, the Pd induced phase nucleates at ascending steps in fingered brims and, on large terraces, in fingered islands. The lack of order suggests that the brims and islands are a disordered alloy formed by exchange between Pd and Cu from the layer underneath. For temperatures exceeding approximate to 160 degrees C, Cu is dug out from the surface in extended, monolayer deep pits, and concurrently, the brims and islands increase in height by one layer. High-resolution STM images of brims and islands in this phase are interpreted as evidence for Cu capping. For Pd evaporation at temperatures of 220-300 degrees C, the surface is characterized by the appearance of individual Pd atoms substituted into the first layer and the presence of subsurface Pd. A short-range order that excludes the population of nearest-neighbour, in-plane sites is revealed by pair-correlation analysis. The Pd atoms form bands in the upper terrace next to steps. These bands are surprisingly stable against further diffusion, possibly due to an attractive interaction with second- and third-nearest (in-plane) neighbours and with subsurface Pd. The lack of any ordering is explained, based on a calculation of the surface energy. Once the population of nearest-neighbour sites is excluded, there is practically no energy gain by ordering. (C) 1998 Elsevier Science B.V. All rights reserved.
引用
收藏
页码:43 / 56
页数:14
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