School of Physics and Engineering, Zhengzhou University, Zhengzhou 450052, People's Republic of China.
J Phys Condens Matter. 2010 Jan 29;22(8):085001. doi: 10.1088/0953-8984/22/8/085001.
Using first-principles calculations, we present a comprehensive study on the atomic and electronic structures of metal adatoms (noble metals Ag, Au, Cu and alkali metals Li, Na, K) adsorbed on a [Formula: see text]-Ag (hereafter [Formula: see text]-Ag) surface. We found that adsorption of noble and alkali adatoms can induce significant structural changes in the topmost Ag layer. The most striking and interesting results are the immersion of the noble and Li adatoms into the substrate Ag layer and the finding of the most stable configurations with three adatoms incorporating into or being adsorbed on the surface dependent on their atomic radii. We also found that the almost empty two-dimensional free-electron-like band s1 and its band folding s1() of the original surface band s1 of the [Formula: see text]-Ag surface split into a gap at the surface Brillouin zone (SBZ) boundary with adsorption of an adatom. The two surface bands gradually move downwards and the s1 band is gradually filled with an increase of coverage. The s1 band is fully occupied with the largest band gap ∼ 0.25 eV between the s1 and s1() bands at the critical coverage of 0.14 monolayers (ML) [three adatoms in a [Formula: see text]-Ag (hereafter [Formula: see text]-Ag) unit cell], which corresponds to the most stable adsorption phase. Although the adsorption configurations are different, both the noble and alkali adatom adsorptions give rise to similar electronic structures at low coverages, indicating a free-electron-like character of the adsorption surfaces.
使用第一性原理计算,我们对金属原子(贵金属 Ag、Au、Cu 和碱金属 Li、Na、K)吸附在 [Formula: see text]-Ag(以下简称 [Formula: see text]-Ag)表面上的原子和电子结构进行了全面研究。我们发现,贵金属和碱金属原子的吸附可以诱导最顶层 Ag 层发生显著的结构变化。最显著和有趣的结果是贵金属和 Li 原子的浸入和碱金属原子的嵌入以及发现最稳定的配置,三个原子可以嵌入或吸附在表面上,这取决于它们的原子半径。我们还发现,[Formula: see text]-Ag 表面原始 s1 表面带的几乎空的二维自由电子样 s1 带和其带折叠 s1() 在吸附原子后在表面布里渊区(SBZ)边界处分裂成一个间隙。随着覆盖率的增加,两个表面带逐渐向下移动,s1 带逐渐被填满。在临界覆盖率为 0.14 单层(ML)[一个 [Formula: see text]-Ag 单元中的三个原子]时,s1 带完全被占据,s1 和 s1() 带之间的最大带隙约为 0.25 eV,这对应于最稳定的吸附相。尽管吸附构型不同,但贵金属和碱金属原子的吸附在低覆盖率下都会导致类似的电子结构,这表明吸附表面具有自由电子的特征。