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从头算研究 c(2×2) CO 覆盖层在 Ag(001)表面的声子色散。

Ab initio calculations of the dispersion of surface phonons of a c(2 × 2) CO overlayer on Ag(001).

机构信息

Department of Physics, University of Central Florida, Orlando, FL 32816, USA.

出版信息

J Phys Condens Matter. 2010 Oct 6;22(39):395001. doi: 10.1088/0953-8984/22/39/395001. Epub 2010 Aug 25.

Abstract

We examine the phonon dispersion of c(2 × 2)-CO on Ag(001) by applying density functional perturbation theory with the generalized-gradient approximation. Our calculations indicate that the c(2 × 2)-CO overlayer on Ag(001) is dynamically stable. We find that the bond length of CO is expanded and its stretch mode (ν(1)) softened by ∼ 9 meV upon adsorption on Ag(001), in excellent agreement with experiments. We show that ν(1) at [Formula in text] alone cannot gauge the metal-CO interaction since it is not entirely determined by the C-O intramolecular force constant. Further softening of ν(1) on Ag(001) is obtained outside [Formula in text], indicative of CO-CO interactions even at a distance of ∼ 4 Å. The frequency of the Ag-CO stretch mode (ν(2)) is ∼ 30 meV and it is nearly dispersionless, implying that the perturbation corresponding to this mode is short-ranged. The frustrated rotation mode of CO (ν(3)) overlaps with the bulk band and mixes with substrate modes inside the SBZ, suggesting this as one of the key features for the enhanced diffusivity of CO on Ag surfaces over that on Cu surfaces. The frustrated translation mode of CO (ν(4)) is everywhere below ∼ 2.8 meV and therefore mixes with substrate modes in the region of the SBZ around [Formula in text]. Depending on the q vector, vertical and in-plane surface modes may soften or stiffen with respect to their counterpart on clean Ag(001). Although the response of most Ag(001) modes to CO adsorption is similar to that of corresponding Cu(001) modes, there are some contrasting features between the dynamics of the two surfaces concerning the changes in the surface force constants and mixing of S(6) with ν(3) on Ag(001).

摘要

我们通过应用密度泛函微扰理论和广义梯度近似来研究 c(2 × 2)-CO 在 Ag(001)上的声子色散。我们的计算表明,c(2 × 2)-CO 覆盖层在 Ag(001)上是动态稳定的。我们发现,CO 的键长在吸附到 Ag(001)上时被扩展,其伸缩模式(ν(1))被软化约 9 meV,与实验结果非常吻合。我们表明,由于 ν(1)不完全由 C-O 分子内力常数决定,因此仅在 [Formula in text] 处的 ν(1)不能衡量金属-CO 相互作用。在 [Formula in text] 之外,ν(1)进一步软化,表明即使在约 4 Å 的距离处,CO-CO 相互作用也存在。Ag-CO 伸缩模式(ν(2))的频率约为 30 meV,几乎没有色散,这意味着对应于该模式的扰动是短程的。CO 的受挫旋转模式(ν(3))与体带重叠,并在 SBZ 内与基质模式混合,这表明这是 CO 在 Ag 表面上扩散性增强的关键特征之一,超过了在 Cu 表面上的扩散性。CO 的受挫平移模式(ν(4))在任何地方都低于约 2.8 meV,因此在 SBZ 围绕 [Formula in text] 的区域内与基质模式混合。根据 q 向量,垂直和平面表面模式相对于清洁 Ag(001)上的对应模式可能会软化或变硬。尽管大多数 Ag(001)模式对 CO 吸附的响应与相应的 Cu(001)模式相似,但在两个表面的动力学方面,存在一些对比特征,涉及到表面力常数的变化和 S(6)与 ν(3)在 Ag(001)上的混合。

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