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氧在(1×1)和(2×1)重构 C(111)表面上的吸附:密度泛函理论研究。

Oxygen adsorption on the (1×1) and (2×1) reconstructed C(111) surfaces: a density functional theory study.

机构信息

Ion Implantation and Surface Studies Program, University of the Witwatersrand, Private Bag 3, Wits 2050, Johannesburg, South Africa.

出版信息

J Phys Condens Matter. 2010 Jul 7;22(26):265007. doi: 10.1088/0953-8984/22/26/265007. Epub 2010 Jun 15.

Abstract

The structural and electronic properties, stability, optimum coverage and workfunction of oxygen atoms at different sites on the (1×1) unreconstructed and the (2×1) reconstructed C(111) surfaces have been investigated using density functional theory. Oxygen atoms prefer on-top sites on the C(111)-(1×1) surface, with an optimum coverage of 1/3 monolayers (ML), while on the (2×1) reconstructed surface, bridge sites are preferred with a coverage of 1/2 ML. With increasing oxygen coverage greater than 1/3 ML on the (1×1) surface, a repulsive interaction develops between the oxygen atoms, while for the (2×1) surface such a repulsive interaction occurs for coverages greater than 0.5 ML. For both surfaces, the workfunction initially increases with oxygen adsorption relative to that of each of the clean surfaces, reaching about ∼6 eV and then decreasing slightly at full monolayer coverage. Minimal buckling of the upper π-bonded chains and no dimerization of the clean (2×1) reconstructed surface was observed. An average valence band width of ∼21 eV occurs, and a surface state associated with the (2×1) surface reconstruction was established at ∼-2.5 eV. In addition, O 2s states were established at around -21 eV for the (1×1) surface and at ∼-22.5 eV on the (2×1) surface. These corresponded to similarly located C 2s states at -21.25 eV for both (1×1) and (2×1) surfaces. O 2p states were observed at the Fermi level, ∼-1.25, -2.5, -4.0, and ∼-7.5 eV on the (1×1) surface, and at ∼-2.5 eV, between -4 and -5 eV and at ∼-7.5 eV on the (2×1) surface.

摘要

使用密度泛函理论研究了不同位置氧原子在(1×1)未重构和(2×1)重构 C(111)表面上的结构和电子性质、稳定性、最佳覆盖度和功函数。氧原子优先占据 C(111)-(1×1)表面的顶位,最佳覆盖度为 1/3 单层(ML),而在(2×1)重构表面上,桥位优先,覆盖度为 1/2 ML。随着氧覆盖度的增加,(1×1)表面上大于 1/3 ML 的氧原子之间会产生排斥相互作用,而对于(2×1)表面,当覆盖度大于 0.5 ML 时会发生这种排斥相互作用。对于这两种表面,与清洁表面相比,功函数在初始阶段随氧吸附而增加,达到约 6 eV 左右,然后在单层覆盖时略有下降。上π键链的最小翘曲和清洁(2×1)重构表面的二聚化都没有观察到。平均价带宽度约为 21 eV,与(2×1)表面重构相关的表面态位于约-2.5 eV。此外,对于(1×1)表面,O 2s 态位于约-21 eV,对于(2×1)表面,O 2s 态位于约-22.5 eV。对于这两种表面,相应的 C 2s 态位于-21.25 eV。在(1×1)表面,O 2p 态位于费米能级附近,约为-1.25、-2.5、-4.0 和-7.5 eV,而在(2×1)表面,位于约-2.5 eV、-4 至-5 eV 和-7.5 eV 之间。

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