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Pt(111)电极上一氧化碳吸附层的动态性质

The Dynamic Nature of CO Adlayers on Pt(111) Electrodes.

作者信息

Wei Jie, Amirbeigiarab Reihaneh, Chen Yan-Xia, Sakong Sung, Gross Axel, Magnussen Olaf M

机构信息

Institute of Experimental and Applied Physics, Kiel University, 24098, Kiel, Germany.

Hefei National Laboratory for Physical Sciences at Microscale, University of Science and Technology of China, Hefei, 230026, China.

出版信息

Angew Chem Int Ed Engl. 2020 Apr 6;59(15):6182-6186. doi: 10.1002/anie.201913412. Epub 2020 Feb 18.

Abstract

CO adlayers on Pt(111) electrode surfaces are an important electrochemical system and of great relevance to electrocatalysis. The potential-dependent structure and dynamics of these adlayers are complex and still controversial, especially in the CO pre-oxidation regime. We here employ in situ high-speed scanning tunneling microscopy for studying the surface phase behavior in CO-saturated 0.1 m H SO on the millisecond time scale. At potentials near the onset of CO pre-oxidation local fluctuations in the (2×2)-CO adlayer are observed, which increase towards more positive potentials. Above 0.20 V (vs. Ag/AgCl), this leads to an adlayer where CO apparently reside on every top site, but still exhibit a (2×2) superstructure modulation. We interpret this observation as a dynamic effect, caused by a small number of highly mobile point defects in the (2×2)-CO adlayer. As shown by density functional theory calculations, the CO lattice near such defects relaxes into a local (1×1) arrangement, which can rapidly propagate across the surface. This scenario, where a static (2×2) CO sublattice coexists with a highly dynamic sublattice of partially occupied top sites, explains the pronounced CO surface mobility during electrooxidation.

摘要

铂(111)电极表面上的一氧化碳吸附层是一个重要的电化学体系,与电催化密切相关。这些吸附层的电位依赖结构和动力学过程复杂且仍存在争议,特别是在一氧化碳预氧化区域。我们在此采用原位高速扫描隧道显微镜,在毫秒时间尺度上研究一氧化碳饱和的0.1 m硫酸中的表面相行为。在接近一氧化碳预氧化起始电位处,观察到(2×2)-一氧化碳吸附层的局部波动,随着电位更正,这种波动增加。在高于0.20 V(相对于Ag/AgCl)时,这导致形成一种吸附层,其中一氧化碳显然占据每个顶位,但仍呈现(2×2)超结构调制。我们将此观察结果解释为由(2×2)-一氧化碳吸附层中少量高度移动的点缺陷引起的动态效应。正如密度泛函理论计算所示,此类缺陷附近的一氧化碳晶格弛豫为局部(1×1)排列,可在表面迅速传播。这种静态(2×2)一氧化碳亚晶格与部分占据顶位的高度动态亚晶格共存的情况,解释了电氧化过程中一氧化碳显著的表面迁移率。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e443/7187359/5d03a425c968/ANIE-59-6182-g001.jpg

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