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Geometry of α-Cr(2)O(3)(0001) as a Function of H(2)O Partial Pressure
[Image: see text] Surface X-ray diffraction has been employed to elucidate the surface structure of α-Cr(2)O(3)(0001) as a function of water partial pressure at room temperature. In ultra high vacuum, following exposure to ∼2000 Langmuir of H(2)O, the surface is found to be terminated by a partially...
Autores principales: | , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical
Society
2015
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4729357/ https://www.ncbi.nlm.nih.gov/pubmed/26877825 http://dx.doi.org/10.1021/acs.jpcc.5b04607 |
Sumario: | [Image: see text] Surface X-ray diffraction has been employed to elucidate the surface structure of α-Cr(2)O(3)(0001) as a function of water partial pressure at room temperature. In ultra high vacuum, following exposure to ∼2000 Langmuir of H(2)O, the surface is found to be terminated by a partially occupied double layer of chromium atoms. No evidence of adsorbed OH/H(2)O is found, which is likely due to either adsorption at minority sites, or X-ray induced desorption. At a water partial pressure of ∼30 mbar, a single OH/H(2)O species is found to be bound atop each surface Cr atom. This adsorption geometry does not agree with that predicted by ab initio calculations, which may be a result of some differences between the experimental conditions and those modeled. |
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