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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 |
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author | Ahmed, M. H. M. Torrelles, X. Treacy, J.P.W. Hussain, H. Nicklin, C. Wincott, P. L. Vaughan, D. J. Thornton, G. Lindsay, R. |
author_facet | Ahmed, M. H. M. Torrelles, X. Treacy, J.P.W. Hussain, H. Nicklin, C. Wincott, P. L. Vaughan, D. J. Thornton, G. Lindsay, R. |
author_sort | Ahmed, M. H. M. |
collection | PubMed |
description | [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. |
format | Online Article Text |
id | pubmed-4729357 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2015 |
publisher | American Chemical
Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-47293572016-02-10 Geometry of α-Cr(2)O(3)(0001) as a Function of H(2)O Partial Pressure Ahmed, M. H. M. Torrelles, X. Treacy, J.P.W. Hussain, H. Nicklin, C. Wincott, P. L. Vaughan, D. J. Thornton, G. Lindsay, R. J Phys Chem C Nanomater Interfaces [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. American Chemical Society 2015-08-24 2015-09-17 /pmc/articles/PMC4729357/ /pubmed/26877825 http://dx.doi.org/10.1021/acs.jpcc.5b04607 Text en Copyright © 2015 American Chemical Society This is an open access article published under a Creative Commons Attribution (CC-BY) License (http://pubs.acs.org/page/policy/authorchoice_ccby_termsofuse.html) , which permits unrestricted use, distribution and reproduction in any medium, provided the author and source are cited. |
spellingShingle | Ahmed, M. H. M. Torrelles, X. Treacy, J.P.W. Hussain, H. Nicklin, C. Wincott, P. L. Vaughan, D. J. Thornton, G. Lindsay, R. Geometry of α-Cr(2)O(3)(0001) as a Function of H(2)O Partial Pressure |
title | Geometry of α-Cr(2)O(3)(0001) as a
Function of H(2)O Partial Pressure |
title_full | Geometry of α-Cr(2)O(3)(0001) as a
Function of H(2)O Partial Pressure |
title_fullStr | Geometry of α-Cr(2)O(3)(0001) as a
Function of H(2)O Partial Pressure |
title_full_unstemmed | Geometry of α-Cr(2)O(3)(0001) as a
Function of H(2)O Partial Pressure |
title_short | Geometry of α-Cr(2)O(3)(0001) as a
Function of H(2)O Partial Pressure |
title_sort | geometry of α-cr(2)o(3)(0001) as a
function of h(2)o partial pressure |
url | 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 |
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