Species formed at cuprite fracture surfaces; observation of O 1s surface core level shift |
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Authors: | Sarah L. Harmer Alan N. Buckley Liang-Jen Fan |
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Affiliation: | a Ian Wark Research Institute, ARC Special Research Centre for Particle and Material Interfaces, University of South Australia, Mawson Lakes, SA 5095, Australia b School of Chemistry, The University of New South Wales, Sydney, NSW 2052, Australia c National Synchrotron Radiation Research Center, Hsinchu 30076, Taiwan |
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Abstract: | ![]() Surfaces of mineral cuprite prepared by fracture under UHV have been characterised by synchrotron XPS and near-edge X-ray absorption spectroscopy before and after exposure to ambient air. Before exposure of the cuprite, the Cu 2p photoelectron and Cu L2,3-edge absorption spectra were consistent with CuI with very little d9 character. Surface-enhanced O 1s spectra from the unexposed mineral revealed a surface species, with binding energy 0.95 ± 0.05 eV below the principal cuprous oxide peak, assigned to under-coordinated oxygen. A second surface species, with binding energy about 1 eV higher than the principal peak, was assigned to either hydroxyl derived from chemisorbed water vapour or surface oxygen dimers produced by restructuring of the cuprite fracture surface. The width of the principal O 1s peak was 0.66 ± 0.02 eV. The observed Cu L3- and O K-edge absorption spectra were in good agreement with those simulated for the cuprite structure. After exposure of the fracture surface to ambient air, the low binding energy O 1s surface species was barely discernible, the original high binding energy O 1s surface species remained of comparable intensity, new intensity appeared at an even higher (∼1.9 eV) binding energy, and the Cu L2,3-edge spectrum indicated the presence of CuII, consistent with the formation of a thin surface layer of Cu(OH)2. |
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Keywords: | Copper oxides Surface electronic phenomena Synchrotron radiation photoelectron spectroscopy NEXAFS spectroscopy Density functional calculations |
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