Please use this identifier to cite or link to this item: http://hdl.handle.net/2445/10823
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dc.contributor.authorRodríguez, José A.cat
dc.contributor.authorLiu, Pingcat
dc.contributor.authorGomes, J.cat
dc.contributor.authorNakamura, K.cat
dc.contributor.authorViñes Solana, Francesccat
dc.contributor.authorSousa Romero, Carmencat
dc.contributor.authorIllas i Riera, Francesccat
dc.date.accessioned2010-01-22T13:10:55Z-
dc.date.available2010-01-22T13:10:55Z-
dc.date.issued2005cat
dc.identifier.issn0163-1829cat
dc.identifier.urihttp://hdl.handle.net/2445/10823-
dc.description.abstractHigh-resolution photoemission and first-principles density-functional calculations were used to study the interaction of oxygen with ZrC(001) and VC(001) surfaces. Atomic oxygen is present on the carbide substrates after small doses of O 2 at room temperature. At 500 K , the oxidation of the surfaces is fast and clear features for Zr O x or V O x are seen in the O ( 1 s ) , Zr ( 3 d ) , and V ( 2 p 3 ∕ 2 ) core levels spectra, with an increase in the metal/carbon ratio of the samples. A big positive shift ( 1.3 – 1.6 eV ) was detected for the C 1 s core level in O ∕ Zr C ( 001 ) , indicating the existence of strong O ↔ C or C ↔ C interactions. A phenomenon corroborated by the results of first-principles calculations, which show a CZrZr hollow as the most stable site for the adsorption of O. Furthermore, the calculations also show that a C ↔ O exchange is exothermic on ZrC(001), and the displaced C atoms bond to CZrZr sites. In the O ∕ Zr C ( 001 ) interface, the surface C atoms play a major role in determining the behavior of the system. In contrast, the adsorption of oxygen induces very minor changes in the C ( 1 s ) spectrum of VC(001). The O ↔ V interactions are stronger than the O ↔ Zr interactions, and O ↔ C interactions do not play a dominant role in the O ∕ V C ( 001 ) interface. In this system, C ↔ O exchange is endothermic. VC(001) has a larger density of metal d states near the Fermi level than ZrC(001), but the rate of oxidation of VC(001) is slower. Therefore the O ∕ Zr C ( 001 ) and O ∕ V C ( 001 ) systems illustrate two different types of pathways for the oxidation of carbide surfaces.-
dc.format.extent11 p.cat
dc.format.mimetypeapplication/pdfeng
dc.language.isoengeng
dc.publisherThe American Physical Societycat
dc.relation.isformatofReproducció digital del document publicat en format paper, proporcionada per PROLA i http://dx.doi.org/10.1103/PhysRevB.72.075427cat
dc.relation.ispartofPhysical Review B, 2005, vol. 72, núm. 7, p. 075427-1-075427-11cat
dc.relation.urihttp://doi.org/10.1103/PhysRevB.72.075427-
dc.rights(c) The American Physical Society, 2005cat
dc.sourceArticles publicats en revistes (Ciència dels Materials i Química Física)-
dc.subject.classificationSuperfícies (Física)cat
dc.subject.classificationCiència dels materialscat
dc.subject.classificationElectrònica de l'estat sòlidcat
dc.subject.otherSurfaces (Physics)eng
dc.subject.otherMaterials scienceeng
dc.subject.otherSolid state electronicseng
dc.titleInteraction of oxygen with ZrC(001) and VC(001): Photoemission and first-principles studieseng
dc.typeinfo:eu-repo/semantics/articleeng
dc.typeinfo:eu-repo/semantics/publishedVersion-
dc.identifier.idgrec526710cat
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess-
Appears in Collections:Articles publicats en revistes (Ciència dels Materials i Química Física)

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