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dc.creatorAtanasoska, Ljiljana L.
dc.creatorO'Grady, William E.
dc.creatorAtanasoski, Radoslav T.
dc.creatorPollak, Fred Hugo
dc.date.accessioned2021-02-09T08:33:28Z
dc.date.available2021-02-09T08:33:28Z
dc.date.issued1988
dc.identifier.issn0039-6028
dc.identifier.urihttps://cer.ihtm.bg.ac.rs/handle/123456789/4213
dc.description.abstractThe (110) and the (100) surfaces of RuO2 show well defined LEED patterns. The surface lattice dimensions agree within 5% with the values predicted from X-ray diffraction. Both surfaces undergo a series of reversible surface reconstructions which result in well defined LEED patterns. These states come about from the loss of surface oxygen and each oxygen and each state is characterized by a well defined O Ru ratio. The final state is an overlayer of Ru metal. Furthermore, nearly equal concentrations of RuO3 are observed on all of the surfaces regardless of the structure which is present. This suggests that RuO3 plays a significant role in the stability of RuO2 surfaces.sr
dc.language.isoensr
dc.publisherElseviersr
dc.relationUS Department of Energy, Contract No. DE-AC02-76CH00016sr
dc.rightsrestrictedAccesssr
dc.sourceSurface Sciencesr
dc.subjectsurface lattice dimensionssr
dc.subjectX-ray diffractionsr
dc.subjectreversible surface reconstructionssr
dc.subjectLEED patternssr
dc.subjectloss of surface oxygensr
dc.subjectoverlayer of Ru metalsr
dc.subjectRuO3sr
dc.subjectRuO2 surfacessr
dc.titleThe surface structure of RuO2: A leed, auger and XPS study of the (110) and (100) facessr
dc.typearticlesr
dc.rights.licenseARRsr
dcterms.abstractПоллак, Фред Хуго; Aтанасоска, Љиљана Л.; О'Градy, Wиллиам Е.; Aтанасоски, Радослав Т.;
dc.citation.volume202
dc.citation.issue1-2
dc.citation.spage142
dc.citation.epage166
dc.identifier.doi10.1016/0039-6028(88)90066-0
dc.identifier.scopus2-s2.0-0001070778
dc.type.versionpublishedVersionsr


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