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Valance-Band photoemission intensities in thorium dioxide

dc.contributor.authorEllis, W. P.en_US
dc.contributor.authorBoring, A. M.en_US
dc.contributor.authorAllen, J. W.en_US
dc.contributor.authorCox, L. E.en_US
dc.contributor.authorCowan, R. D.en_US
dc.contributor.authorPate, B. B.en_US
dc.contributor.authorArko, A. J.en_US
dc.contributor.authorLindau, I.en_US
dc.date.accessioned2006-04-07T20:39:56Z
dc.date.available2006-04-07T20:39:56Z
dc.date.issued1989-11en_US
dc.identifier.citationEllis, W. P., Boring, A. M., Allen, J. W., Cox, L. E., Cowan, R. D., Pate, B. B., Arko, A. J., Lindau, I. (1989/11)."Valance-Band photoemission intensities in thorium dioxide." Solid State Communications 72(7): 725-729. <http://hdl.handle.net/2027.42/27709>en_US
dc.identifier.urihttp://www.sciencedirect.com/science/article/B6TVW-46T4KND-139/2/90aa68cb5788febfefaa1185bd7e8332en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/27709
dc.description.abstractResonant photoemission spectra of the O 2p-derived valence band of insulating ThO2 are compared to linear muffin-tin orbital (LMTO) density-of-state (DOS) and XPS intensity calculations. At Th 5d corelevel threshold energies (85 [les] hv [les] 120 eV), resonance is greatest at the bottom of the O 2p band where calculated p/d hybrid states are greatest; p/f hybrid content is weak by comparison. We conclude that the dominant hybridization is between O 2p states and Th 6d.en_US
dc.format.extent435384 bytes
dc.format.extent3118 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherElsevieren_US
dc.titleValance-Band photoemission intensities in thorium dioxideen_US
dc.typeArticleen_US
dc.rights.robotsIndexNoFollowen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Physics, University of Michigan, Ann Arbor, MI 48109-1120, U.S.A.en_US
dc.contributor.affiliationotherUniversity of California, Los Alamos National Laboratory, Los Alamos, NM 87545, U.S.A.en_US
dc.contributor.affiliationotherUniversity of California, Los Alamos National Laboratory, Los Alamos, NM 87545, U.S.A.en_US
dc.contributor.affiliationotherUniversity of California, Los Alamos National Laboratory, Los Alamos, NM 87545, U.S.A.en_US
dc.contributor.affiliationotherUniversity of California, Los Alamos National Laboratory, Los Alamos, NM 87545, U.S.A.en_US
dc.contributor.affiliationotherStanford Synchrotron Radiation Laboratory, Stanford University, Stanford, CA 94305, U.S.A.en_US
dc.contributor.affiliationotherUniversity of California, Los Alamos National Laboratory, Los Alamos, NM 87545, U.S.A.en_US
dc.contributor.affiliationotherStanford Synchrotron Radiation Laboratory, Stanford University, Stanford, CA 94305, U.S.A.en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/27709/1/0000095.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1016/0038-1098(89)90682-0en_US
dc.identifier.sourceSolid State Communicationsen_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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