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dc.contributor.authorHuang, DJen_US
dc.contributor.authorJeng, HTen_US
dc.contributor.authorChang, CFen_US
dc.contributor.authorGuo, GYen_US
dc.contributor.authorChen, Jen_US
dc.contributor.authorWu, WPen_US
dc.contributor.authorChung, SCen_US
dc.contributor.authorShyu, SGen_US
dc.contributor.authorWu, CCen_US
dc.contributor.authorLin, HJen_US
dc.contributor.authorChen, CTen_US
dc.date.accessioned2019-04-03T06:39:49Z-
dc.date.available2019-04-03T06:39:49Z-
dc.date.issued2002-11-01en_US
dc.identifier.issn1098-0121en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.66.174440en_US
dc.identifier.urihttp://hdl.handle.net/11536/28394-
dc.description.abstractWith measurements of the magnetic circular dichroism and band-structure calculations in the local spin density approximation (LSDA+U) approach, we revealed that the orbital moment of O in CrO2 is ferromagnetically coupled to that of Cr, whereas the spin moment of O is antiferromagnetically coupled to that of Cr. Spin and orbital magnetic moments of Cr and O are enhanced as Coulomb interaction energy U increases. Comparing the magnetic circular diachromism data with the LSDA+U calculations, we conclude that it is essential to include the on-site Coulomb energy for adequately describing the orbital magnetic moments of CrO2.en_US
dc.language.isoen_USen_US
dc.titleOrbital magnetic moments of oxygen and chromium in CrO2en_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.66.174440en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume66en_US
dc.citation.issue17en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000179611700084en_US
dc.citation.woscount26en_US
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