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dc.contributor.authorWang, Jia-Binen_US
dc.contributor.authorWu, Kuei-Chingen_US
dc.contributor.authorMi, Jyun-Weien_US
dc.contributor.authorLuo, Chih-Weien_US
dc.contributor.authorWu, Kaung-Hsiungen_US
dc.contributor.authorUen, Tzeng-Mingen_US
dc.contributor.authorLin, Jiunn-Yuanen_US
dc.contributor.authorJuang, Jenh-Yihen_US
dc.contributor.authorLiu, Shiu-Jenen_US
dc.date.accessioned2015-07-21T08:29:14Z-
dc.date.available2015-07-21T08:29:14Z-
dc.date.issued2015-02-01en_US
dc.identifier.issn0947-8396en_US
dc.identifier.urihttp://dx.doi.org/10.1007/s00339-014-8788-2en_US
dc.identifier.urihttp://hdl.handle.net/11536/124188-
dc.description.abstractMarked room-temperature ferromagnetism (RTFM) was obtained in carbon- and nitrogen-doped rutile powders. X-ray photoelectron spectroscopy measurements revealed the co-existence of considerable densities of states near the Fermi level () and oxygen vacancies primarily induced by C- and N-doping. Density functional theory calculations showed that the local moments responsible for the observed RTFM in N-doped were primarily attributed to the partially populated, spin-polarized Ti band. In addition to the unfilled Ti band, the spin splitting in C states near in C-doped , which may be induced by the interaction between the C impurities and neighboring oxygen ions, results in Stoner band-splitting-type ferromagnetism.en_US
dc.language.isoen_USen_US
dc.titleRoom-temperature ferromagnetism in carbon- and nitrogen-doped rutile TiO2en_US
dc.typeArticleen_US
dc.identifier.doi10.1007/s00339-014-8788-2en_US
dc.identifier.journalAPPLIED PHYSICS A-MATERIALS SCIENCE & PROCESSINGen_US
dc.citation.volume118en_US
dc.citation.spage725en_US
dc.citation.epage731en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000348300100044en_US
dc.citation.woscount0en_US
Appears in Collections:Articles