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dc.contributor.authorCOEY, JOHN MICHAEL DAVIDen
dc.date.accessioned2009-08-14T12:56:47Z
dc.date.available2009-08-14T12:56:47Z
dc.date.issued2005en
dc.date.submitted2005en
dc.identifier.citationJ. M. D. Coey, High temperature ferromagnetism in dilute ferromagnetic oxides, Journal of Applied Physics, 97, 10, 2005, 10D313en
dc.identifier.otherYen
dc.descriptionPUBLISHEDen
dc.description.abstractHigh temperature ferromagnetism in thin films of dilute magnetic oxides is a widespread phenomenon, of which there appear to be two sources. One is the contribution of the 3d dopant ions themselves, the other is related to crystal defects in the interface region. The latter contributes a magnetic moment of 100?400??B per square nanometer of substrate area, which is largely independent of film thickness or dopant concentration. It is suggested that the defects are two-electron or two-hole centers which have a spin triplet as ground state or low-lying excited state. HfO2, an example of the former, is ferromagnetic even when undoped. In ZnO or SnO2, examples of the latter, the magnetic dopant may stabilize the spin triplet by exchange.en
dc.description.sponsorshipThis work was supported by Science Foundation Ireland, as part of the CINSE Project. The author is grateful to many coworkers, including L. S. Dorneles, C. B. Fitzgerald, R. Gunning, J. G. Lunney, M. Moliner, P. Stamenov, M. Venkatesan, and Y. Zhou. M. Konno of Hitachi Science Systems Ltd. kindly took the STEM image.en
dc.format.extent10D313en
dc.format.mimetypeapplication/pdf
dc.language.isoenen
dc.relation.ispartofseriesJournal of Applied Physicsen
dc.relation.ispartofseries97en
dc.relation.ispartofseries10en
dc.rightsYen
dc.subjectPhysicsen
dc.titleHigh temperature ferromagnetism in dilute ferromagnetic oxidesen
dc.typeJournal Articleen
dc.type.supercollectionscholarly_publicationsen
dc.type.supercollectionrefereed_publicationsen
dc.identifier.peoplefinderurlhttp://people.tcd.ie/jcoeyen
dc.identifier.rssinternalid60486en
dc.identifier.urihttp://hdl.handle.net/2262/31832


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