Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/2509
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dc.contributorDepartment of Applied Physics-
dc.contributorMaterials Research Centre-
dc.creatorGu, YH-
dc.creatorWang, Y-
dc.creatorChen, F-
dc.creatorChan, HLW-
dc.creatorChen, W-
dc.date.accessioned2014-12-11T08:27:07Z-
dc.date.available2014-12-11T08:27:07Z-
dc.identifier.issn0021-8979-
dc.identifier.urihttp://hdl.handle.net/10397/2509-
dc.language.isoenen_US
dc.publisherAmerican Institute of Physicsen_US
dc.rights© 2010 American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the American Institute of Physics. The following article appeared in Y.H. Gu et al., J. Appl. Phys. 108, 094112 (2010) and may be found at http://link.aip.org/link/?jap/108/094112en_US
dc.subjectBismuth compoundsen_US
dc.subjectDielectric lossesen_US
dc.subjectDielectric polarisationen_US
dc.subjectElectrical resistivityen_US
dc.subjectFerroelectric ceramicsen_US
dc.subjectFerromagnetic materialsen_US
dc.subjectLeakage currentsen_US
dc.subjectMultiferroicsen_US
dc.subjectRemanenceen_US
dc.subjectStoichiometryen_US
dc.subjectX-ray diffractionen_US
dc.titleNonstoichiometric BiFe₀.₉Ti₀.₀₅O₃multiferroic ceramics with ultrahigh electrical resistivityen_US
dc.typeJournal/Magazine Articleen_US
dc.description.otherinformationAuthor name used in this publication: Helen Lai Wah Chanen_US
dc.description.otherinformationAuthor name used in this publication: Wan Ping Chenen_US
dc.identifier.spage1-
dc.identifier.epage5-
dc.identifier.volume108-
dc.identifier.issue9-
dc.identifier.doi10.1063/1.3506526-
dcterms.abstractBiFeO₃, BiFe₀.₉Ti₀.₁O₃, and BiFe₀.₉Ti₀.₀₅O₃ceramics of relatively high perovskite phase content were prepared for a comparison study. While both BiFe₀.₉Ti₀.₁O₃ and BiFe₀.₉Ti₀.₀₅O₃ exhibit similarly improved weak ferromagnetism over BiFeO₃, there exists a major difference in the x-ray diffraction patterns of BiFe₀.₉Ti₀.₁O₃and BiFe₀.₉Ti₀.₀₅O₃ , and the leakage current of BiFe₀.₉Ti₀.₀₅O₃is decreased by five orders of magnitude from that of BiFe₀.₉Ti₀.₁O₃. With an ultrahigh electrical resistivity, over 1 x 10¹⁴Ωcm, BiFe₀.₉Ti₀.₀₅O₃ ceramic displays an especially low dielectric loss, 0.015 at 100 Hz, a remanent polarization Pힲ of 0.23 μC/cm² and a remanent magnetization Mힲ of 0.13 emu/g at room temperature. It is proposed that the Fe-deficiency in BiFe₀.₉Ti₀.₀₅O₃ decreases the amount of Fe²⁺ and leads to the ultrahigh electrical resistivity. Nonstoichiometric compositions should receive more attention for developing high quality BiFeO₃ multiferroic materials.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of applied physics, 1 Nov. 2010, v. 108, no. 9, 094112, p. 1-5-
dcterms.isPartOfJournal of applied physics-
dcterms.issued2010-11-01-
dc.identifier.isiWOS:000284270900113-
dc.identifier.scopus2-s2.0-78649286653-
dc.identifier.eissn1089-7550-
dc.identifier.rosgroupidr52498-
dc.description.ros2010-2011 > Academic research: refereed > Publication in refereed journal-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_IR/PIRAen_US
dc.description.pubStatusPublisheden_US
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