Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/4349
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dc.contributorDepartment of Applied Physics-
dc.creatorYuan, GL-
dc.creatorOr, DSW-
dc.creatorLiu, J-
dc.creatorLiu, ZG-
dc.date.accessioned2014-12-11T08:23:33Z-
dc.date.available2014-12-11T08:23:33Z-
dc.identifier.issn0003-6951-
dc.identifier.urihttp://hdl.handle.net/10397/4349-
dc.language.isoenen_US
dc.publisherAmerican Institute of Physicsen_US
dc.rights© 2006 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 G. L. Yuan et al., Appl. Phys. Lett. 89, 052905 (2006) and may be found at http://apl.aip.org/applab/v89/i5/p052905_s1en_US
dc.subjectBismuth compoundsen_US
dc.subjectNeodymium compoundsen_US
dc.subjectMultiferroicsen_US
dc.subjectFerroelectric ceramicsen_US
dc.subjectFerromagnetic materialsen_US
dc.subjectFerroelectric transitionsen_US
dc.subjectCrystal structureen_US
dc.subjectMagnetisationen_US
dc.subjectMagnetoelectric effectsen_US
dc.subjectNeel temperatureen_US
dc.subjectDielectric polarisationen_US
dc.subjectX-ray diffractionen_US
dc.titleStructural transformation and ferroelectromagnetic behavior in single-phase Bi[sub 1-x]Nd[sub x]FeO₃multiferroic ceramicsen_US
dc.typeJournal/Magazine Articleen_US
dc.description.otherinformationAuthor name used in this publication: Siu Wing Oren_US
dc.identifier.spage1-
dc.identifier.epage3-
dc.identifier.volume89-
dc.identifier.issue5-
dc.identifier.doi10.1063/1.2266992-
dcterms.abstractSingle-phase Bi[sub 1-x]Nd[sub x]FeO₃ (BNFO[sub x]) (x = 0–0.2) multiferroic ceramics were prepared to study the effects of Nd substitution on their crystal structure and ferroelectromagnetic behavior. Rietveld refinement of x-ray diffraction data showed a continual transformation of crystal structure from the rhombohedral structure of BNFO[sub x = 0] (BiFeO₃) to a triclinic structure in BNFO[sub x = 0.05–0.15] and a pseudotetragonal structure in BNFO[sub x = 0.175–0.2]. Ferroelectromagnetic measurements revealed the existence of ferroelectricity with remnant polarization of ∼ 9 μC/cm² in BNFO[sub x = 0–0.175], paraelectricity in BNFO[sub x = 0.2], and weak ferromagnetism with remnant magnetizations of 0.07–0.227 emu/g in BNFO[sub x = 0.15–0.2]. Magnetoelectric coupling was obvious in BNFO[sub x = 0.15–0.175] near the Néel temperature of ∼ 380 °C.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationApplied physics letters, 31 July 2006, v. 89, no. 5, 052905, p. 1-3-
dcterms.isPartOfApplied physics letters-
dcterms.issued2006-07-31-
dc.identifier.isiWOS:000239520200072-
dc.identifier.scopus2-s2.0-33748448908-
dc.identifier.eissn1077-3118-
dc.identifier.rosgroupidr31850-
dc.description.ros2006-2007 > 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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