Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/4352
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dc.contributorDepartment of Applied Physics-
dc.creatorLam, KH-
dc.creatorLo, CY-
dc.creatorDai, J-
dc.creatorChan, HLW-
dc.creatorLuo, H-
dc.date.accessioned2014-12-11T08:23:20Z-
dc.date.available2014-12-11T08:23:20Z-
dc.identifier.issn0021-8979-
dc.identifier.urihttp://hdl.handle.net/10397/4352-
dc.language.isoenen_US
dc.publisherAmerican Institute of Physicsen_US
dc.rights© 2011 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 K. H. Lam et al., J. Appl. Phys. 109, 024505 (2011) and may be found at http://link.aip.org/link/?jap/109/024505.en_US
dc.subjectLead compoundsen_US
dc.subjectMagnetic sensorsen_US
dc.subjectMagnetoelectric effectsen_US
dc.subjectMagnetostrictionen_US
dc.subjectPermanent magnetsen_US
dc.subjectPiezoceramicsen_US
dc.titleEnhanced magnetoelectric effect in a stress-biased lead magnesium niobate-lead titanate single crystal/Terfenol-D alloy magnetoelectric sensoren_US
dc.typeJournal/Magazine Articleen_US
dc.description.otherinformationAuthor name used in this publication: K. H. Lamen_US
dc.description.otherinformationAuthor name used in this publication: C. Y. Loen_US
dc.description.otherinformationAuthor name used in this publication: J. Y. Daien_US
dc.description.otherinformationAuthor name used in this publication: H. L. W. Chanen_US
dc.description.otherinformationAuthor name used in this publication: H. S. Luoen_US
dc.identifier.spage1-
dc.identifier.epage4-
dc.identifier.volume109-
dc.identifier.issue2-
dc.identifier.doi10.1063/1.3536636-
dcterms.abstractA stress-biased magnetoelectric sensor with a built-in permanent magnet has been fabricated using piezoelectric lead magnesium niobate-lead titanate single crystal and magnetostrictive Terfenol-D alloy. The resonance characteristics and magnetoelectric performance of the sensor have been evaluated under different stress-biased conditions. The resonance of the sensor shifts to higher frequency with increasing preloading stress. Due to the piezoelectric and magnetostrictive enhancements under preload, the device exhibits a giant magnetoelectric voltage coefficient of 0.22 V/Oe at a preloading stress of 2.5 MPa. This compact device has the potential to be used as a standalone sensor without requiring external power input.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of applied physics, 15 Jan. 2011, v. 109, no. 2, 024505, p. 1-4-
dcterms.isPartOfJournal of applied physics-
dcterms.issued2011-01-15-
dc.identifier.isiWOS:000286896400097-
dc.identifier.scopus2-s2.0-79551663666-
dc.identifier.eissn1089-7550-
dc.identifier.rosgroupidr52175-
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
dc.description.oaCategoryVoR alloweden_US
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