Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/5286
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dc.contributorDepartment of Electrical Engineering-
dc.creatorLeung, CM-
dc.creatorOr, DSW-
dc.creatorWang, F-
dc.creatorHo, SL-
dc.creatorLuo, H-
dc.date.accessioned2014-12-11T08:29:06Z-
dc.date.available2014-12-11T08:29:06Z-
dc.identifier.issn0034-6748-
dc.identifier.urihttp://hdl.handle.net/10397/5286-
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 C. M. Leung et al., Review of scientific instruments 82, 013903 (2011) and may be found at http://link.aip.org/link/?rsi/82/013903en_US
dc.subjectDysprosium alloysen_US
dc.subjectIron alloysen_US
dc.subjectLead compoundsen_US
dc.subjectMagnetoelectric effectsen_US
dc.subjectMagnetoelectronicsen_US
dc.subjectPiezeoelectric transducersen_US
dc.subjectTerbium alloysen_US
dc.subjectTransformersen_US
dc.titleEnhanced magnetoelectric effect in heterostructure of magnetostrictive alloy bars and piezoelectric single-crystal transformeren_US
dc.typeJournal/Magazine Articleen_US
dc.description.otherinformationAuthor name used in this publication: Siu Wing Oren_US
dc.description.otherinformationAuthor name used in this publication: S. L. Hoen_US
dc.identifier.spage1-
dc.identifier.epage5-
dc.identifier.volume82-
dc.identifier.issue1-
dc.identifier.doi10.1063/1.3529439-
dcterms.abstractWe report an enhanced magnetoelectric (ME) effect in a heterostructure consisting of a long-type, longitudinally–longitudinally polarized 0.71Pb(Mg₁/₃Nb₂/₃)O₃–0.29PbTiO₃ (PMN-PT) piezoelectric single-crystal transformer with its input part sandwiched between two longitudinally magnetized Tb₀.₃Dy₀.₇Fe₁.₉₂ (Terfenol-D) magnetostrictive alloy bars. The observed ME effect has two independent operational modes: namely, ME sensing mode and ME transduction mode. The ME sensing mode features a large ME voltage coefficient (αV) of ∼0.32 V/Oe over a flat frequency range of 1–50 kHz, while the ME transduction mode possesses two colossal resonance αV of 7.6 and 7.9 V/Oe, corresponding to the first and second longitudinal resonances, at 56.2 and 127.9 kHz, respectively. This enhanced dual-mode ME effect not only enables the application potential of the heterostructure, but also advances the technology of power-free ME sensors and transducers.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationReview of scientific instruments, Jan. 2011, v. 82, no. 1, 013903, p. 1-5-
dcterms.isPartOfReview of scientific instruments-
dcterms.issued2011-01-
dc.identifier.isiWOS:000287545600034-
dc.identifier.scopus2-s2.0-79551658272-
dc.identifier.eissn1089-7623-
dc.identifier.rosgroupidr52176-
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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