Giant magnetoelectric effect in Pb(Zr,Ti)O(3)-bimorph/NdFeB laminate device

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dc.contributorVirginia Techen
dc.contributor.authorXing, Zengpingen
dc.contributor.authorLi, Jiefangen
dc.contributor.authorViehland, Dwight D.en
dc.contributor.departmentMaterials Science and Engineering (MSE)en
dc.date.accessed2014-01-17en
dc.date.accessioned2014-01-28T18:00:13Zen
dc.date.available2014-01-28T18:00:13Zen
dc.date.issued2008-07-01en
dc.description.abstractA Pb(Zr,Ti)O(3)-bimorph/NdFeB laminate device has a giant magnetoelectric (ME) effect. Our results reveal a giant ME coefficient of 16 V/cm Oe or 62 nC/cm Oe at a low (subresonant) frequency of 10 Hz, and one of 250 V/cm Oe or 960 nC/cm Oe at a first order resonant bending mode frequency of similar to 60 Hz. The findings show a simple means by which to achieve magnetoelectric effects, without the use of magnetostrictive material. (C) 2008 American Institute of Physics.en
dc.format.mimetypeapplication/pdfen
dc.identifier.citationXing, Zengping; Li, Jiefang; Viehland, D., "Giant magnetoelectric effect in Pb(Zr,Ti)O(3)-bimorph/NdFeB laminate device," Appl. Phys. Lett. 93, 013505 (2008); http://dx.doi.org/10.1063/1.2956676en
dc.identifier.doihttps://doi.org/10.1063/1.2956676en
dc.identifier.issn0003-6951en
dc.identifier.urihttp://hdl.handle.net/10919/25175en
dc.identifier.urlhttp://scitation.aip.org/content/aip/journal/apl/93/1/10.1063/1.2956676en
dc.language.isoen_USen
dc.publisherAIP Publishingen
dc.rightsIn Copyrighten
dc.rights.urihttp://rightsstatements.org/vocab/InC/1.0/en
dc.subjectCantilever beamen
dc.subjectFrequencyen
dc.subjectPhysicsen
dc.titleGiant magnetoelectric effect in Pb(Zr,Ti)O(3)-bimorph/NdFeB laminate deviceen
dc.title.serialApplied Physics Lettersen
dc.typeArticle - Refereeden
dc.type.dcmitypeTexten

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