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dc.contributor.authorChien, W. C.en_US
dc.contributor.authorLo, C. K.en_US
dc.contributor.authorHsieh, L. C.en_US
dc.contributor.authorYao, Y. D.en_US
dc.contributor.authorHan, X. F.en_US
dc.contributor.authorZeng, Z. M.en_US
dc.contributor.authorPeng, T. Y.en_US
dc.contributor.authorLin, P.en_US
dc.date.accessioned2014-12-08T15:15:23Z-
dc.date.available2014-12-08T15:15:23Z-
dc.date.issued2006-11-13en_US
dc.identifier.issn0003-6951en_US
dc.identifier.urihttp://dx.doi.org/10.1063/1.2374807en_US
dc.identifier.urihttp://hdl.handle.net/11536/11550-
dc.description.abstractThe magnetoimpedance effect was employed to study magnetotunneling junction (MTJ) with the structure of Ru(5 nm)/Cu(10 nm)/Ru(5 nm)/IrMn(10 nm)/CoFeB(4 nm)/Al(1.2 nm)-oxide/CoFeB(4 nm)/Ru(5 nm). A huge change of more than +/- 17 000% was observed in the imaginary part of the impedance between the magnetically parallel and antiparallel states of the MTJ. The inverse behavior of the magnetoimpedance (MI) loop occurs beyond 21.1 MHz; however, the normal MI at low frequency and the inverse MI at high frequency exhibit the same magnetization reversal as checked by the Kerr effect. The reversal in MI was due to the dominance of magnetocapacitance at high frequency. (c) 2006 American Institute of Physics.en_US
dc.language.isoen_USen_US
dc.titleEnhancement and inverse behaviors of magnetoimpedance in a magnetotunneling junction by driving frequencyen_US
dc.typeArticleen_US
dc.identifier.doi10.1063/1.2374807en_US
dc.identifier.journalAPPLIED PHYSICS LETTERSen_US
dc.citation.volume89en_US
dc.citation.issue20en_US
dc.citation.epageen_US
dc.contributor.department材料科學與工程學系zh_TW
dc.contributor.departmentDepartment of Materials Science and Engineeringen_US
dc.identifier.wosnumberWOS:000242100200067-
dc.citation.woscount11-
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