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dc.contributor.authorPeng, TYen_US
dc.contributor.authorChen, SYen_US
dc.contributor.authorHsieh, LCen_US
dc.contributor.authorLo, CKen_US
dc.contributor.authorHuang, YWen_US
dc.contributor.authorChien, WCen_US
dc.contributor.authorYao, YDen_US
dc.date.accessioned2014-12-08T15:16:49Z-
dc.date.available2014-12-08T15:16:49Z-
dc.date.issued2006-04-15en_US
dc.identifier.issn0021-8979en_US
dc.identifier.urihttp://dx.doi.org/10.1063/1.2177125en_US
dc.identifier.urihttp://hdl.handle.net/11536/12369-
dc.description.abstractThe magnetoimpedance (MZ) effect of the pseudo-spin-valve transistor (PSVT) was investigated at room temperature in the frequency ranged from 100 Hz to 15 MHz. The PSVT can be regarded as a complex combination of resistors, inductors, and capacitors, while the impedance (Z) consists of a real part, the resistance (R), and an imaginary part, the reactance (X). Besides, all these components exhibit magnetic hysteresis. It is due to the frequency dependent behavior that R does not reach a minimum at the resonant frequency (f(r)). The frequency dependences of MZ and MX ratios cross zero at f(x)=6.5 MHz and at f(r)=3.65 MHz, respectively. The shape of magnetoreactance (MX) loop is reverse to the magnetoresistance (MR) loop; furthermore, MX ratio changes sign from negative at f < f(r) to positive at f>f(r). The MZ loop also reverses shape and sign after crossing f(x). For instance, the MZ loop with a ratio of 0.077% at 6 MHz switches to -0.086% and -0.125% at 7 and 8 MHz, respectively. (C) 2006 American Institute of Physics.en_US
dc.language.isoen_USen_US
dc.titleImpedance behavior of spin-valve transistoren_US
dc.typeArticleen_US
dc.identifier.doi10.1063/1.2177125en_US
dc.identifier.journalJOURNAL OF APPLIED PHYSICSen_US
dc.citation.volume99en_US
dc.citation.issue8en_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:000237404200435-
dc.citation.woscount4-
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