Please use this identifier to cite or link to this item: https://doi.org/10.1063/1.4943244
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dc.titleRoom temperature giant magnetoimpedance in polycrystalline La0.75Ba0.25MnO3
dc.contributor.authorKumar P.
dc.contributor.authorRubi K.
dc.contributor.authorMahendiran R.
dc.date.accessioned2020-09-08T03:46:22Z
dc.date.available2020-09-08T03:46:22Z
dc.date.issued2016
dc.identifier.citationKumar P., Rubi K., Mahendiran R. (2016). Room temperature giant magnetoimpedance in polycrystalline La0.75Ba0.25MnO3. AIP Advances 6 (5) : 55913. ScholarBank@NUS Repository. https://doi.org/10.1063/1.4943244
dc.identifier.issn2158-3226
dc.identifier.urihttps://scholarbank.nus.edu.sg/handle/10635/174627
dc.description.abstractWe report the magnetic field dependence of electrical impedance Z in polycrystalline La0.75Ba0.25MnO3 a function of frequency from f = 1 MHz to 1 GHz at room temperature. The magnetoimpedance [MI = ΔZ/Z(0) where ΔZ = Z(H)-Z(0)] is -37.5 % (-58.5%) at 1(10) MHz for H = 1.2 kOe, which far exceeds mere -1.15% dc magnetoresistance. As f increases above 10 MHz, MI decreases in magnitude and changes sign from negative to positive. The change in sign of MI results from the transition of a single peak at H = 0 to two peaks at H = ± Hp accompanied by a minimum at the origin. Hp shifts towards higher field with increasing frequency. The occurrence of giant radio-frequency magnetoimpedance is promising for low-field sensor applications. © 2016 Author(s).
dc.sourceUnpaywall 20200831
dc.subjectDc magnetoresistance
dc.subjectElectrical impedance
dc.subjectFunction of frequency
dc.subjectGiant magneto-impedance
dc.subjectMagnetic field dependences
dc.subjectMagneto-impedance
dc.subjectPolycrystalline
dc.subjectRadio frequencies
dc.subjectManganese oxide
dc.typeArticle
dc.contributor.departmentELECTRICAL AND COMPUTER ENGINEERING
dc.contributor.departmentPHYSICS
dc.description.doi10.1063/1.4943244
dc.description.sourcetitleAIP Advances
dc.description.volume6
dc.description.issue5
dc.description.page55913
dc.published.statePublished
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