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Self-biased converse magnetoelectric effect
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10.1063/1.3662420
/content/aip/journal/apl/99/20/10.1063/1.3662420
http://aip.metastore.ingenta.com/content/aip/journal/apl/99/20/10.1063/1.3662420
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

(Color online) (a) α DME and (b) α CME coefficients as a function of Hbias , (c) Integral values of α DME and α CME with respect to the Hbias , and (d) Magnetostriction of Ni, KNNLS-NZF, and bending mode KNNLS-NZF/Ni/KNNLS-NZF as a function of Hbias .

Image of FIG. 2.
FIG. 2.

(Color online) (a) Impedance and phase spectra for three-phase laminate under applied AC electric field, (b) α DME and (c) α CME as a function of frequency under applied Hbias of 0 and 100 Oe.

Image of FIG. 3.
FIG. 3.

(Color online) Magnetic flux density under Hbias  = 0 Oe measured by periodically applying AC voltage of 1 V at 21 kHz. Insets show the configuration of bending-mode three-phase laminate (KNNLS-NZF/Ni/KNNLS-NZF) and the change in magnetic flux density with increasing AC voltage.

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/content/aip/journal/apl/99/20/10.1063/1.3662420
2011-11-17
2014-04-19
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Self-biased converse magnetoelectric effect
http://aip.metastore.ingenta.com/content/aip/journal/apl/99/20/10.1063/1.3662420
10.1063/1.3662420
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