Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/4371
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dc.contributor.authorKeswani, Bhavna C.en_US
dc.contributor.authorPatil, S. I.en_US
dc.contributor.authorJames, A. R.en_US
dc.contributor.authorNath, R. C.en_US
dc.contributor.authorBOOMISHANKAR, RAMAMOORTHYen_US
dc.contributor.authorKolekar, Y. D.en_US
dc.contributor.authorRamana, C. V.en_US
dc.date.accessioned2020-01-28T03:46:13Z
dc.date.available2020-01-28T03:46:13Z
dc.date.issued2019-12en_US
dc.identifier.citationJournal of Applied Physics, 126(22).en_US
dc.identifier.issn1089-7550en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/4371-
dc.identifier.urihttps://doi.org/10.1063/1.5124159en_US
dc.description.abstractThe structural, magnetic, ferroelectric, and magnetoelectric (ME) properties of lead-free ferroelectric phase (0.45)Ba0.7Ca0.3TiO3-(0.55)BaTi0.8Zr0.2O3 (BCZT) and rare earth modified Co-Mn ferrite phase Co0.7Mn0.3Fe1.95Dy0.05O4 (CMFDO) magnetoelectric (ME) composites are reported. X-ray diffraction confirms the presence of a crystal structure corresponding to both the ferroelectric and ferrite phases, which was further confirmed by Raman spectroscopic measurements. Scanning electron micrograph imaging along with the elemental mapping reveals the distribution of CMFDO grains in a BCZT matrix. The variation of dc resistivity with temperature indicates a semiconducting nature of the ME composite. The ME composite shows usual dielectric dispersion behavior with a higher dielectric constant value in the low frequency region compared to the individual ferroic phases, due to the space charge effects. Frequency dependent ac conductivity reveals that the conduction process in the ME composite is due to the small polaron hopping mechanism. Also, the variation of dielectric constant with temperature reveals the presence of two dielectric anomalies corresponding to ferroelectric phase transitions, i.e., from orthorhombic (O) to tetragonal (T) phases (∼298–323 K) and tetragonal (T) to cubic (C) phases (∼400 K). The ME composite exhibits both the ferroelectric [i.e., polarization (P) vs electric field (E)] and ferrimagnetic [i.e., magnetization (M) vs magnetic field (H)] hysteresis loops that confirm its multiferroic nature. The P-E hysteresis loop indicates the significant changes in remanent polarization (ΔPr ∼ 54%) after magnetic poling, confirming the presence of strong magnetoelectric coupling in the ME composite. Further, the strength of the ME coupling calculated was ∼54%, which is remarkable. Thus, the ME composite prepared in the present study may be a suitable candidate for applications in magnetic field sensors and multistate memory devices and may be suitable alternatives for single phase multiferroicsen_US
dc.language.isoenen_US
dc.publisherAIP Publishingen_US
dc.subjectDielectric-Properties; Functional-properties; Ceramic compositesen_US
dc.subjectFerriteen_US
dc.subjectConnectivityen_US
dc.subjectResistivityen_US
dc.subjectGDen_US
dc.subjectTOC-JAN-2020en_US
dc.subject2019en_US
dc.titleStructural, magnetic and ferroelectric properties of lead free piezoelectric 0.9(0.45Ba(0.7)Ca(0.3)TiO(3)-0.55BaTi(0.8)Zr(0.2)O(3)) and magnetostrictive 0.1(Co0.7Mn0.3Fe1.95Dy0.05O4) magnetoelectric particulate compositeen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Chemistryen_US
dc.identifier.sourcetitleJournal of Applied Physicsen_US
dc.publication.originofpublisherForeignen_US
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