Please use this identifier to cite or link to this item: http://localhost:8080/xmlui/handle/123456789/1241
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dc.contributor.authorBurianova, L-
dc.contributor.authorPanos, S-
dc.contributor.authorStennett, M C-
dc.contributor.authorWest, A R-
dc.contributor.authorSubodh, G-
dc.contributor.authorSebastian, M T-
dc.contributor.authorKamba, S-
dc.date.accessioned2014-03-28T05:55:26Z-
dc.date.available2014-03-28T05:55:26Z-
dc.date.issued2010-
dc.identifier.citationJournal of Electroceramics 25(2-4):116-121;Oct 2010en_US
dc.identifier.issn1385-3449-
dc.identifier.urihttp://ir.niist.res.in:8080/jspui/handle/123456789/1241-
dc.description.abstractIn this paper, measurements of the nonlinear ferroelectric, piezoelectric and dielectric properties of Pb9Ce2Ti12O36 (Pb9CTO) and Ba2NdTi2Nb3O15 (BNTN) ferroelectric ceramics are presented. Hysteresis P(E) loops were measured as a function of applied electric field, frequency and temperature. The coercive field (E (c)) and remnant polarization (P (r)) displayed temperature and frequency dependence. Lead-free BNTN ceramics exhibited a coercive field E (c) > 2.4 kV mm(-1) and a piezoelectric coefficient d (33) = 2 pC N-1. The hysteresis loop was pinched above 110A degrees C and a linear response was observed at 155A degrees C, typical of a paraelectric material. Pb9CTO was shown to be ferroelectric with coercive field E (c) = 1.2 kV mm(-1) and a d (33) = 65 pC N-1. The frequency dependences of the impedance of the Pb9CTO discs were analyzed.en_US
dc.language.isoenen_US
dc.publisherSpringeren_US
dc.subjectFerroelectric propertiesen_US
dc.subjectPiezoelectric propertiesen_US
dc.subjectPb free ferroelectric ceramicsen_US
dc.titlePiezoelectric and ferroelectric properties of new Pb9Ce2Ti12O36 and lead-free Ba2NdTi2Nb3O15 ceramicsen_US
dc.typeArticleen_US
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