dc.contributor.author |
Burianova, L |
|
dc.contributor.author |
Panos, S |
|
dc.contributor.author |
Stennett, M C |
|
dc.contributor.author |
West, A R |
|
dc.contributor.author |
Subodh, G |
|
dc.contributor.author |
Sebastian, M T |
|
dc.contributor.author |
Kamba, S |
|
dc.date.accessioned |
2014-03-28T05:55:26Z |
|
dc.date.available |
2014-03-28T05:55:26Z |
|
dc.date.issued |
2010 |
|
dc.identifier.citation |
Journal of Electroceramics 25(2-4):116-121;Oct 2010 |
en_US |
dc.identifier.issn |
1385-3449 |
|
dc.identifier.uri |
http://ir.niist.res.in:8080/jspui/handle/123456789/1241 |
|
dc.description.abstract |
In 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.iso |
en |
en_US |
dc.publisher |
Springer |
en_US |
dc.subject |
Ferroelectric properties |
en_US |
dc.subject |
Piezoelectric properties |
en_US |
dc.subject |
Pb free ferroelectric ceramics |
en_US |
dc.title |
Piezoelectric and ferroelectric properties of new Pb9Ce2Ti12O36 and lead-free Ba2NdTi2Nb3O15 ceramics |
en_US |
dc.type |
Article |
en_US |