dc.contributor.author | Rozana Aina, Maulat Osman, Dr. | |
dc.contributor.author | Masó, Nahum | |
dc.contributor.author | West, Anthony R. | |
dc.date.accessioned | 2014-01-02T03:23:34Z | |
dc.date.available | 2014-01-02T03:23:34Z | |
dc.date.issued | 2012-01 | |
dc.identifier.citation | Journal of the American Ceramic Society, vol. 95(1), 2012, pages 296-302 | en_US |
dc.identifier.issn | 0002-7820 | |
dc.identifier.uri | http://onlinelibrary.wiley.com/doi/10.1111/j.1551-2916.2011.04779.x/abstract;jsessionid=31BE2529C1916CC9D075ECC2895B6093.f04t01 | |
dc.identifier.uri | http://dspace.unimap.edu.my/123456789/30944 | |
dc.description | Link to publisher's homepage at http://ceramics.org/ | en_US |
dc.description.abstract | Fixed frequency plots of ε and tan δ versus temperature for (Bi 1.5Zn 0.5)(Zn 0.5Nb 1.5)O 7 (BZN) ceramics with the pyrochlore structure show relaxor-like response below ∼180 K with frequency-independent permittivity of ∼130 above ∼180 K and over the frequency range of 10 3-10 6 Hz. Impedance data in the range, 10-180 K fit an equivalent circuit derived from the classic dielectric relaxation circuit in which the relaxation resistance is replaced by a constant phase element (CPE). Temperature dependence of the circuit parameters shows that BZN is not ferroelectric; the CPE, which is responsible for the relaxor-like behavior, gradually changes from primarily capacitive to primarily resistive with increasing temperature. | en_US |
dc.language.iso | en | en_US |
dc.publisher | The American Ceramic Society | en_US |
dc.subject | Bismuth zinc niobate | en_US |
dc.subject | Pyrochlore structures | en_US |
dc.subject | Ferroelectricity | en_US |
dc.subject | Circuit parameter | en_US |
dc.title | Bismuth zinc niobate pyrochlore, a relaxor-like non-ferroelectric | en_US |
dc.type | Article | en_US |
dc.contributor.url | rozana@unimap.edu.my | en_US |
dc.contributor.url | a.r.west@sheffield.ac.uk | en_US |