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DC Field | Value | Language |
---|---|---|
dc.contributor.author | O. Khamman | en_US |
dc.contributor.author | X. Tan | en_US |
dc.contributor.author | S. Ananta | en_US |
dc.contributor.author | R. Yimnirun | en_US |
dc.date.accessioned | 2018-09-10T03:17:30Z | - |
dc.date.available | 2018-09-10T03:17:30Z | - |
dc.date.issued | 2009-08-01 | en_US |
dc.identifier.issn | 15734803 | en_US |
dc.identifier.issn | 00222461 | en_US |
dc.identifier.other | 2-s2.0-67650091079 | en_US |
dc.identifier.other | 10.1007/s10853-009-3644-z | en_US |
dc.identifier.uri | https://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=67650091079&origin=inward | en_US |
dc.identifier.uri | http://cmuir.cmu.ac.th/jspui/handle/6653943832/59575 | - |
dc.description.abstract | The (1 - x)Bi(Zn1/2Ti1/2)O3-xPbZrO3solid solution ceramics were prepared by using solid-state reaction method, and their ferroelectric properties were investigated. It was found that the perovskite structure is stable for compositions with x ≥ 0.900. Within this composition range, the crystal structure of the solid solution preserves the orthorhombic symmetry of PbZrO3(PZ). The Curie point of the ceramics was found to decrease with increasing Bi(Zn1/2Ti1/2)O3(BZT) content. The intermediate ferroelectric phase of PZ was stabilized by BZT addition and exists within a much wider temperature range in the solid solution. © 2009 Springer Science+Business Media, LLC. | en_US |
dc.subject | Engineering | en_US |
dc.subject | Materials Science | en_US |
dc.title | Ferroelectric properties of (1 - X)Bi(Zn<inf>1/2</inf>Ti<inf>1/2</inf>)O<inf>3</inf>-xPbZrO<inf>3</inf>ceramics | en_US |
dc.type | Journal | en_US |
article.title.sourcetitle | Journal of Materials Science | en_US |
article.volume | 44 | en_US |
article.stream.affiliations | Chiang Mai University | en_US |
article.stream.affiliations | Iowa State University | en_US |
Appears in Collections: | CMUL: Journal Articles |
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