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dc.contributor.authorSukum Eitssayeamen_US
dc.contributor.authorUraiwan Inthataen_US
dc.contributor.authorKrit Sujarittangtumen_US
dc.contributor.authorSuchittra Inthongen_US
dc.contributor.authorPiewpan Parjansrien_US
dc.contributor.authorKamonpan Pengpaten_US
dc.contributor.authorGobwute Rujijanagulen_US
dc.contributor.authorTawee Tunkasirien_US
dc.date.accessioned2018-09-04T04:23:28Z-
dc.date.available2018-09-04T04:23:28Z-
dc.date.issued2011-07-29en_US
dc.identifier.issn15635112en_US
dc.identifier.issn00150193en_US
dc.identifier.other2-s2.0-79960713901en_US
dc.identifier.other10.1080/00150193.2011.577390en_US
dc.identifier.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=79960713901&origin=inwarden_US
dc.identifier.urihttp://cmuir.cmu.ac.th/jspui/handle/6653943832/50081-
dc.description.abstractThe (1-x)Ba0.9Sr0.1[Ti0.8(Fe1/3Nb2/3)0.2]O3-xBiZn1/2Ti1/2O3solid solution ceramics were synthesized via a solid-state reaction method where x = 0.02, 0.04, 0.06, 0.08 and 0.10. The structural and electrical properties of these ceramics system were investigated as a function of the BZT content by X-ray diffraction (XRD) and dielectric measurement techniques. The XRD analysis demonstrated that with increasing BZT content in (1-x)BSTFN-xBZT, the structural change occurred from the rhombohedral to the tetragonal phase at room temperature. Changes in the dielectric behaviorwere found to depend on the BZT content. Copyright © Taylor &Francis Group, LLC.en_US
dc.subjectMaterials Scienceen_US
dc.subjectPhysics and Astronomyen_US
dc.titlePreparation and electrical properties of (1-x)Ba<inf>0.9</inf>Sr<inf>0.1</inf>[Ti<inf>0.8</inf>(Fe<inf>0.5</inf>Nb<inf>0.5</inf>)<inf>0.2</inf>]O<inf>3</inf>-xBiZn<inf>0.5</inf>Ti<inf>0.5</inf>O<inf>3</inf>ceramicsen_US
dc.typeJournalen_US
article.title.sourcetitleFerroelectricsen_US
article.volume415en_US
article.stream.affiliationsChiang Mai Universityen_US
article.stream.affiliationsMae Fah Luang Universityen_US
Appears in Collections:CMUL: Journal Articles

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