Please use this identifier to cite or link to this item: http://cmuir.cmu.ac.th/jspui/handle/6653943832/50854
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dc.contributor.authorPiyachon Ketsuwanen_US
dc.contributor.authorAnurak Prasatkhetragarnen_US
dc.contributor.authorSupon Anantaen_US
dc.contributor.authorChien Chih Huangen_US
dc.contributor.authorDavid P. Cannen_US
dc.contributor.authorRattikorn Yimnirunen_US
dc.date.accessioned2018-09-04T04:46:33Z-
dc.date.available2018-09-04T04:46:33Z-
dc.date.issued2010-02-08en_US
dc.identifier.issn10139826en_US
dc.identifier.other2-s2.0-75749126529en_US
dc.identifier.other10.4028/www.scientific.net/KEM.421-422.255en_US
dc.identifier.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=75749126529&origin=inwarden_US
dc.identifier.urihttp://cmuir.cmu.ac.th/jspui/handle/6653943832/50854-
dc.description.abstractThe Bi0.2K0.8(Zn0.1Ti0.1) Ta0.8O3 and Li doped ceramics prepared via the solid-state reaction technique were investigated. The XRD patterns show the single phase cubic perovskite structure without any evidence of secondary phases when sintered at 1250 °C for undoped Bi0.2K0.8(Zn 0.1Ti0.1)Ta0.8O3 and sintered at 1100 °C for Li doped one. The dielectric properties indicate the diffused phase transition (DPT). The dielectric loss of undoped ceramic increases with increasing frequency in temperature range 270 °C down to -150 °C, which suggests low temperature relaxation, while the dielectric loss of Li doped ceramic reveals the interesting lower value over a wide temperature range of about 0 - 300 °C. © (2010) Trans Tech Publications.en_US
dc.subjectEngineeringen_US
dc.subjectMaterials Scienceen_US
dc.titleDielectric properties of Bi0.2K0.8(Zn 0.1Ti0.1)Ta0.8O3 ceramicsen_US
dc.typeBook Seriesen_US
article.title.sourcetitleKey Engineering Materialsen_US
article.volume421-422en_US
article.stream.affiliationsNaresuan Universityen_US
article.stream.affiliationsChiang Mai Universityen_US
article.stream.affiliationsOregon State Universityen_US
article.stream.affiliationsSuranaree University of Technologyen_US
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