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dc.contributor.authorN. Vittayakornen_US
dc.contributor.authorG. Rujijanagulen_US
dc.contributor.authorX. Tanen_US
dc.contributor.authorH. Heen_US
dc.contributor.authorM. A. Marquardten_US
dc.contributor.authorD. P. Cannen_US
dc.date.accessioned2018-09-11T08:57:05Z-
dc.date.available2018-09-11T08:57:05Z-
dc.date.issued2006-03-01en_US
dc.identifier.issn15738663en_US
dc.identifier.issn13853449en_US
dc.identifier.other2-s2.0-33646015076en_US
dc.identifier.other10.1007/s10832-006-4927-2en_US
dc.identifier.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=33646015076&origin=inwarden_US
dc.identifier.urihttp://cmuir.cmu.ac.th/jspui/handle/6653943832/61687-
dc.description.abstractCeramics in the xPb(Zn1/3Nb2/3)O3-(1-x) Pb(Zr0.5Ti0.5)O3[xPZN-(1-x)PZT] solid solution system are expected to display excellent dielectric, piezoelectric, and ferroelectric properties in compositions close to the morphotropic phase boundary (MPB). The dielectric behavior of ceramics with x = 0.1-0.6 has been characterized in order to identify the MPB compositions in this system. Combined with X-ray diffraction results, ferroelectric hysteresis measurements, and Raman reflectivity analysis, it was consistently shown that an MPB exists between x = 0.2 and x = 0.3 in this binary system. When x ≤ 0.2, the tetragonal phase dominates at ambient temperatures. In the range of x ≥ 0.3, the rhombohedral phase dominates. For this rhombohedral phase, electrical measurements reveal a profound frequency dispersion in the dielectric response when x ≥ 0.6, suggesting a transition from normal ferroelectric to relaxor ferroelectric between 0.5 ≥ x ≤ 0.6. Excellent piezoelectric properties were found in 0.3PZN-0.7PZT, the composition closest to the MPB with a rhombohedral structure. The results are summarized in a PZN-PZT binary phase diagram. © Springer Science + Business Media, Inc. 2006.en_US
dc.subjectEngineeringen_US
dc.subjectMaterials Scienceen_US
dc.subjectPhysics and Astronomyen_US
dc.titleDielectric properties and morphotropic phase boundaries in the xPb(Zn<inf>1/3</inf>Nb<inf>2/3</inf>)O<inf>3</inf>-(1-x)Pb(Zr<inf>0.5</inf>Ti<inf>0.5</inf>O<inf>3</inf>pseudo-binary systemen_US
dc.typeJournalen_US
article.title.sourcetitleJournal of Electroceramicsen_US
article.volume16en_US
article.stream.affiliationsKing Mongkut's Institute of Technology Ladkrabangen_US
article.stream.affiliationsChiang Mai Universityen_US
article.stream.affiliationsIowa State Universityen_US
article.stream.affiliationsOregon State Universityen_US
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