Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/394
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dc.contributorDepartment of Applied Physics-
dc.contributorMaterials Research Centre-
dc.creatorLin, Den_US
dc.creatorKwok, KWen_US
dc.creatorChan, HLWen_US
dc.date.accessioned2014-12-11T08:27:31Z-
dc.date.available2014-12-11T08:27:31Z-
dc.identifier.issn0021-8979en_US
dc.identifier.urihttp://hdl.handle.net/10397/394-
dc.language.isoenen_US
dc.publisherAmerican Institute of Physicsen_US
dc.rights© 2007 American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the American Institute of Physics. The following article appeared in D. Lin, K.W. Kwok, & H.L.W. Chan. J. Appl. Phys. 102, 074113 (2007) and may be found at http://link.aip.org/link/?jap/102/074113en_US
dc.subjectBarium compoundsen_US
dc.subjectCopper compoundsen_US
dc.subjectCrystal structureen_US
dc.subjectDensificationen_US
dc.subjectDielectric lossesen_US
dc.subjectDielectric polarisationen_US
dc.subjectDielectric relaxationen_US
dc.subjectFerroelectric Curie temperatureen_US
dc.subjectPiezoceramicsen_US
dc.subjectPotassium compoundsen_US
dc.subjectSodium compoundsen_US
dc.titleStructure, dielectric, and piezoelectric properties of CuO-doped K₀.₅Na₀.₅NbO₃ -BaTiO₃ lead-free ceramicsen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage1en_US
dc.identifier.epage6en_US
dc.identifier.volume102en_US
dc.identifier.doi10.1063/1.2787164en_US
dcterms.abstractLead-free piezoelectric ceramics (1−x)K[sub 0.5]Na[sub 0.5]NbO₃+xBaTiO₃+y mol % CuO have been fabricated by an ordinary sintering technique. Our results show that the doping of CuO is effective in promoting the densification of the ceramics. With the doping of CuO, all the ceramics can be well sintered and exhibit a dense, pure perovskite structure. After the formation of a solid solution with BaTiO₃, both the paraelectric cubic-ferroelectric tetragonal and ferroelectric tetragonal-ferroelectric orthorhombic phase transition temperatures decrease and a relax behavior is induced. Coexistence of the orthorhombic and tetragonal phases is formed in the ceramics with 0.04≤x≤0.06 and y=1.00 at room temperature. Because of the more possible polarization states arising from the coexistence of the two phases and the improved densification, the piezoelectric and dielectric properties of the ceramics are enhanced significantly. The ceramic with x=0.06 and y=1.00 exhibits the optimum properties: d[sub 33]=193 pC/N, k[sub p]=0.43, k[sub t]=0.40, and T[sub C]=314 °C. On the other hand, the ceramics with 0≤x≤0.01 and y=1.0 exhibit excellent “hard” piezoelectric characteristics: k[sub p]~0.40, k[sub t]~0.47, Q[sub m]~1940, ε[sub r]~230, and tan δ~0.5%.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of applied physics, 11 Oct. 2007, v. 102, 074113, p. 1-6en_US
dcterms.isPartOfJournal of applied physicsen_US
dcterms.issued2007-10-11-
dc.identifier.isiWOS:000250147700103-
dc.identifier.scopus2-s2.0-35348915973-
dc.identifier.eissn1089-7550en_US
dc.identifier.rosgroupidr36985-
dc.description.ros2007-2008 > Academic research: refereed > Publication in refereed journal-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_IR/PIRA-
dc.description.pubStatusPublisheden_US
dc.description.oaCategoryVoR alloweden_US
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