Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/4232
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dc.contributorDepartment of Applied Physics-
dc.creatorLin, D-
dc.creatorKwok, KW-
dc.creatorLam, KH-
dc.creatorChan, HLW-
dc.date.accessioned2014-12-11T08:28:17Z-
dc.date.available2014-12-11T08:28:17Z-
dc.identifier.issn0021-8979-
dc.identifier.urihttp://hdl.handle.net/10397/4232-
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 et al., J. Appl. Phys. 101, 074111 (2007) and may be found at http://link.aip.org/link/?jap/101/074111.en_US
dc.subjectPotassium compoundsen_US
dc.subjectSodium compoundsen_US
dc.subjectLithium compoundsen_US
dc.subjectPiezoceramicsen_US
dc.subjectSinteringen_US
dc.subjectX-ray diffractionen_US
dc.subjectFerroelectric transitionsen_US
dc.subjectPiezoelectricityen_US
dc.subjectDielectric polarisationen_US
dc.subjectFerroelectric Curie temperatureen_US
dc.titleStructure and electrical properties of K₀.₅Na₀.₅NbO₃-LiSbO₃lead-free piezoelectric ceramicsen_US
dc.typeJournal/Magazine Articleen_US
dc.description.otherinformationAuthor name used in this publication: K. W. Kwoken_US
dc.description.otherinformationAuthor name used in this publication: K. H. Lamen_US
dc.description.otherinformationAuthor name used in this publication: H. L. W. Chanen_US
dc.identifier.spage1-
dc.identifier.epage6-
dc.identifier.volume101-
dc.identifier.issue7-
dc.identifier.doi10.1063/1.2715486-
dcterms.abstractLead-free piezoelectric ceramics (1−x)K₀.₅Na ₀.₅NbO₃-xLiSbO₃have been fabricated by a conventional ceramic sintering technique. The results of x-ray diffraction suggest that Liᐩ and Sb⁵ᐩ diffuse into the K₀.₅Na₀.₅NbO₃lattices to form a solid solution with a perovskite structure. The ceramics can be well sintered at 1070–1110 ℃ . The introduction of LiSbO₃into the Na₀.₅K₀.₅NbO₃solid solution decreases slightly the paraelectric cubic-ferroelectric tetragonal phase transition temperature (Tᴄ) , but greatly shifts the ferroelectric tetragonal-ferroelectric orthorhombic phase transition (T[sub O–F]) to room temperature. Coexistence of the orthorhombic and tetragonal phases is formed at 0.05< x <0.07 at room temperature, leading to a significant enhancement of the piezoelectric properties. For the ceramic with x=0.06, the piezoelectric properties become optimum: piezoelectric constant d₃₃=212 pC/N, planar and thickness electromechanical coupling factors kP =46% and kt=47%, respectively, remanent polarization Pᵣ=15.0 μC/cm², coercive field Ec=1.74 kV/mm, and Curie temperature Tᴄ=358 °C.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of applied physics, 1 Apr. 2007, v. 101, no. 7, 074111, p. 1-6-
dcterms.isPartOfJournal of applied physics-
dcterms.issued2007-04-01-
dc.identifier.isiWOS:000245691000073-
dc.identifier.eissn1089-7550-
dc.identifier.rosgroupidr34816-
dc.description.ros2006-2007 > Academic research: refereed > Publication in refereed journal-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_IR/PIRAen_US
dc.description.pubStatusPublisheden_US
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