Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/602
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dc.contributorDepartment of Applied Physics-
dc.contributorMaterials Research Centre-
dc.creatorLin, D-
dc.creatorKwok, KW-
dc.creatorChan, HLW-
dc.date.accessioned2014-12-11T08:24:10Z-
dc.date.available2014-12-11T08:24:10Z-
dc.identifier.issn0021-8979-
dc.identifier.urihttp://hdl.handle.net/10397/602-
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, 034102 (2007) and may be found at http://link.aip.org/link/?jap/102/034102en_US
dc.subjectCrystal microstructureen_US
dc.subjectFerroelectric Curie temperatureen_US
dc.subjectFerroelectric materialsen_US
dc.subjectLithium compoundsen_US
dc.subjectPiezoceramicsen_US
dc.subjectPiezoelectric materialsen_US
dc.subjectPotassium compoundsen_US
dc.subjectSinteringen_US
dc.subjectSodium compoundsen_US
dc.titleMicrostructure, phase transition, and electrical properties of (K[sub 0.5]Na[sub 0.5])[sub 1-x]Li[sub x](Nb[sub 1-y]Ta[sub y])O₃ lead-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: H. L. W. Chanen_US
dc.identifier.spage1-
dc.identifier.epage7-
dc.identifier.volume102-
dc.identifier.issue3-
dc.identifier.doi10.1063/1.2761852-
dcterms.abstractLead-free ceramics (K[sub 0.5]Na[sub 0.5])[sub 1−x]Li[sub x](Nb[sub 1−y]Ta[sub y])O₃ have been prepared by an ordinary sintering technique. Our results reveal that Li[sup +] and Ta[sup 5+] diffuse into the K[sub 0.5]Na[sub 0.5]NbO₃ lattices to form a solid solution with a perovskite structure. The substitution of Li[sup +] induces an increase in the Curie temperature (T[sub C]) and a decrease in the ferroelectric tetragonal-ferroelectric orthorhombic phase transition temperature (T[sub O-T]). On the other hand, both T[sub C] and T[sub O-T] decrease after the substitution of Ta[sup 5+]. A coexistence of the orthorhombic and tetragonal phases is formed at 0.03<x<0.06 and 0.10<y<0.25 near room temperature, leading to significant enhancements of the piezoelectric properties. For the ceramic with x=0.04 and y=0.225, the piezoelectric properties become optimum, giving a piezoelectric coefficient d₃₃=208 pC/N, electromechanical coupling factors k[sub p]=48% and k[sub t]=49%, remanent polarization P[sub r]=14.2 µC/cm², coercive field E[sub c]=1.21 kV/mm, and Curie temperature T[sub C]=320 °C.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of applied physics, 3 Aug. 2007, v. 102, 034102, no. 3, p. 1-7-
dcterms.isPartOfJournal of applied physics-
dcterms.issued2007-08-03-
dc.identifier.isiWOS:000249240600072-
dc.identifier.scopus2-s2.0-34548011958-
dc.identifier.eissn1089-7550-
dc.identifier.rosgroupidr36968-
dc.description.ros2007-2008 > 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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