Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/4980
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dc.contributorDepartment of Applied Physics-
dc.creatorWu, W-
dc.creatorWong, KH-
dc.creatorMak, CL-
dc.creatorChoy, CL-
dc.creatorZhang, YH-
dc.date.accessioned2014-12-11T08:28:22Z-
dc.date.available2014-12-11T08:28:22Z-
dc.identifier.issn0021-8979-
dc.identifier.urihttp://hdl.handle.net/10397/4980-
dc.language.isoenen_US
dc.publisherAmerican Institute of Physicsen_US
dc.rights© 2000 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 W. Wu et al., J. Appl. Phys. 88, 2068 (2000) and may be found at http://link.aip.org/link/?jap/88/2068.en_US
dc.subjectLead compoundsen_US
dc.subjectLanthanum compoundsen_US
dc.subjectPulsed laser depositionen_US
dc.subjectFerroelectric materialsen_US
dc.subjectFerroelectric thin filmsen_US
dc.subjectField effect transistorsen_US
dc.subjectDielectric polarisationen_US
dc.titleEpitaxial Pb(Zr₀.₅₂Ti₀.₄₈)O₃/La₀.₃₅Nd₀.₃₅Sr₀.₃MnO₃heterostructures for fabrication of ferroelectric field-effect transistoren_US
dc.typeJournal/Magazine Articleen_US
dc.description.otherinformationAuthor name used in this publication: K. H. Wongen_US
dc.description.otherinformationAuthor name used in this publication: C. L. Maken_US
dc.description.otherinformationAuthor name used in this publication: C. L. Choyen_US
dc.identifier.spage2068-
dc.identifier.epage2071-
dc.identifier.volume88-
dc.identifier.issue4-
dc.identifier.doi10.1063/1.1305859-
dcterms.abstractEpitaxial La₀.₃₅Nd₀.₃₅Sr₀.₃MnO₃(LNSMO) thin films and Pb(Zr₀.₅ ₂Ti₀.₄₈)O₃(PZT)/LNSMO heterostructures have been grown on LaAlO₃(001) substrates by the pulsed laser deposition method. The oxygen concentration in the LNSMO films is quite sensitive to the deposition oxygen pressure and can be controlled during the fabrication process. It is, however, stable against in situ postdeposition thermal treatments. Consequently, the resistivity and the metal-semiconductor transition temperature of the LNSMO films can be tuned and fixed during film growth. Electrical measurements on the Pt/PZT/LNSMO ferroelectric capacitor show a remnant polarization of ~35 μC/cm² and a coercive field of 30–40 kV/cm at low driving voltages. Switching endurance tests suggest no polarization loss up to about 10¹⁰ bipolar switching cycles. The advantages of using epitaxial LNSMO films as the semiconducting channel in an all-perovskite ferroelectric field-effect transistor are discussed.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of applied physics, 15 Aug. 2000, v. 88, no. 4, p. 2068-2071-
dcterms.isPartOfJournal of applied physics-
dcterms.issued2000-08-15-
dc.identifier.isiWOS:000088783800060-
dc.identifier.scopus2-s2.0-0000330028-
dc.identifier.eissn1089-7550-
dc.identifier.rosgroupidr03178-
dc.description.ros2000-2001 > 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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