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hal.structure.identifierLaboratoire des Matériaux Ferroélectriques [LMF]
dc.contributor.authorCHAKER, Chiheb
hal.structure.identifierLaboratoire des Matériaux Ferroélectriques [LMF]
dc.contributor.authorEL GHARBI, Walid
hal.structure.identifierLaboratoire des Matériaux Ferroélectriques [LMF]
dc.contributor.authorABDELMOULA, Najmeddine
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorSIMON, Annie
hal.structure.identifierLaboratoire des Matériaux Ferroélectriques [LMF]
dc.contributor.authorKHEMAKHEM, Hamadi
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorMAGLIONE, Mario
dc.date.issued2011
dc.identifier.issn0022-3697
dc.description.abstractEnNa<sub>1−<i>x</i></sub>Li<sub><i>x</i></sub>NbO<sub>3</sub> ceramics with composition 0.05≤<i>x</i>≤0.30 were prepared by solid-state reaction method and sintered in the temperature range 1100-1150 °C. These ceramics were characterised by X-ray diffraction as well as dielectric permittivity measurements and Raman spectroscopy. Dielectric properties of ceramics belonging to the whole composition domain were investigated in a broad range of temperatures from 300 to 750 K and frequencies from 0.1 to 200 kHz. The Rietveld refinement powder X-ray diffraction analysis showed that these ceramics have a single phase of perovskite structure with orthorhombic symmetry for <i>x</i>≤0.15 and two phases coexistence of rhombohedral and orthorhombic above <i>x</i>=0.20. The evolution of the permittivity as a function of temperature and frequency showed that these ceramics Na<sub>1−<i>x</i></sub>Li<sub><i>x</i></sub>NbO<sub>3</sub> with composition 0.05≤<i>x</i>≤0.15 present the classical ferroelectric character and the phase transition temperature <i>T</i><sub>C</sub> increases as <i>x</i> content increases. The polarisation state was checked by pyroelectric and piezoelectric measurements. For <i>x</i>=0.05, the piezoelectric coefficient <i>d</i><sub>31</sub> is of 2pC/N. The evolution of the Raman spectra was studied as a function of temperatures and compositions. The results of the Raman spectroscopy study confirm our dielectric measurements, and they indicate clearly the transition from the polar ferroelectric phase to the non-polar paraelectric one.
dc.language.isoen
dc.publisherElsevier
dc.subject.enCeramics
dc.subject.enX-ray diffraction
dc.subject.enRaman spectroscopy
dc.subject.enFerroelectricity
dc.subject.enPhase transitions
dc.typeArticle de revue
dc.identifier.doi10.1016/j.jpcs.2011.07.002
dc.subject.halChimie/Matériaux
bordeaux.journalJournal of Physics and Chemistry of Solids
bordeaux.page1140-1146
bordeaux.volume72
bordeaux.issue10
bordeaux.peerReviewedoui
hal.identifierhal-00617183
hal.version1
hal.popularnon
hal.audienceInternationale
hal.origin.linkhttps://hal.archives-ouvertes.fr//hal-00617183v1
bordeaux.COinSctx_ver=Z39.88-2004&amp;rft_val_fmt=info:ofi/fmt:kev:mtx:journal&amp;rft.jtitle=Journal%20of%20Physics%20and%20Chemistry%20of%20Solids&amp;rft.date=2011&amp;rft.volume=72&amp;rft.issue=10&amp;rft.spage=1140-1146&amp;rft.epage=1140-1146&amp;rft.eissn=0022-3697&amp;rft.issn=0022-3697&amp;rft.au=CHAKER,%20Chiheb&amp;EL%20GHARBI,%20Walid&amp;ABDELMOULA,%20Najmeddine&amp;SIMON,%20Annie&amp;KHEMAKHEM,%20Hamadi&amp;rft.genre=article


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