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Effect of Li2O on the defect polarization in CuO-added (K0.9Na0.1)NbO3 piezoelectric ceramics

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dc.contributor.authorKim, Dae-Hyeon-
dc.contributor.authorPark, Jongseong-
dc.contributor.authorLee, Tae-Gon-
dc.contributor.authorCho, Sung-Hoon-
dc.contributor.authorPark, Su-Jin-
dc.contributor.authorLee, Ku-Tak-
dc.contributor.authorKim, Jong-Hyun-
dc.contributor.authorNahm, Sahn-
dc.date.accessioned2021-09-02T23:55:01Z-
dc.date.available2021-09-02T23:55:01Z-
dc.date.created2021-06-19-
dc.date.issued2017-11-
dc.identifier.issn0002-7820-
dc.identifier.urihttps://scholar.korea.ac.kr/handle/2021.sw.korea/81803-
dc.description.abstractCuO-added (LixK0.9-xNa0.1)NbO3 [C(LxK0.9-xN0.1)N] ceramics with 0.0 <= x <= 0.05 were well-sintered at 960 degrees C for 6 hours. The lattice parameters of the specimens decreased with the addition of Li2O. Defect polarization (PD) formed between Cu2+ ions and oxygen vacancies. Double polarization vs electric field (P-E) hysteresis and sprout-shaped strain vs electric field (S-E) curves were observed in these specimens with a large strain of 0.16% at 7.0 kV/mm, possibly owing to the presence of PD. When the P-E curve was measured at temperatures higher than 75 degrees C, the C(K0.9N0.1)N ceramic exhibited a normal P-E hysteresis curve, whereas the C(L0.04K0.86N0.1)N ceramic maintained the double P-E hysteresis curve up to 125 degrees C, indicating that Li2O increased the thermal stability of PD. The latter specimen also showed the sprout shaped S-E curve with a strain of 0.15% at 7.0 kV/mm after 104 cycles of a high electric field of 7.0 kV/mm.-
dc.languageEnglish-
dc.language.isoen-
dc.publisherWILEY-
dc.subjectFIELD-INDUCED STRAIN-
dc.subjectLEAD-FREE CERAMICS-
dc.subjectFERROELECTRIC PROPERTIES-
dc.subjectTEMPERATURE-
dc.subjectDEPENDENCE-
dc.subjectACTUATORS-
dc.titleEffect of Li2O on the defect polarization in CuO-added (K0.9Na0.1)NbO3 piezoelectric ceramics-
dc.typeArticle-
dc.contributor.affiliatedAuthorNahm, Sahn-
dc.identifier.doi10.1111/jace.15047-
dc.identifier.scopusid2-s2.0-85021805991-
dc.identifier.wosid000416463600028-
dc.identifier.bibliographicCitationJOURNAL OF THE AMERICAN CERAMIC SOCIETY, v.100, no.11, pp.5193 - 5201-
dc.relation.isPartOfJOURNAL OF THE AMERICAN CERAMIC SOCIETY-
dc.citation.titleJOURNAL OF THE AMERICAN CERAMIC SOCIETY-
dc.citation.volume100-
dc.citation.number11-
dc.citation.startPage5193-
dc.citation.endPage5201-
dc.type.rimsART-
dc.type.docTypeArticle-
dc.description.journalClass1-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
dc.relation.journalResearchAreaMaterials Science-
dc.relation.journalWebOfScienceCategoryMaterials Science, Ceramics-
dc.subject.keywordPlusFIELD-INDUCED STRAIN-
dc.subject.keywordPlusLEAD-FREE CERAMICS-
dc.subject.keywordPlusFERROELECTRIC PROPERTIES-
dc.subject.keywordPlusTEMPERATURE-
dc.subject.keywordPlusDEPENDENCE-
dc.subject.keywordPlusACTUATORS-
dc.subject.keywordAuthorlead-free ceramics-
dc.subject.keywordAuthorlow temperature-
dc.subject.keywordAuthorpiezoelectric materials/properties-
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