CRYSTAL-STRUCTURE AND B-SITE ORDERING IN ANTIFERROELECTRIC PB(MG1/2W1/2)O3, PB(CO1/2W1/2)O3 AND PB(YB1/2NB1/2)O3

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dc.contributor.authorChoo, Woong Kilko
dc.contributor.authorKIM, HJko
dc.contributor.authorYANG, JHko
dc.contributor.authorLIM, Hko
dc.contributor.authorLee, JeongYongko
dc.contributor.authorKWON, JRko
dc.contributor.authorCHUN, CHko
dc.date.accessioned2013-02-27T08:09:20Z-
dc.date.available2013-02-27T08:09:20Z-
dc.date.created2012-02-06-
dc.date.created2012-02-06-
dc.date.issued1993-09-
dc.identifier.citationJAPANESE JOURNAL OF APPLIED PHYSICS PART 1-REGULAR PAPERS SHORT NOTES REVIEW PAPERS, v.32, no.9B, pp.4249 - 4253-
dc.identifier.issn0021-4922-
dc.identifier.urihttp://hdl.handle.net/10203/67398-
dc.description.abstractThe high-temperature phase of Pb(Mg1/2W1/2)O3, Pb(Co1/2W1/2)O3 and Pb(Yb1/2Nb1/2)O3 belongs to the space group Fm3m with the unit cell size of 2a(c) X 2a(c) X 2a(c) where a(c) is the lattice parameter of the cubic perovskite unit cell. All these complex perovskites undergo phase transition into low-temperature orthorhombic structures with a shrunken lattice parameter along the c-axis and the approximate square-root 2 a lattice parameters along the a0- and b0-axes, which are, respectively, parallel to the prototype [110]c and [110BAR]c directions. The symmetry along the b0-axis of the perovskites is most prominently distinguished from that along the a0-axis in that the low-temperature structure is modulated in the b0-axis direction. For Pb(Mg1/2W1/2)O3, a diffraction pattern detrimental to the crystal structure determination well below the Curie temperature is presented. At the same time, the crystal structures of lock-in phases of the aforementioned oxides are compared with the well-known structure of PbZrO3.-
dc.languageEnglish-
dc.publisherJAPAN J APPLIED PHYSICS-
dc.subjectELECTRON-DIFFRACTION-
dc.subjectNEUTRON-DIFFRACTION-
dc.subjectPHASE-TRANSITIONS-
dc.subjectSOLID-SOLUTION-
dc.subjectPBZRO3-
dc.titleCRYSTAL-STRUCTURE AND B-SITE ORDERING IN ANTIFERROELECTRIC PB(MG1/2W1/2)O3, PB(CO1/2W1/2)O3 AND PB(YB1/2NB1/2)O3-
dc.typeArticle-
dc.identifier.wosidA1993MD98800054-
dc.type.rimsART-
dc.citation.volume32-
dc.citation.issue9B-
dc.citation.beginningpage4249-
dc.citation.endingpage4253-
dc.citation.publicationnameJAPANESE JOURNAL OF APPLIED PHYSICS PART 1-REGULAR PAPERS SHORT NOTES REVIEW PAPERS-
dc.contributor.localauthorLee, JeongYong-
dc.contributor.nonIdAuthorKIM, HJ-
dc.contributor.nonIdAuthorYANG, JH-
dc.contributor.nonIdAuthorLIM, H-
dc.contributor.nonIdAuthorKWON, JR-
dc.contributor.nonIdAuthorCHUN, CH-
dc.type.journalArticleArticle; Proceedings Paper-
dc.subject.keywordAuthorANTIFERROELECTRICS-
dc.subject.keywordAuthorCRYSTAL STRUCTURE-
dc.subject.keywordAuthorORDERING-
dc.subject.keywordAuthorPHASE TRANSITION-
dc.subject.keywordAuthorCOMPLEX PEROVSKITES-
dc.subject.keywordAuthorPB(MG1/2W1/2)O3-
dc.subject.keywordAuthorPB(CO1/2W1/2)O3-
dc.subject.keywordAuthorPB(YB1/2NB1/2)O3-
dc.subject.keywordPlusELECTRON-DIFFRACTION-
dc.subject.keywordPlusNEUTRON-DIFFRACTION-
dc.subject.keywordPlusPHASE-TRANSITIONS-
dc.subject.keywordPlusSOLID-SOLUTION-
dc.subject.keywordPlusPBZRO3-
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