{"title":"Phase structure of the ceramic samples of the BiScO3–PbTiO3–PbMg⅓Nb⅔O3 system near the morphotropic phase boundary studied by the Rietveld method","authors":"Vladimir Sirotinkin, Alexandr Bush, Maksim Sysoev","doi":"10.1515/zkri-2024-0065","DOIUrl":null,"url":null,"abstract":"An X-ray diffraction study of ceramic samples of the BiScO<jats:sub>3</jats:sub>–PbTiO<jats:sub>3</jats:sub>–PbMg<jats:sub>⅓</jats:sub>Nb<jats:sub>⅔</jats:sub>O<jats:sub>3</jats:sub> system with compositions close to the morphotropic phase boundary was carried out at room temperature. The existence of wide areas of solid solutions has been established. The symmetry of the PbTiO<jats:sub>3</jats:sub>-based solid solutions is tetragonal (space group <jats:italic>P</jats:italic>4<jats:italic>mm</jats:italic>). The symmetry of the PbMg<jats:sub>⅓</jats:sub>Nb<jats:sub>⅔</jats:sub>O<jats:sub>3</jats:sub>-based solid solutions is cubic (space group <jats:italic>Pm</jats:italic> <jats:inline-formula> <jats:alternatives> <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"> <m:mrow> <m:mover accent=\"true\"> <m:mn>3</m:mn> <m:mo>‾</m:mo> </m:mover> </m:mrow> </m:math> <jats:tex-math>$\\overline{3}$</jats:tex-math> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_zkri-2024-0065_ineq_201.png\" /> </jats:alternatives> </jats:inline-formula> <jats:italic>m</jats:italic>). Near the BiScO<jats:sub>3</jats:sub> side, the solid solutions are rhombohedral (space group <jats:italic>R</jats:italic>3<jats:italic>m</jats:italic>). During the morphotropic phase transition from the cubic solid solutions to the tetragonal ones, additional phases appear. If a tetragonal phase prevails ((1 − 2<jats:italic>x</jats:italic>)BiScO<jats:sub>3</jats:sub>–<jats:italic>x</jats:italic>PbTiO<jats:sub>3</jats:sub>–<jats:italic>x</jats:italic>PbMg<jats:sub>⅓</jats:sub>Nb<jats:sub>⅔</jats:sub>O<jats:sub>3</jats:sub> <jats:italic>x</jats:italic> = 0.46; (1 − 2<jats:italic>x</jats:italic>)BiScO<jats:sub>3</jats:sub>–1.1<jats:italic>x</jats:italic>PbTiO<jats:sub>3</jats:sub>–0.9<jats:italic>x</jats:italic>PbMg<jats:sub>⅓</jats:sub>Nb<jats:sub>⅔</jats:sub>O<jats:sub>3</jats:sub> <jats:italic>x</jats:italic> = 0.45 and 0.42), a satisfactory model is a model with a minority cubic phase (space group <jats:italic>Pm</jats:italic> <jats:inline-formula> <jats:alternatives> <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"> <m:mrow> <m:mover accent=\"true\"> <m:mn>3</m:mn> <m:mo>‾</m:mo> </m:mover> </m:mrow> </m:math> <jats:tex-math>$\\overline{3}$</jats:tex-math> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_zkri-2024-0065_ineq_001.png\" /> </jats:alternatives> </jats:inline-formula> <jats:italic>m</jats:italic>). If a cubic phase prevails ((1 − 2<jats:italic>x</jats:italic>)BiScO<jats:sub>3</jats:sub>–1.1<jats:italic>x</jats:italic>PbTiO<jats:sub>3</jats:sub>–0.9<jats:italic>x</jats:italic>PbMg<jats:sub>⅓</jats:sub>Nb<jats:sub>⅔</jats:sub>O<jats:sub>3</jats:sub> <jats:italic>x</jats:italic> = 0.39 and 0.36; (1 − 2<jats:italic>x</jats:italic>)BiScO<jats:sub>3</jats:sub>–0.8<jats:italic>x</jats:italic>PbTiO<jats:sub>3</jats:sub>–1.2<jats:italic>x</jats:italic>PbMg<jats:sub>⅓</jats:sub>Nb<jats:sub>⅔</jats:sub>O<jats:sub>3</jats:sub> <jats:italic>x</jats:italic> = 0.4), a model with a minority monoclinic phase (space group <jats:italic>Cm</jats:italic>) or with two minority phases: tetragonal (space group <jats:italic>P</jats:italic>4<jats:italic>mm</jats:italic>) and monoclinic (space group <jats:italic>Cm</jats:italic>) is satisfactory.","PeriodicalId":23855,"journal":{"name":"Zeitschrift für Kristallographie - Crystalline Materials","volume":"7 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-04-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Zeitschrift für Kristallographie - Crystalline Materials","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1515/zkri-2024-0065","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
An X-ray diffraction study of ceramic samples of the BiScO3–PbTiO3–PbMg⅓Nb⅔O3 system with compositions close to the morphotropic phase boundary was carried out at room temperature. The existence of wide areas of solid solutions has been established. The symmetry of the PbTiO3-based solid solutions is tetragonal (space group P4mm). The symmetry of the PbMg⅓Nb⅔O3-based solid solutions is cubic (space group Pm3‾$\overline{3}$m). Near the BiScO3 side, the solid solutions are rhombohedral (space group R3m). During the morphotropic phase transition from the cubic solid solutions to the tetragonal ones, additional phases appear. If a tetragonal phase prevails ((1 − 2x)BiScO3–xPbTiO3–xPbMg⅓Nb⅔O3x = 0.46; (1 − 2x)BiScO3–1.1xPbTiO3–0.9xPbMg⅓Nb⅔O3x = 0.45 and 0.42), a satisfactory model is a model with a minority cubic phase (space group Pm3‾$\overline{3}$m). If a cubic phase prevails ((1 − 2x)BiScO3–1.1xPbTiO3–0.9xPbMg⅓Nb⅔O3x = 0.39 and 0.36; (1 − 2x)BiScO3–0.8xPbTiO3–1.2xPbMg⅓Nb⅔O3x = 0.4), a model with a minority monoclinic phase (space group Cm) or with two minority phases: tetragonal (space group P4mm) and monoclinic (space group Cm) is satisfactory.