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dc.contributor.authorNavavan Thongmeeen_US
dc.contributor.authorAnucha Wacharapasornen_US
dc.contributor.authorSukanda Jiansirisomboonen_US
dc.date.accessioned2018-09-10T03:18:56Z-
dc.date.available2018-09-10T03:18:56Z-
dc.date.issued2009-12-01en_US
dc.identifier.issn15635112en_US
dc.identifier.issn00150193en_US
dc.identifier.other2-s2.0-77749304224en_US
dc.identifier.other10.1080/00150190902889473en_US
dc.identifier.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=77749304224&origin=inwarden_US
dc.identifier.urihttp://cmuir.cmu.ac.th/jspui/handle/6653943832/59650-
dc.description.abstractThe ceramics with formula (1-x)PZT - xBLT were fabricated by a solid-state reaction method. X-ray diffractometry indicated complete solid solutions occurred for all compositions. Perovskite phase with tetragonal crystal structure and corresponding lattice distortion was observed. PZT-rich ceramics also possessed relatively high densities due to their more equiaxed grains with high packing capability compared to the ceramics with an addition of plate-shaped BLT. Measurement of dielectric constant indicated a gradual decrease with increasing BLT content. PZT ceramic exhibited a peak of phase transition, while broader peak were seen for PZT - BLT solid solutions, suggesting more diffuse transformation occurred due to an addition of BLT. A shift of transition temperature (Tc) to lower temperature was also observed in the PZT - BLT solid solutions. Copyright © Taylor & Francis Group, LLC.en_US
dc.subjectMaterials Scienceen_US
dc.subjectPhysics and Astronomyen_US
dc.titleDielectric properties of complex structured (1-x)Pb(Zr<inf>0.52</inf>Ti<inf>0.48</inf>)O<inf>3</inf>- X(Bi<inf>3.25</inf>La<inf>0.75</inf>)Ti<inf>3</inf>O<inf>12</inf>ceramicsen_US
dc.typeJournalen_US
article.title.sourcetitleFerroelectricsen_US
article.volume384en_US
article.stream.affiliationsChiang Mai Universityen_US
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