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<dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:invenio="http://invenio-software.org/elements/1.0" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd"><dc:identifier>doi:10.1016/j.jssc.2022.123525</dc:identifier><dc:language>eng</dc:language><dc:creator>Orera, Alodia</dc:creator><dc:creator>Oliete, Patricia B.</dc:creator><dc:creator>Merino, Rosa I.</dc:creator><dc:creator>Sanjuán, María Luisa</dc:creator><dc:title>Eutectic ceramics of the CeO2 – ZrO2 – MgO system produced by laser-assisted directional solidification</dc:title><dc:identifier>ART-2022-130718</dc:identifier><dc:description>Oxide eutectics have great potentiality as structural or functional materials, owing to the outstanding properties derived from the eutectic microstructure. Among them, the eutectic of the ZrO2 – MgO system is particularly noteworthy because of the unusual combination of thermomechanical, optical and electrical properties. In a recent application, Zr1-δMgδO2-δ – MgO eutectic oxides have been used to produce porous supports for molten-carbonate based CO2 separation membranes. Here we explore composite ceramic oxides of the CexZr1-xO2 – MgO (x ​≤ ​0.5) system with eutectic microstructure, with the motivation that incorporating cerium may enhance the CO2 permeation properties. Eutectic composites with different cerium content are produced by a laser-assisted directional solidification technique at variable solidification rate, v. In all cases the composite bicrystal consists of two phases, MgO and a fluorite-like (CexZr1-x)1-yMgyO2-y phase. A purely fibrilar microstructure is found for x ​≥ ​0.3 ​at v ​= ​25 ​mm/h, with MgO fibres embedded within the fluorite-like matrix. The MgO mol% in the eutectic composites decreases from ∼53% for x ​= ​0 to ∼48% for x ​= ​0.5. X-ray and Raman results evidence long-range ordering in a quasi-tetragonal monoclinic symmetry for x ​= ​0.5. Impedance spectroscopy results are consistent with a change from ionic to mainly electronic conductivity when the atmosphere is changed from air or Ar to 5%H2–Ar.</dc:description><dc:date>2022</dc:date><dc:source>http://zaguan.unizar.es/record/119928</dc:source><dc:doi>10.1016/j.jssc.2022.123525</dc:doi><dc:identifier>http://zaguan.unizar.es/record/119928</dc:identifier><dc:identifier>oai:zaguan.unizar.es:119928</dc:identifier><dc:relation>info:eu-repo/grantAgreement/ES/DGA/T02-20R</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MCINN/AEI/RYC2018-025553-I</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MCINN/FEDER/PID2019-107106RB-C32</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MCINN/FEDER/PID2021-124863OB-I00</dc:relation><dc:identifier.citation>JOURNAL OF SOLID STATE CHEMISTRY 315 (2022), 123525 [9 pp]</dc:identifier.citation><dc:rights>by-nc-nd</dc:rights><dc:rights>http://creativecommons.org/licenses/by-nc-nd/3.0/es/</dc:rights><dc:rights>info:eu-repo/semantics/openAccess</dc:rights></dc:dc>

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