Please use this identifier to cite or link to this item: http://hdl.handle.net/10773/36540
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dc.contributor.authorSalak, A.N.pt_PT
dc.contributor.authorCardoso, J.P.pt_PT
dc.contributor.authorKhalyavin, D.D.pt_PT
dc.contributor.authorBarbier, A.pt_PT
dc.contributor.authorFertey, P.pt_PT
dc.contributor.authorMikhalev, S.M.pt_PT
dc.contributor.authorOlekhnovich, N.M.pt_PT
dc.contributor.authorPushkarev, A.V.pt_PT
dc.contributor.authorRadyush, Yu V.pt_PT
dc.contributor.authorStanulis, A.pt_PT
dc.contributor.authorRamanauskas, R.pt_PT
dc.date.accessioned2023-03-09T16:12:11Z-
dc.date.available2023-03-09T16:12:11Z-
dc.date.issued2023-02-25-
dc.identifier.issn0022-4596pt_PT
dc.identifier.urihttp://hdl.handle.net/10773/36540-
dc.description.abstractCrystal structures of the high-pressure synthesized perovskite phases of the (1-x)BiFe0.5Sc0.5O3-xLaFe0.5Sc0.5O3 (0 ​= ​x ​≤ ​1) system and their temperature and pressure behaviours were studied using laboratory and synchrotron X-ray diffractions as well as neutron diffraction. At room temperature, the as-prepared phases with x ​≤ ​0.05 have an antipolar structure with the Pnma symmetry and with the √2ap ​× ​4ap ​× ​2√2ap superstructure (where ap is the pseudocubic perovskite unit-cell parameter). An incommensurately modulated phase with the Imma(00γ)s00 superspace group is observed for 0.10 ​= ​x ​≤ ​0.33, while a non-polar Pnma phase (√2ap ​× ​2ap ​× ​√2ap) is stable when x ​≥ ​0.34. The antipolar Pnma phase in the as-prepared samples with composition corresponding to x ​= ​0 transforms into the polar Ima2 one via irreversible annealing-caused transformation accompanied by a formation of a high-temperature intermediate polar R3c polymorph, while the antipolar Pnma phase in samples with x ​= ​0.05 is stable until the decomposition temperature. In the solid solutions with 0.10 ​= ​x ​≤ ​0.33, increasing temperature was found to result in a reversible transformation of the Imma(00γ)s00 phase into a non-polar Pnma one. The transition temperature decreases with increasing x. A hydrostatic pressure of few GPa was also shown to induce a reversible Imma(00γ)s00 → Pnma transformation.pt_PT
dc.language.isoengpt_PT
dc.publisherElsevierpt_PT
dc.relationinfo:eu-repo/grantAgreement/FCT/POR_CENTRO/SFRH%2FBD%2F145281%2F2019/PTpt_PT
dc.relationinfo:eu-repo/grantAgreement/FCT/6817 - DCRRNI ID/UIDB%2F50011%2F2020/PTpt_PT
dc.relationinfo:eu-repo/grantAgreement/FCT/6817 - DCRRNI ID/UIDP%2F50011%2F2020/PTpt_PT
dc.relationLA/P/0006/2020pt_PT
dc.rightsopenAccesspt_PT
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/pt_PT
dc.subjectHigh-pressure synthesispt_PT
dc.subjectMetastable perovskite phasept_PT
dc.subjectIncommensurate modulationpt_PT
dc.titleComposition-, temperature- and pressure-induced transitions between high-pressure stabilized perovskite phases of the (1-x)BiFe0.5Sc0.5O3 - xLaFe0.5Sc0.5O3 seriespt_PT
dc.typearticlept_PT
dc.description.versionpublishedpt_PT
dc.peerreviewedyespt_PT
degois.publication.titleJournal of Solid State Chemistrypt_PT
degois.publication.volume322pt_PT
dc.identifier.doi10.1016/j.jssc.2023.123937pt_PT
dc.identifier.essn1095-726Xpt_PT
dc.identifier.articlenumber123937pt_PT
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