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dc.contributor.authorBasbus, Juan F.es_ES
dc.contributor.authorArce, Mauricio D.es_ES
dc.contributor.authorNapolitano, Federico R.es_ES
dc.contributor.authorTroiani, Horacio E.es_ES
dc.contributor.authorAlonso, J. A.es_ES
dc.contributor.authorSaleta, Martín E.es_ES
dc.contributor.authorGonzález, Miguel A.es_ES
dc.contributor.authorCuello, G. J.es_ES
dc.contributor.authorFernández-Díaz, M. T.es_ES
dc.contributor.authorPardo Sainz, Migueles_ES
dc.contributor.authorBonanos, Nikolaoses_ES
dc.contributor.authorJimenez, Catalina E.es_ES
dc.contributor.authorGiebeler, Larses_ES
dc.contributor.authorFigueroa, Santiago J. A.es_ES
dc.contributor.authorCaneiro, Albertoes_ES
dc.contributor.authorSerquis, Adriana C.es_ES
dc.contributor.authorMogni, Liliana V.es_ES
dc.date.accessioned2020-09-04T07:40:42Z-
dc.date.available2020-09-04T07:40:42Z-
dc.date.issued2020-
dc.identifier.citationACS Applied Energy Materials 3(3): 2881-2892 (2020)es_ES
dc.identifier.issn2574-0962-
dc.identifier.urihttp://hdl.handle.net/10261/219098-
dc.description.abstractOxides with proton conductivity have a great potential for applications in environmental energy technology. Despite the BaCe0.4Zr0.4Y0.2O3−δ (BCZY) perovskites being well-known proton conductors, it is a challenge to determine the optimal operating temperature range where the energy applications benefit most from this unique property. The protonic transport properties strongly depend on crystal structure and local distortions in the participating cation coordination sphere, according to related temperatures and gas feed. The transport and crystallographic properties of BCZY were simultaneously studied by impedance spectroscopy (IS) and synchrotron X-ray diffraction (S-XRD). A strong correlation between conductivity and the lattice parameter, corresponding in principle to a cubic symmetry, was observed, mainly between 400 and 700 °C. The protonic conductivity range was analyzed by the H/D isotopic effect on the impedance spectra, which helped to identify protonic conduction as the governing transport mechanism below 600 °C, while the transport via oxygen vacancies dominates above this temperature. In order to assess the real crystallographic structure, the simultaneous refinement of laboratory XRD and neutron diffraction (ND) patterns was performed. According to this, BCZY changes from rhombohedral symmetry below 400 °C to cubic at 600 °C in a second-order phase transition. Complementary quasielastic neutron scattering (QENS) enables us to determine a protonic jump length of 3.1 Å, which matches the O–O distances in the octahedral oxygen coordination sphere around the cations. These results support the protonic self-diffusion through proton hopping between intraoctahedral O sites as the main transport mechanism up to 600 °C.es_ES
dc.description.sponsorshipThis work was supported by Agencia Nacional de Promocion de Ciencia y Tecnologia (ANPCyT) PICT-2016-2965 and PICT2014-1849, CONICET PIP-2015-0565, LNLS (Brazil), under proposals 20150099 and 20170278, and ILL (France) under proposal 7-03-168. L. Giebeler is grateful to the German Federal Ministry of Education and Research (BMBF) and the Argentinian Ministry of Science and Technology (MinCyT) for funding in the bilateral project DeFLeST (01DN14002). J. A. Alonso thanks the Spanish Ministry for Science, Innovation and Universities for funding the Project MAT2017-84496-R.es_ES
dc.language.isoenges_ES
dc.publisherAmerican Chemical Societyes_ES
dc.relationinfo:eu-repo/grantAgreement/AEI/Plan Estatal de Investigación Científica y Técnica y de Innovación 2017-2020/MAT2017-84496-Res_ES
dc.relationMAT2017-84496-R/AEI/10.13039/501100011033es_ES
dc.rightsclosedAccesses_ES
dc.titleRevisiting the crystal structure of BaCe0.4Zr0.4Y0.2O3−δ proton conducting perovskite and its correlation with transport propertieses_ES
dc.typeartículoes_ES
dc.identifier.doi10.1021/acsaem.9b02498-
dc.description.peerreviewedPeer reviewedes_ES
dc.relation.publisherversionhttps://doi.org/10.1021/acsaem.9b02498es_ES
dc.contributor.funderAgencia Nacional de Promoción Científica y Tecnológica (Argentina)es_ES
dc.contributor.funderConsejo Nacional de Investigaciones Científicas y Técnicas (Argentina)es_ES
dc.contributor.funderLaboratório Nacional de Luz Síncrotron (Brasil)es_ES
dc.contributor.funderFederal Ministry of Education and Research (Germany)es_ES
dc.contributor.funderMinisterio de Ciencia, Tecnología e Innovación Productiva (Argentina)es_ES
dc.contributor.funderAgencia Estatal de Investigación (España)es_ES
dc.contributor.funderMinisterio de Ciencia, Innovación y Universidades (España)es_ES
dc.relation.csices_ES
oprm.item.hasRevisionno ko 0 false*
dc.identifier.funderhttp://dx.doi.org/10.13039/501100002923es_ES
dc.identifier.funderhttp://dx.doi.org/10.13039/501100003074es_ES
dc.identifier.funderhttp://dx.doi.org/10.13039/501100011033es_ES
dc.identifier.funderhttp://dx.doi.org/10.13039/501100002347es_ES
dc.identifier.funderhttp://dx.doi.org/10.13039/501100003033es_ES
dc.type.coarhttp://purl.org/coar/resource_type/c_6501es_ES
item.languageiso639-1en-
item.fulltextNo Fulltext-
item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
item.cerifentitytypePublications-
item.grantfulltextnone-
item.openairetypeartículo-
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