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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:10.1002/aelm.202400962</dc:identifier><dc:language>eng</dc:language><dc:creator>Lafuerza, Sara</dc:creator><dc:creator>Blasco, Javier</dc:creator><dc:creator>Evangelisti, Marco</dc:creator><dc:creator>Subías, Gloria</dc:creator><dc:creator>Gracia, David</dc:creator><dc:creator>Pardo, José Á.</dc:creator><dc:creator>Barriuso, Eduardo</dc:creator><dc:creator>Torrelles, Xavier</dc:creator><dc:creator>Padilla-Pantoja, Jessica</dc:creator><dc:creator>Caicedo, José M.</dc:creator><dc:creator>Santiso, José</dc:creator><dc:title>High‐quality epitaxial five‐layer aurivillius films with in‐plane ferroelectricity for electrocaloric cooling</dc:title><dc:identifier>ART-2025-144348</dc:identifier><dc:description>High‐quality purely c‐axis oriented epitaxial thin films of the Aurivillius phase Sr2Bi4Ti5O18 with n = 5 (Sr,Bi)TiO3 perovskite‐like layers, are grown on SrTiO3 substrates by pulsed laser deposition. The highest crystalline quality is obtained with a 20 wt.% Bi‐excess target and average stacking order values in the proximity of the ideal value n = 5 are attained for an optimum deposition temperature of 650 °C. Scanning transmission electron microscopy reveals regions with n ranging from 4 to 6 around an average thickness of n = 5, in agreement with the X‐ray diffraction analysis. Interdigital electrodes are used to probe the in‐plane polarization and survey the electrocaloric properties. A maximum adiabatic temperature change of ΔT ∼ 0.95 °C for an electric field of 150 kV cm−1 is observed at ≈135 °C. Larger values are expected at higher temperatures around the ferroelectric Curie temperature, TC. Since TC of Sr2Bi4Ti5O18 can be tuned by codoping, the findings pave the way toward a large electrocaloric effect at ambient temperature.</dc:description><dc:date>2025</dc:date><dc:source>http://zaguan.unizar.es/record/161716</dc:source><dc:doi>10.1002/aelm.202400962</dc:doi><dc:identifier>http://zaguan.unizar.es/record/161716</dc:identifier><dc:identifier>oai:zaguan.unizar.es:161716</dc:identifier><dc:relation>info:eu-repo/grantAgreement/ES/AEI/CEX2023-001263-S</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/DGA/E11-23R</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/DGA/E12-23R</dc:relation><dc:relation>info:eu-repo/grantAgreement/EC/H2020/101007825/EU/ULtra ThIn MAgneto Thermal sEnsor-Ing/ULTIMATE-I</dc:relation><dc:relation>This project has received funding from the European Union’s Horizon 2020 research and innovation program under grant agreement No H2020 101007825-ULTIMATE-I</dc:relation><dc:relation>info:eu-repo/grantAgreement/EC/H2020/101029019/EU/Exploring Aurivillius phases for Green Electrocaloric Refrigeration/EAGER</dc:relation><dc:relation>This project has received funding from the European Union’s Horizon 2020 research and innovation program under grant agreement No H2020 101029019-EAGER</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MICINN/CEX2021-001214-S</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MICINN/CEX2023-001286-S</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MICINN/PID2021-123276OB-I00</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MICINN/PID2021-124734OB-C21</dc:relation><dc:identifier.citation>Advanced Electronic Materials (2025), 2400962 [10 pp.]</dc:identifier.citation><dc:rights>by</dc:rights><dc:rights>https://creativecommons.org/licenses/by/4.0/deed.es</dc:rights><dc:rights>info:eu-repo/semantics/openAccess</dc:rights></dc:dc>

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