Balancing structure and performance: Optimized BZO nanorod doping in Ca-interlayered YBCO multilayers

dc.contributor.authorCondo, C.
dc.contributor.authorMejia, S.
dc.contributor.authorAye, M. M.
dc.contributor.authorRivasto, E.
dc.contributor.authorHuhtinen, H.
dc.contributor.authorPaturi, P.
dc.contributor.organizationfi=Wihurin fysiikantutkimuslaboratorio|en=Wihuri Physical Laboratory|
dc.contributor.organizationfi=hammaslääketieteen laitos|en=Institute of Dentistry|
dc.contributor.organization-code1.2.246.10.2458963.20.64787032594
dc.contributor.organization-code1.2.246.10.2458963.20.26581883332
dc.converis.publication-id509015193
dc.converis.urlhttps://research.utu.fi/converis/portal/Publication/509015193
dc.date.accessioned2026-06-15T20:11:24Z
dc.description.abstractThis study demonstrates the enhancement of critical current density over a wide temperature and magnetic field range in BZO-doped YBCO multilayer structures using a Ca-doped YBCO intermediate layer. Compared to single-layer BZO doped YBCO films, the Ca-doped interlayer improves crystalline quality and reduces non-uniform strain, particularly at low BZO doping concentrations, and promotes better growth of BZO nanorods. Additionally, multilayering slightly increases YBCO's oxygen content across all BZO concentrations, contributing to a higher critical temperature and zero-field critical current density. Besides of this, multilayering enhances critical current density across the magnetic field range, especially at low fields and high BZO concentrations. However, the highest absolute zero-f ield critical current density is achieved in undoped multilayered YBCO, whereas in fields above 2T and up to 50K, the best performance is obtained with 4% BZO-doped YBCO layers separated by Ca-doped interlayers. At around 1T, 2% BZO doping yields the highest critical current density. This paper also explores the possible mechanisms behind these effects, proposing that multilayering BZO-doped YBCO with a crystal structure-balancing interlayer could be key to next-generation YBCO coated conductors for high-temperature superconductor applications. Optimising the BZO concentration is crucial when tailoring YBCO compositions for different operating conditions.
dc.format.pagerange5
dc.format.pagerange1
dc.identifier.eissn2378-7074
dc.identifier.jour-issn1051-8223
dc.identifier.urihttps://www.utupub.fi/handle/11111/62017
dc.identifier.urlhttps://doi.org/10.1109/tasc.2026.3656256
dc.identifier.urnURN:NBN:fi-fe2026061571130
dc.language.isoen
dc.okm.affiliatedauthorCondo, Caius
dc.okm.affiliatedauthorMejia, Samuel
dc.okm.affiliatedauthorAye, Moe
dc.okm.affiliatedauthorRivasto, Elmeri
dc.okm.affiliatedauthorHuhtinen, Hannu
dc.okm.affiliatedauthorPaturi, Petriina
dc.okm.discipline114 Physical sciencesen_GB
dc.okm.discipline114 Fysiikkafi_FI
dc.okm.internationalcopublicationinternational co-publication
dc.okm.internationalityInternational publication
dc.okm.typeA1 ScientificArticle
dc.publisherInstitute of Electrical and Electronics Engineers (IEEE)
dc.publisher.countryUnited Statesen_GB
dc.publisher.countryYhdysvallat (USA)fi_FI
dc.publisher.country-codeUS
dc.relation.doi10.1109/TASC.2026.3656256
dc.relation.ispartofjournalIEEE Transactions on Applied Superconductivity
dc.titleBalancing structure and performance: Optimized BZO nanorod doping in Ca-interlayered YBCO multilayers
dc.year.issued2026

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