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dc.contributor.authorStrambini, E.
dc.contributor.authorSpies, M.
dc.contributor.authorLigato, N.
dc.contributor.authorIlić, S.
dc.contributor.authorRouco, M.
dc.contributor.authorGonzález-Orellana, Carmen
dc.contributor.authorIlyn, Maxim
dc.contributor.authorRogero, Celia
dc.contributor.authorBergeret, F. S.
dc.contributor.authorMoodera, J. S.
dc.contributor.authorVirtanen, Pauli
dc.contributor.authorHeikkilä, Tero T.
dc.contributor.authorGiazotto, F.
dc.date.accessioned2022-05-19T09:16:16Z
dc.date.available2022-05-19T09:16:16Z
dc.date.issued2022
dc.identifier.citationStrambini, E., Spies, M., Ligato, N., Ilić, S., Rouco, M., González-Orellana, C., Ilyn, M., Rogero, C., Bergeret, F. S., Moodera, J. S., Virtanen, P., Heikkilä, T. T., & Giazotto, F. (2022). Superconducting spintronic tunnel diode. <i>Nature Communications</i>, <i>13</i>, Article 2431. <a href="https://doi.org/10.1038/s41467-022-29990-2" target="_blank">https://doi.org/10.1038/s41467-022-29990-2</a>
dc.identifier.otherCONVID_144349563
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/81168
dc.description.abstractDiodes are key elements for electronics, optics, and detection. Their evolution towards low dissipation electronics has seen the hybridization with superconductors and the realization of supercurrent diodes with zero resistance in only one direction. Here, we present the quasi-particle counterpart, a superconducting tunnel diode with zero conductance in only one direction. The direction-selective propagation of the charge has been obtained through the broken electron-hole symmetry induced by the spin selection of the ferromagnetic tunnel barrier: a EuS thin film separating a superconducting Al and a normal metal Cu layer. The Cu/EuS/Al tunnel junction achieves a large rectification (up to ∼40%) already for a small voltage bias (∼200 μV) thanks to the small energy scale of the system: the Al superconducting gap. With the help of an analytical theoretical model we can link the maximum rectification to the spin polarization (P) of the barrier and describe the quasi-ideal Shockley-diode behavior of the junction. This cryogenic spintronic rectifier is promising for the application in highly-sensitive radiation detection for which two different configurations are evaluated. In addition, the superconducting diode may pave the way for future low-dissipation and fast superconducting electronics.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherSpringer Science and Business Media LLC
dc.relation.ispartofseriesNature Communications
dc.rightsCC BY 4.0
dc.titleSuperconducting spintronic tunnel diode
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202205192800
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.contributor.oppiaineNanoscience Centerfi
dc.contributor.oppiaineNanoscience Centeren
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn2041-1723
dc.relation.volume13
dc.type.versionpublishedVersion
dc.rights.copyright© The Author(s) 2022
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber800923
dc.relation.grantnumber800923
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/800923/EU//SUPERTED
dc.subject.ysosuprajohtavuus
dc.subject.ysosuprajohteet
dc.subject.ysoelektroniikka
dc.subject.ysodiodit
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p9398
jyx.subject.urihttp://www.yso.fi/onto/yso/p9946
jyx.subject.urihttp://www.yso.fi/onto/yso/p4890
jyx.subject.urihttp://www.yso.fi/onto/yso/p13006
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1038/s41467-022-29990-2
dc.relation.funderEuropean Commissionen
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramFET Future and Emerging Technologies, H2020en
jyx.fundingprogramFET Future and Emerging Technologies, H2020fi
jyx.fundinginformationThis work was mainly supported by the EU’s Horizon 2020 research and innovation program under Grant Agreement No. 800923 (SUPERTED) funding all the authors. E.S. and F.G. acknowledge the European Research Council under Grant Agreement No. 899315 (TERASEC), and the EU’s Horizon 2020 research and innovation program under Grant Agreement No. 964398 (SUPERGATE) for partial financial support. M.S. and E.S. acknowledge partial funding from the European Union’s Horizon 2020 research and innovation program under the Marie Skłodowska Curie Action IF Grant No. 101022473 (SuperCONtacts). J.M. acknowledges financial support in the USA by the Army Research Office (grant ARO W911NF-20-2-0061), ONR (grant N00014-20-1-2306), NSF (grant DMR 1700137) and NSF C-Accel Track C Grant No. 2040620. The work of F.S.B., C.R. and M.I. was supported by the Spanish Ministerio de Ciencia e Innovacion (MICINN) through Project PID2020-114252GB-I00 (SPIRIT). F.S.B. acknowledges financial support by the A. v. Humboldt Foundation.
datacite.isSupplementedBy.doi10.17011/jyx/dataset/93202
datacite.isSupplementedBy.doi10.17011/jyx/dataset/93203
datacite.isSupplementedByVirtanen, Pauli. (2024). <i>Computer simulations for properties of spin-split S/FI structures and tunnel junctions (parent dataset)</i>. University of Jyväskylä. <a href="https://doi.org/10.17011/jyx/dataset/93202" target="_blank">https://doi.org/10.17011/jyx/dataset/93202</a>. <a href="http://urn.fi/URN:NBN:fi:jyu-202402011709">https://urn.fi/URN:NBN:fi:jyu-202402011709</a>
datacite.isSupplementedByVirtanen, Pauli. (2024). <i>Computer simulations for properties of spin-split S/FI structures and tunnel junctions</i>. V. 25.1.2024. University of Jyväskylä. <a href="https://doi.org/10.17011/jyx/dataset/93203" target="_blank">https://doi.org/10.17011/jyx/dataset/93203</a>. <a href="http://urn.fi/URN:NBN:fi:jyu-202402011710">https://urn.fi/URN:NBN:fi:jyu-202402011710</a>
dc.type.okmA1


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