Show simple item record

dc.contributor.authorHijano, Alberto
dc.contributor.authorIlić, Stefan
dc.contributor.authorRouco, Mikel
dc.contributor.authorGonzález-Orellana, Carmen
dc.contributor.authorIlyn, Maxim
dc.contributor.authorRogero, Celia
dc.contributor.authorVirtanen, P.
dc.contributor.authorHeikkilä, T. T.
dc.contributor.authorKhorshidian, S.
dc.contributor.authorSpies, M.
dc.contributor.authorLigato, N.
dc.contributor.authorGiazotto, F.
dc.contributor.authorStrambini, E.
dc.contributor.authorBergeret, F. Sebastián
dc.date.accessioned2021-07-12T10:14:41Z
dc.date.available2021-07-12T10:14:41Z
dc.date.issued2021
dc.identifier.citationHijano, A., Ilić, S., Rouco, M., González-Orellana, C., Ilyn, M., Rogero, C., Virtanen, P., Heikkilä, T.T., Khorshidian, S., Spies, M., Ligato, N., Giazotto, F., Strambini, E., & Bergeret, F. S. (2021). Coexistence of superconductivity and spin-splitting fields in superconductor/ferromagnetic insulator bilayers of arbitrary thickness. <i>Physical Review Research</i>, <i>3</i>(2), Article 023131. <a href="https://doi.org/10.1103/PhysRevResearch.3.023131" target="_blank">https://doi.org/10.1103/PhysRevResearch.3.023131</a>
dc.identifier.otherCONVID_98977728
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/77101
dc.description.abstractFerromagnetic insulators (FI) can induce a strong exchange field in an adjacent superconductor (S) via the magnetic proximity effect. This manifests as spin splitting of the BCS density of states of the superconductor, an important ingredient for numerous superconducting spintronics applications and the realization of Majorana fermions. A crucial parameter that determines the magnitude of the induced spin splitting in FI/S bilayers is the thickness of the S layer d: In very thin samples, the superconductivity is suppressed by the strong magnetism. By contrast, in very thick samples, the spin splitting is absent at distances away from the interface. In this work, we calculate the density of states and critical exchange field of FI/S bilayers of arbitrary thickness. From here, we determine the range of parameters of interest for applications, where the exchange field and superconductivity coexist. We show that for d>3.0ξs, the paramagnetic phase transition is always of the second order, in contrast to the first-order transition in thinner samples at low temperatures. Here ξs is the superconducting coherence length. Finally, we compare our theory with the tunneling spectroscopy measurements in several EuS/Al/AlOx/Al samples. If the Al film in contact with the EuS is thinner than a certain critical value, we do not observe superconductivity, whereas, in thicker samples, we find evidence of a first-order phase transition induced by an external field. The complete transition is preceded by a regime in which normal and superconducting regions coexist. We attribute this mixed phase to inhomogeneities of the Al film thickness and the presence of superparamagnetic grains at the EuS/Al interface with different switching fields. The steplike evolution of the tunnel-barrier magnetoresistance supports this assumption. Our results demonstrate on the one hand, the important role of the S layer thickness, which is particularly relevant for the fabrication of high-quality samples suitable for applications. On the other hand, the agreement between theory and experiment demonstrates the accuracy of our theory, which, originally developed for homogeneous situations, is generalized to highly inhomogeneous systems.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review Research
dc.rightsCC BY 4.0
dc.titleCoexistence of superconductivity and spin-splitting fields in superconductor/ferromagnetic insulator bilayers of arbitrary thickness
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202107124286
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.description.reviewstatuspeerReviewed
dc.relation.issn2643-1564
dc.relation.numberinseries2
dc.relation.volume3
dc.type.versionpublishedVersion
dc.rights.copyright© Authors, 2021
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber317118
dc.subject.ysosuprajohtavuus
dc.subject.ysonanoelektroniikka
dc.subject.ysosuprajohteet
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p9398
jyx.subject.urihttp://www.yso.fi/onto/yso/p26991
jyx.subject.urihttp://www.yso.fi/onto/yso/p9946
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevResearch.3.023131
dc.relation.funderSuomen Akatemiafi
dc.relation.funderAcademy of Finlanden
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundingprogramAcademy Project, AoFen
jyx.fundinginformationF.S.B. acknowledges funding by the Spanish Ministerio de Ciencia, Innovación y Universidades (MICINN) (Project FIS2017-82804-P). T.T.H. acknowledges funding from the Academy of Finland (Project number 317118). A.H. acknowledges funding by the Department of Education of the Basque Government (Ikasiker grant). C.G.-O. acknowledges funding of the Ph.D. fellowship from MPC foundation. S.K. acknowledges for the fellowship of the ICTP Program for Training and Research in Italian laboratories, Trieste, Italy. C.R. acknowledges support from Gobierno Vasco (Grant No. IT 1255-19). F.G. acknowledges the European Research Council under the EU's Horizon 2020 Grant Agreement No. 899315-TERASEC for partial financial support. We acknowledge funding from EU's Horizon 2020 research and innovation program under Grant Agreement No. 800923 (SUPERTED). F.S.B. thanks the Institute of Solid State Theory at University of Münster for its kind hospitality.


Files in this item

Thumbnail

This item appears in the following Collection(s)

Show simple item record

CC BY 4.0
Except where otherwise noted, this item's license is described as CC BY 4.0