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dc.contributor.authorWinyard, Thomas
dc.contributor.authorSilaev, Mikhail
dc.contributor.authorBabaev, Egor
dc.date.accessioned2019-02-25T11:58:02Z
dc.date.available2019-02-25T11:58:02Z
dc.date.issued2019
dc.identifier.citationWinyard, T., Silaev, M., & Babaev, E. (2019). Hierarchies of length-scale based typology in anisotropic U(1)s-wave multiband superconductors. <i>Physical Review B</i>, <i>99</i>(6), Article 064509. <a href="https://doi.org/10.1103/PhysRevB.99.064509" target="_blank">https://doi.org/10.1103/PhysRevB.99.064509</a>
dc.identifier.otherCONVID_28933441
dc.identifier.otherTUTKAID_80731
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/62958
dc.description.abstractSince Ginzburg and Landau's seminal work in 1950, superconducting states have been classified by the hierarchy of the fundamental length scales of the theory, the magnetic-field penetration lengths and coherence lengths. In the simplest single-component case they form a dimensionless ratio κ. The model was generalized by Ginzburg for anisotropic materials in 1952. In this paper we expand the above length-scale analysis to anisotropic multicomponent superconductors that can have multiple coherence lengths as well as multiple magnetic-field penetration lengths, leading to unconventional length-scale hierarchies. We demonstrate that the anisotropies in multiband superconductors lead to new regimes with various mixed hierarchies in different directions. For example, a regime is possible, where for a field applied in a certain direction coherence lengths are smaller than the magnetic-field penetration lengths in one of the perpendicular directions, whereas the penetration lengths are larger in the other direction. Focusing on a model of a clean anisotropic multiband s-wave supercocoductors we show exampes of a new regime where vortex cores overlap in one direction, resulting in attractive core-core interaction, while in the orthogonal direction the magnetic-field penetration length exceeds the coherence lengths, leading to dominance of repulsive current-current interaction, resulting in an unconventional magnetic response.en
dc.format.mimetypeapplication/pdf
dc.languageeng
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.ispartofseriesPhysical Review B
dc.rightsCC BY 4.0
dc.subject.othermultiband superconductivity
dc.subject.othervortex lattices
dc.titleHierarchies of length-scale based typology in anisotropic U(1)s-wave multiband superconductors
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-201902221620
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.contributor.oppiaineFysiikkafi
dc.contributor.oppiaineNanoscience Centerfi
dc.contributor.oppiainePhysicsen
dc.contributor.oppiaineNanoscience Centeren
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.date.updated2019-02-22T13:15:13Z
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn2469-9950
dc.relation.numberinseries6
dc.relation.volume99
dc.type.versionpublishedVersion
dc.rights.copyright© 2019 American Physical Society
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber297439
dc.subject.ysosuprajohteet
dc.subject.ysosuprajohtavuus
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p9946
jyx.subject.urihttp://www.yso.fi/onto/yso/p9398
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevB.99.064509
dc.relation.funderSuomen Akatemiafi
dc.relation.funderResearch Council of Finlanden
jyx.fundingprogramAkatemiatutkija, SAfi
jyx.fundingprogramAcademy Research Fellow, AoFen
jyx.fundinginformationThe work was supported by the Swedish Research Council Grants No. 642-2013-7837 and No. VR2016-06122 and Goran Gustafsson Foundation for Research in Natural Sciences and Medicine and EPSERC Grant No. EP/P024688/1). M.S. was supported by the Academy of Finland (Project No. 297439). Part of this work was performed at the Aspen Center for Physics, which is supported by National Science Foundation Grant No. PHY-1607611.
dc.type.okmA1


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