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Mechanism of ferromagnetic resonance in ferromagnet-superconductor trilayers
KTH, School of Engineering Sciences (SCI), Applied Physics. V. G. Baryakhtar Institute of Magnetism of the National Academy of Sciences of Ukraine, Kyiv 03142, Ukraine.ORCID iD: 0000-0002-7663-6131
V. G. Baryakhtar Institute of Magnetism of the National Academy of Sciences of Ukraine, Kyiv 03142, Ukraine; Institute of Spintronics and Quantum Information, Faculty of Physics and Astronomy, Adam Mickiewicz University, Poznań, Uniwersytetu Poznańskiego 2, 61-614 Poznań, Poland, Poznań, Uniwersytetu Poznańskiego 2.ORCID iD: 0000-0002-2186-1382
KTH, School of Engineering Sciences (SCI), Applied Physics, Light and Matter Physics. V. G. Baryakhtar Institute of Magnetism of the National Academy of Sciences of Ukraine, Kyiv 03142, Ukraine.ORCID iD: 0000-0001-8754-3152
KTH, School of Engineering Sciences (SCI), Applied Physics, Light and Matter Physics.ORCID iD: 0000-0003-2339-1692
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2026 (English)In: Physical Review B, ISSN 2469-9950, E-ISSN 2469-9969, Vol. 113, no 1, p. 1-9, article id 014425Article in journal (Refereed) Published
Abstract [en]

Temperature dependent magnetic properties of superconductor-ferromagnet-superconductor (SC/FM/SC) trilayers are studied both experimentally and theoretically, with a focus on ferromagnetic resonance (FMR). The influence of the SC and FM layer thicknesses on the FMR field is examined. To differentiate the mechanisms involved, we additionally investigate structures containing nonmagnetic metallic (M) or insulating (I) spacers (SC/FM/M/SC or SC/FM/I/SC). All the studied multilayers show large reductions in the FMR field below the critical temperature of the SC, except the system containing an insulating spacer (SC/FM/I/SC). This SC-induced FMR-shift (resonance field/frequency) is larger for thicker SC as well as FM layers, reaching a saturation value for very large thicknesses. To explain the measured results, an analytical model is developed, in which the FM-magnetization precession modulates the magnetic flux in the system, thereby inducing an alternating supercurrent in the SC, which in turn produces a dynamic back-action magnetic field on the FM that shifts its resonance frequency. The model considers closed current loops, where the FM layer conductively links the supercurrents flowing in the opposite directions in the two outer SC layers. Our results provide a practical route for increasing the operating frequency of magnonic devices.

Place, publisher, year, edition, pages
American Physical Society (APS) , 2026. Vol. 113, no 1, p. 1-9, article id 014425
National Category
Condensed Matter Physics
Identifiers
URN: urn:nbn:se:kth:diva-377921DOI: 10.1103/blxk-m6pzISI: 001671902600004Scopus ID: 2-s2.0-105030342910OAI: oai:DiVA.org:kth-377921DiVA, id: diva2:2045008
Note

QC 20260311

Available from: 2026-03-11 Created: 2026-03-11 Last updated: 2026-03-11Bibliographically approved

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Popadiuk, DariiaKravets, AnatoliiKorenivski, Vladislav

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Popadiuk, DariiaKharlan, JuliaKravets, AnatoliiKorenivski, VladislavKłos, Jarosław W.Golub, Vladimir
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