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Extinction and Recovery of Superconductivity by Interference in Superconductor/Ferromagnet Bilayers

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dc.contributor.author SIDORENKO, A. S.
dc.contributor.author ZDRAVKOV, V. I.
dc.contributor.author KEHRLE, J.
dc.contributor.author MORARI, R.
dc.contributor.author ANTROPOV, E.
dc.contributor.author OBERMEIER, G.
dc.contributor.author GSELL, S.
dc.contributor.author SCHRECK, M.
dc.contributor.author MÜLLER, C.
dc.contributor.author RYAZANOV, V. V.
dc.contributor.author HORN, S.
dc.contributor.author TIDECKS, R.
dc.contributor.author TAGIROV, L. R.
dc.date.accessioned 2020-12-02T11:19:47Z
dc.date.available 2020-12-02T11:19:47Z
dc.date.issued 2009
dc.identifier.citation A. S. SIDORENKO V. I. ZDRAVKOV J. KEHRLE R. et al. Extinction and Recovery of Superconductivity by Interference in Superconductor/Ferromagnet Bilayers. In: Nanoscale Phenomena. NanoScience and Technology, 2009, pp. 3-11. ISBN 978-3-642-00708-8. en_US
dc.identifier.uri https://doi.org/10.1007/978-3-642-00708-8_1
dc.identifier.uri http://repository.utm.md/handle/5014/11890
dc.description Acces full text: https://doi.org/10.1007/978-3-642-00708-8_1 en_US
dc.description.abstract In superconductor–ferromagnet (S/F) metallic contacts, the superconducting condensate penetrates through the S/F interface into a ferromagnetic layer. In contrast to the conventional S/N proximity effect, the pairing wave function not only decays deep into the F metal, but simultaneously oscillates. Interference of the oscillating pairing function in a ferromagnetic film gives rise to a modulation of the pairing function flux crossing the S/F interface, which results in oscillations of superconducting transition temperature of the adjacent S layer. In this work, we report on the experimental observation of the superconductivity reentrance phenomenon with double suppression of the superconductivity in Nb ∕ Cu1 − x Ni x bilayers as a function of the ferromagnetic layer thickness, d CuNi. The superconducting T c drops sharply with increasing d CuNi till total suppression of superconductivity at d CuNi ≈ 2. 5 nm. At a further increase of the Nb ∕ Cu1 − x Ni x layer thickness, the superconductivity restores at d CuNi ≥ 24 nm. Then, with the subsequent increase of d CuNi, the superconductivity vanishes again at d CuNi ≈ 38 nm. en_US
dc.language.iso en en_US
dc.publisher Springer Nature Switzerland en_US
dc.rights Attribution-NonCommercial-NoDerivs 3.0 United States *
dc.rights.uri http://creativecommons.org/licenses/by-nc-nd/3.0/us/ *
dc.subject superconducting condensate en_US
dc.subject spectrometry en_US
dc.subject ferromagnetic layers en_US
dc.subject layers en_US
dc.subject metallic contacts en_US
dc.subject pairing en_US
dc.subject splitting en_US
dc.subject superconductivity en_US
dc.title Extinction and Recovery of Superconductivity by Interference in Superconductor/Ferromagnet Bilayers en_US
dc.type Book chapter en_US


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