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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