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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Keimer, Bernhard
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (8/8 displayed)
- 2024Quantifying the $U 5f$ covalence and degree of localization in U intermetallicscitations
- 2023Singlet magnetism in intermetallic $UGa_2$ unveiled by inelastic x-ray scatteringcitations
- 2023Phase formation in hole- and electron-doped rare-earth nickelate single crystalscitations
- 2023Coherent propagation of spin-orbit excitons in a correlated metalcitations
- 2021Formation mechanism of Ruddlesden–Popper faults in compressive-strained ABO3 perovskite superlatticescitations
- 2020Proximity effect in [Nb(1.5 nm)/Fe( x )]$_{10}$ /Nb(50 nm) superconductor/ferromagnet heterostructurescitations
- 2020Proximity effect in [Nb(1.5 nm)/Fe(x)]10/Nb(50 nm) superconductor/ferromagnet heterostructurescitations
- 2020Charge ordering in superconducting copper oxidescitations
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article
Proximity effect in [Nb(1.5 nm)/Fe(x)]10/Nb(50 nm) superconductor/ferromagnet heterostructures
Abstract
<jats:p>We have investigated the structural, magnetic and superconduction properties of [Nb(1.5 nm)/Fe(<jats:italic>x</jats:italic>)]<jats:sub>10</jats:sub> superlattices deposited on a thick Nb(50 nm) layer. Our investigation showed that the Nb(50 nm) layer grows epitaxially at 800 °C on the Al<jats:sub>2</jats:sub>O<jats:sub>3</jats:sub>(1−102) substrate. Samples grown at this condition possess a high residual resistivity ratio of 15–20. By using neutron reflectometry we show that Fe/Nb superlattices with <jats:italic>x <</jats:italic> 4 nm form a depth-modulated FeNb alloy with concentration of iron varying between 60% and 90%. This alloy has weak ferromagnetic properties. The proximity of this weak ferromagnetic layer to a thick superconductor leads to an intermediate phase that is characterized by a suppressed but still finite resistance of structure in a temperature interval of about 1 K below the superconducting transition of thick Nb. By increasing the thickness of the Fe layer to <jats:italic>x</jats:italic> = 4 nm the intermediate phase disappears. We attribute the intermediate state to proximity induced non-homogeneous superconductivity in the structure.</jats:p>