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Proximity effect in [Nb(1.5 nm)/Fe(x)](10)/Nb(50 nm) superconductor/ferromagnet heterostructures
We have investigated the structural, magnetic and superconduction properties of [Nb(1.5 nm)/Fe(x)](10) 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(2)O(3)(1−102) substrate. Samples grown at this condition...
Autores principales: | , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Beilstein-Institut
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7445414/ https://www.ncbi.nlm.nih.gov/pubmed/32874825 http://dx.doi.org/10.3762/bjnano.11.109 |
Sumario: | We have investigated the structural, magnetic and superconduction properties of [Nb(1.5 nm)/Fe(x)](10) 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(2)O(3)(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 x < 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 x = 4 nm the intermediate phase disappears. We attribute the intermediate state to proximity induced non-homogeneous superconductivity in the structure. |
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