Upper critical field in trilayer ferromagnet-superconductor-ferromagnet (FSF) structures
Upper critical magnetic field Hc2 in geometries parallel and perpendicular to the heterostructure surface in thin film ferromagnet–superconductor–ferromagnet trilayer spin-valve cores is studied theoretically and experimentally. A wedge deposition technique is used for single-run preparation of a se...
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D.Ghitu Institute of Electronic Engineering and Nanotechnologies
2013
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oai:doaj.org-article:cd19e2e3a511402999638fc3c420162d2021-11-21T12:00:21ZUpper critical field in trilayer ferromagnet-superconductor-ferromagnet (FSF) structures2537-63651810-648Xhttps://doaj.org/article/cd19e2e3a511402999638fc3c420162d2013-09-01T00:00:00Zhttps://mjps.nanotech.md/archive/2013/article/27695https://doaj.org/toc/1810-648Xhttps://doaj.org/toc/2537-6365Upper critical magnetic field Hc2 in geometries parallel and perpendicular to the heterostructure surface in thin film ferromagnet–superconductor–ferromagnet trilayer spin-valve cores is studied theoretically and experimentally. A wedge deposition technique is used for single-run preparation of a set of samples with thickness dF1 of the bottom and dF2 of the top ferromagnet (F) Cu41Ni59. The critical field Hc2 is measured in a temperature range of 0.4–8 K and magnetic fields of up to 9 T. A transition from an oscillatory to reentrant behavior of the superconducting transition temperature versus F-layer thickness induced by an external magnetic field is observed for the first time. To correctly interpret the experimental data, we develop a quasiclassical theory, which makes it possible to estimate the temperature dependence of the critical field and the superconducting transition temperature for an arbitrary set of system parameters. A fairly good agreement between our theoretical predictions and experimental data is demonstrated for all samples, using a single set of fit parameters. This confirms the adequacy of the Fulde–Ferrell–Larkin–Ovchinnikov (FFLO) physics in determining the unusual superconducting properties of the studied Cu41Ni59/Nb/ Cu41Ni59 spin-valve core trilayers.Antropov, EvgheniD.Ghitu Institute of Electronic Engineering and NanotechnologiesarticlePhysicsQC1-999ElectronicsTK7800-8360ENMoldavian Journal of the Physical Sciences, Vol 12, Iss 1-2, Pp 44-50 (2013) |
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Physics QC1-999 Electronics TK7800-8360 |
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Physics QC1-999 Electronics TK7800-8360 Antropov, Evgheni Upper critical field in trilayer ferromagnet-superconductor-ferromagnet (FSF) structures |
description |
Upper critical magnetic field Hc2 in geometries parallel and perpendicular to the heterostructure surface in thin film ferromagnet–superconductor–ferromagnet trilayer spin-valve cores is studied theoretically and experimentally. A wedge deposition technique is used for single-run preparation of a set of samples with thickness dF1 of the bottom and dF2 of the top ferromagnet (F) Cu41Ni59. The critical field Hc2 is measured in a temperature range of 0.4–8 K and magnetic fields of up to 9 T. A transition from an oscillatory to reentrant behavior of the superconducting transition temperature versus F-layer thickness induced by an external magnetic field is observed for the first time. To correctly interpret the experimental data, we develop a quasiclassical theory, which makes it possible to estimate the temperature dependence of the critical field and the superconducting transition temperature for an arbitrary set of system parameters. A fairly good agreement between our theoretical predictions and experimental data is demonstrated for all samples, using a single set of fit parameters. This confirms the adequacy of the Fulde–Ferrell–Larkin–Ovchinnikov (FFLO) physics in determining the unusual superconducting properties of the studied Cu41Ni59/Nb/ Cu41Ni59 spin-valve core trilayers. |
format |
article |
author |
Antropov, Evgheni |
author_facet |
Antropov, Evgheni |
author_sort |
Antropov, Evgheni |
title |
Upper critical field in trilayer ferromagnet-superconductor-ferromagnet (FSF) structures |
title_short |
Upper critical field in trilayer ferromagnet-superconductor-ferromagnet (FSF) structures |
title_full |
Upper critical field in trilayer ferromagnet-superconductor-ferromagnet (FSF) structures |
title_fullStr |
Upper critical field in trilayer ferromagnet-superconductor-ferromagnet (FSF) structures |
title_full_unstemmed |
Upper critical field in trilayer ferromagnet-superconductor-ferromagnet (FSF) structures |
title_sort |
upper critical field in trilayer ferromagnet-superconductor-ferromagnet (fsf) structures |
publisher |
D.Ghitu Institute of Electronic Engineering and Nanotechnologies |
publishDate |
2013 |
url |
https://doaj.org/article/cd19e2e3a511402999638fc3c420162d |
work_keys_str_mv |
AT antropovevgheni uppercriticalfieldintrilayerferromagnetsuperconductorferromagnetfsfstructures |
_version_ |
1718419330429878272 |