2010
DOI: 10.1103/physrevb.81.214518
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Josephson effect in superconductor/ferromagnet structures with a complex weak-link region

Abstract: The critical currents I C of SNF-FN-FNS, SN-FN-NS, and SNF-N-FNS Josephson junctions ͑Ssuperconductor, F-ferromagnetic, N-normal metal͒ with complex SNF or SN electrodes ͑N or NF bilayer are situated under a superconductor͒ are calculated in the framework of linearized Usadel equations for arbitrary overlap length d of SN interface. We demonstrate that in these geometries, in the case of large resistances of SN interfaces, the critical current can exceed that in ramp-type junctions. Based on these results, the… Show more

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Cited by 19 publications
(11 citation statements)
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References 60 publications
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“…is the sum [74] of the resistance of the bridge, R NB , and the resistances of two S-N interfaces, R SN ,…”
Section: Calculation Of Sn -N -Ns Junction Supercurrentmentioning
confidence: 99%
“…is the sum [74] of the resistance of the bridge, R NB , and the resistances of two S-N interfaces, R SN ,…”
Section: Calculation Of Sn -N -Ns Junction Supercurrentmentioning
confidence: 99%
“…is the sum [75] of the resistance of the bridge, R nb , and the resistances of two SN interfaces, R sn ,…”
Section: Calculation Of Sn-n-ns Junction Supercurrentmentioning
confidence: 99%
“…It was suggested recently in [47][48][49][50][51][52] to fabricate 'current in plane' SFS devices having a weak link region consisting of NF or FNF multilayers with the supercurrent flowing parallel to the FN interfaces. In these structures, superconductivity is induced from the S banks into the normal (N) film, while F films serve as a source of spin-polarized electrons, which diffuse from the F-layer to the N-layer, thus providing an effective exchange field in a weak link.…”
Section: Introductionmentioning
confidence: 99%
“…Its strength can be controlled [53,54] by transparencies of NF interfaces, as well as by the products of densities of states at the Fermi level, N F , N N , and film thicknesses, d F , d N . It was shown in [47][48][49][50][51] that the reduction of effective exchange energy in a weak link permits one to increase the decay length from the scale of the order of ∼1 up to ∼100 nm. The calculations performed in these papers did not go beyond a linear approximation in which the amplitude of the second harmonic in the CPR is small.…”
Section: Introductionmentioning
confidence: 99%