1. A Josephson junction based on a highly disordered superconductor/low-resistivity normal metal bilayer
- Author
-
Pavel M. Marychev and Denis Yu. Vodolazov
- Subjects
Superconducting coherence length ,Josephson effect ,Materials science ,normal metal–superconductor bilayer ,General Physics and Astronomy ,02 engineering and technology ,lcsh:Chemical technology ,lcsh:Technology ,01 natural sciences ,Full Research Paper ,Electrical resistivity and conductivity ,Condensed Matter::Superconductivity ,Phase (matter) ,0103 physical sciences ,Nanotechnology ,lcsh:TP1-1185 ,General Materials Science ,Electrical and Electronic Engineering ,lcsh:Science ,010306 general physics ,Superconductivity ,Condensed matter physics ,lcsh:T ,Bilayer ,joule heating ,021001 nanoscience & nanotechnology ,lcsh:QC1-999 ,Nanoscience ,josephson junction ,lcsh:Q ,0210 nano-technology ,Joule heating ,Layer (electronics) ,lcsh:Physics - Abstract
We calculate the current–phase relation (CPR) of a SN-S-SN Josephson junction based on a SN bilayer of variable thickness composed of a highly disordered superconductor (S) and a low-resistivity normal metal (N) with proximity-induced superconductivity. In such a junction, the N layer provides both a large concentration of phase in the weak link and good heat dissipation. We find that when the thickness of the S and the N layer and the length of the S constriction are about the superconducting coherence length the CPR is single-valued and can be close to a sinusoidal shape. The product IcRn can reach Δ(0)/2|e| (Ic is the critical current of the junction, Rn is its normal-state resistance, Δ(0) is the superconductor gap of a single S layer at zero temperature). Our calculations show, that the proper choice of the thickness of the N layer leads both to nonhysteretic current–voltage characteristics even at low temperatures and a relatively large product IcRn.
- Published
- 2020
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