Critical temperatures and critical currents of wide and narrow quasi-one-dimensional superconducting aluminum structures in zero magnetic field
V. I. Kuznetsov, O. V. Trofimov
TLDR
Narrower quasi-one-dimensional superconducting aluminum structures exhibit lower critical temperatures and currents due to boundary effects.
Key contributions
- Found narrower Al structures have lower critical temperature and critical current density.
- Proposes depairing centers at dirty boundaries strongly influence narrower structures.
- Observed two distinct temperature-dependent critical current behaviors in these structures.
- Critical current follows Kupriyanov-Lukichev theory at low temps and Josephson current at high temps.
Why it matters
This paper reveals how geometric confinement impacts critical properties in quasi-one-dimensional superconductors. These findings are vital for understanding fundamental physics and for designing advanced nanoscale superconducting devices, where precise control over critical parameters is essential.
Original Abstract
We measured the critical temperatures and critical switching and retrapping currents of wide and narrow thin-film quasi-one-dimensional superconducting aluminum structures of the same thickness in zero magnetic field. For the first time, we found that the narrower the structure, the lower the critical temperature and critical current density in the structure. Probably, the influence of depairing centers that are on dirty longitudinal boundaries of the structure, is the stronger than the narrower the structure. It is found for the first time that, in most cases, the temperature-dependent switching critical current in both structures is approximated by two functions. At temperatures below the temperature corresponding to the bottom of the resistive N-S transition of structures, the switching critical current is described by the Kupriyanov-Lukichev theory. At temperatures close to the top of the N-S transition, the switching current is linear with temperature and coincides with the critical Josephson current. At these temperatures, Josephson SNS junctions are formed in structures.
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