Dissipative phases across the superconductor-to-insulator transition
Fran\c{c}ois Cou\"edo, Olivier Crauste, Anne-A\"elle Drillien, Vincent, Humbert, Laurent Berg\'e, Claire. A. Marrache-Kikuchi, Louis Dumoulin

TL;DR
This paper explores the complex phase diagram of amorphous NbSi thin films, revealing two metallic states between superconducting and insulating phases, influenced by disorder and film thickness, challenging traditional views of the superconductor-insulator transition.
Contribution
It identifies two distinct dissipative metallic phases in 2D amorphous NbSi films and links their emergence to inhomogeneous superconductivity destruction, expanding understanding of quantum phase transitions.
Findings
Two metallic phases exist between superconducting and insulating states.
Dissipative states have disorder-dependent resistance behavior.
Superconducting fluctuations promote metallic states.
Abstract
Competing phenomena in low dimensional systems can generate exotic electronic phases, either through symmetry breaking or a non-trivial topology. In two-dimensional (2D) systems, the interplay between superfluidity, disorder and repulsive interactions is especially fruitful in this respect although both the exact nature of the phases and the microscopic processes at play are still open questions. In particular, in 2D, once superconductivity is destroyed by disorder, an insulating ground state is expected to emerge, as a result of a direct superconductor-to-insulator quantum phase transition. In such systems, no metallic state is theoretically expected to survive to the slightest disorder. Here we map out the phase diagram of amorphous NbSi thin films as functions of disorder and film thickness, with two metallic phases in between the superconducting and insulating ones. These two…
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