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Updated: Jun 5, 2025

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
Published on: August 2, 2019
Collective energy gap of preformed Cooper pairs in disordered superconductors
Thomas Dubouchet1, Benjamin Sacépé2, Johanna Seidemann2
1Univ. Grenoble Alpes, CEA, INAC, PHELIQS, F-38000 Grenoble, France.
Abstract:
In most superconductors, the transition to the superconducting state is driven by the binding of electrons into Cooper pairs [1]. The condensation of these pairs into a single, phase coherent, quantum state takes place at the same time as their formation at the transition temperature, Tc . A different scenario occurs in some disordered, amorphous, superconductors: Instead of a pairing-driven transition, in-coherent Cooper pairs first pre-form above Tc , causing the opening of a pseudogap, and then, at Tc , condense into the phase coherent superconducting state [2-11]. Such a two-step scenario implies the existence of a new energy scale, Δ c , driving the collective superconducting transition of the preformed pairs [2-6]. Here we unveil this energy scale by means of Andreev spectroscopy [5, 12] in superconducting thin films of amorphous indium oxide. We observe two Andreev conductance peaks at ± Δ c that develop only below Tc and for highly disordered films on the verge of the transition to insulator. Our findings demonstrate that amorphous superconducting films provide prototypical disordered quantum systems to explore the collective superfluid transition of preformed Cooper-pairs.
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