Collective energy gap of preformed Cooper pairs in disordered superconductors

无序超导体中预形成库珀对的集体能隙

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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, T(c) . A different scenario occurs in some disordered, amorphous, superconductors: Instead of a pairing-driven transition, in-coherent Cooper pairs first pre-form above T(c) , causing the opening of a pseudogap, and then, at T(c) , 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 T(c) 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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