Multiple Quasiparticle Bound States in a Trap Created by a Local Superconducting Gap Variation

TL;DR

This paper investigates how local variations in the superconducting gap create multiple bound states for quasiparticles, affecting their dynamics and recombination, with implications for superconducting device performance.

Contribution

It introduces a model showing multiple bound states due to gap variations and analyzes their dependence on trap parameters, extending understanding beyond semiclassical approximations.

Findings

Multiple bound states exist in gap variations, depending on trap size and depth.

Infinite bound states appear near the gap edge in higher dimensions.

Results impact understanding of quasiparticle recombination in disordered superconductors.

Abstract

At low temperature, the concentration of quasiparticles observed in superconducting circuits far exceeds the predictions of microscopic BCS theory at equilibrium. As a source of dissipation, these excess quasiparticles degrade the performance of various devices. Therefore, understanding their dynamics, especially their recombination into Cooper pairs, is an active topic of current research. In disordered superconductors, spatial fluctuations in the superconducting gap can trap quasiparticles and modify their eigenspectrum. Since this spectrum plays a key role in quasiparticle dynamics, it must be carefully investigated. To this end, we introduce a toy model of a single trap. Specifically, we consider a shallow disk-shaped gap variation in a clean superconductor. Using a semiclassical approximation, we demonstrate the existence of multiple bound states and give the dependence of their number on the size and depth of the gap suppression. Extending our analysis beyond the semiclassical regime, in dimensions larger than one, we observe an infinite number of bound states very close to the gap edge, even for an arbitrarily small trap. These results deepen our understanding of trapped quasiparticles and may have important implications for their recombination in disordered superconductors.