Andreev bound states in a superconducting qubit at odd parity

Journal Article (2026)
Author(s)

Manuel Houzet (Université Grenoble Alpes)

Julia S. Meyer (Université Grenoble Alpes)

Yuli V. Nazarov (Kavli institute of nanoscience Delft, TU Delft - Applied Sciences)

Research Group
QN/Nazarov Group
DOI related publication
https://doi.org/10.1007/s10909-026-03398-4 Final published version
More Info
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Publication Year
2026
Language
English
Research Group
QN/Nazarov Group
Journal title
Journal of Low Temperature Physics
Issue number
3
Volume number
222
Article number
71
Downloads counter
8
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Abstract

The quantum mechanics of the Josephson effect is the core ingredient for quantum technologies with superconducting circuits. A new avenue was recently opened in this field by predicting that the Josephson quantum mechanics in the odd parity sector, when a quasiparticle is trapped in an Andreev bound state, is fundamentally different from the conventional one in the even sector. The focus was then on a Josephson junction surrounded by an electromagnetic environment formed of a collection of bosonic modes, including the case of an ohmic environment. Here we consider the distinct case of a superconducting qubit made of a single Josephson junction whose environment reduces to a capacitance. We find a novel structure for the low-lying discrete states in the odd sector, which is altogether different from the one that appears in the even sector. Our study of the bound-state spectrum ranges from the Coulomb-dominated (Cooper pair box) to the Josephson-dominated (transmon) regime. Our prediction could be tested in forthcoming experiments with superconductor/semiconductor/superconductor junctions, which have been studied intensively in recent years, both using nanowires as well as two-dimensional electron gases.