One Extra Electron Reshapes a Quantum Bit express

Original: "Andreev bound states in a superconducting qubit at odd parity"
arXiv:2601.23100 · 2026-01-30 · CC BY 4.0 · 1 min
In a superconducting circuit, a trapped electron rearranges energy levels like an extra passenger in a crowded car.

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A superconducting qubit is a tiny electrical circuit that behaves like an artificial atom. In its normal state, current flows through it without resistance, and the energy levels are evenly spaced, like steps on a staircase. But if a single electron gets stuck in the circuit, everything changes. That extra electron is like a passenger who squeezes into an overcrowded car: it doesn't just take up space: it forces everyone else to shift and rearrange.

The authors calculated what the energy levels look like in such a qubit with one stuck electron. It turns out they line up in a completely different order than in a normal qubit without the extra electron. Moreover, this order depends on which is stronger: the electric field that holds the electrons, or the ability of the current to flow without resistance. It's as if passengers in a crowded car reseat themselves differently depending on how much the train shakes.

One extra electron doesn't just change a single step on the staircase: it changes the whole shape of the staircase, just as one unexpected guest can change the seating arrangement at a table.

This behavior could be tested in experiments with hybrid superconductors, which combine a superconductor with a regular semiconductor. In recent years, researchers have learned to make these structures very carefully — both from thin wires and from flat layers where electrons move as if on a highway. If the prediction holds up, it would offer a new way to control quantum bits — simply by adding or removing one electron.

Original abstract

as written by the authors arXiv:2601.23100

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 in 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.

In a superconducting qubit, one extra electron can change the system's energy as noticeably as one wrong note changes a melody.

Scientists
Niels BohrPascual JordanWerner HeisenbergWolfgang PauliEmmy NoetherDavid Deutsch
Concepts
josephson current Josephson effect transmon qubit triplet superconductivity bound state supersymmetric quantum mechanics superconductivity electron pairing Cooper pair aluminum oxide superconducting electronics state single qubit operation anyon non abelian anyons superconducting phase transition quantum order disorder boundary conditions semiconductor qubits edge states