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This study advances superconducting quantum computing by resolving decoherence mechanisms in fluxonium qubits, specifically addressing the challenge of isolating quasiparticle effects where charge-parity detection is unavailable. By incorporating superconducting gap asymmetry into theoretical models, researchers successfully constrain quasiparticle contributions across different junction elements to improve device fidelity and coherence times.
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Quasiparticle-induced transitions in a fluxonium qubit

arXiv2 min read

arXiv:2607.21329v1 Announce Type: new Abstract: Quasiparticles are a prominent decoherence source in superconducting qubits, but their effects are notoriously difficult to isolate in fluxonium. Unlike a transmon, fluxonium is insensitive to offset charge, precluding charge-parity detection of quasiparticle tunneling. We address this challenge by measuring the excitation and de-excitation rates in a fluxonium qubit under controlled on-chip quasiparticle injection. We show that to accurately model the external magnetic flux dependence of the quasiparticle-induced transition rates, it is necessary to account for the superconducting gap asymmetry across the Josephson junctions. A comparison between theory and experiment constrains the relative quasiparticle contributions of the junction array and the small junction and helps explain previously reported discrepancies between the bounds on the quasiparticle densities inferred for these two circuit elements.

Abstract:Quasiparticles are a prominent decoherence source in superconducting qubits, but their effects are notoriously difficult to isolate in fluxonium. Unlike a transmon, fluxonium is insensitive to offset charge, precluding charge-parity detection of quasiparticle tunneling. We address this challenge by measuring the excitation and de-excitation rates in a fluxonium qubit under controlled on-chip quasiparticle injection. We show that to accurately model the external magnetic flux dependence of the quasiparticle-induced transition rates, it is necessary to account for the superconducting gap asymmetry across the Josephson junctions. A comparison between theory and experiment constrains the relative quasiparticle contributions of the junction array and the small junction and helps explain previously reported discrepancies between the bounds on the quasiparticle densities inferred for these two circuit elements.

arXiv:2607.21329 [quant-ph]

(or arXiv:2607.21329v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2607.21329 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 213 words

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