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This paper proposes using superconducting qubits as direct scattering targets for particle detection, leveraging their microwave-level spacings to resolve device geometry against incident particles with significantly higher momentum transfer. By treating the qubit's transition response as a differential scattering cross-section kernel, this approach opens sensitivity to the eV-to-keV dark matter mass regime largely inaccessible to current experiments. The work represents a significant theoretical advance at the intersection of quantum circuit design and fundamental particle physics detection methods.
Source coveringarXiv

Superconducting Qubits as Quantum Targets for Direct Particle Scattering

arXiv2 min read

arXiv:2611.05469v1 Announce Type: cross Abstract: We introduce a novel approach to particle detection in which a superconducting qubit itself serves as the scattering target and a resolved transition between circuit eigenstates constitutes the observable final state. The scattering amplitude factorizes into the incident-particle current and a finite-momentum electromagnetic transition response of the qubit. This momentum dependence is essential in that the energy transfer is fixed by the microwave-scale level spacing, whereas a nonrelativistic incident particle can transfer a spatial momentum parametrically larger than that energy and thereby resolve the device geometry. For charge-dominated processes, we recast the response as an induced-offset-charge kernel obtained from an auxiliary electrostatic weighting potential, providing a practical route from circuit geometry to a differential scattering cross section. We illustrate the framework with an Xmon-style transmon and photon-mediated scattering of dark matter. The exceptionally small qubit transition threshold opens sensitivity to an eV-to-keV mass regime that is largely unexplored by existing direct-detection experiments.

Abstract:We introduce a novel approach to particle detection in which a superconducting qubit itself serves as the scattering target and a resolved transition between circuit eigenstates constitutes the observable final state. The scattering amplitude factorizes into the incident-particle current and a finite-momentum electromagnetic transition response of the qubit. This momentum dependence is essential in that the energy transfer is fixed by the microwave-scale level spacing, whereas a nonrelativistic incident particle can transfer a spatial momentum parametrically larger than that energy and thereby resolve the device geometry. For charge-dominated processes, we recast the response as an induced-offset-charge kernel obtained from an auxiliary electrostatic weighting potential, providing a practical route from circuit geometry to a differential scattering cross section. We illustrate the framework with an Xmon-style transmon and photon-mediated scattering of dark matter. The exceptionally small qubit transition threshold opens sensitivity to an eV-to-keV mass regime that is largely unexplored by existing direct-detection experiments.

arXiv:2611.05469 [hep-ph]

(or arXiv:2611.05469v1 [hep-ph] for this version)

https://doi.org/10.48550/arXiv.2611.05469 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 243 words

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