aiqbench analysis
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.
Superconducting Qubits as Quantum Targets for Direct Particle Scattering
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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