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This paper shows that a transmon qubit can be read out through a millimeter-wave cavity, with the cavity frequency more than ten times the qubit frequency. The large detuning suppresses unwanted state transitions, so the qubit tolerates very strong readout drives and still reaches over 99% measurement fidelity without a quantum-limited amplifier. For quantum hardware readers, the result is a proof of concept for mm-wave interfaces to superconducting qubits, though it is a single-qubit, lab-scale demonstration whose scalability remains untested.
Millimeter Wave Readout of a Superconducting Qubit
arXiv:2603.13837v2 Announce Type: replace Abstract: Millimeter waves are emerging as an enabling technology for connecting and enhancing different quantum platforms such as Rydberg atoms, optomechanics, and superconducting qubits. In this work, we explore the interaction between millimeter wave photons and conventional transmon qubits, specifically for qubit readout. We study a circuit quantum electrodynamic (cQED) system consisting of a millimeter wave cavity at $\omega_r = 2\pi \times 34.7$ GHz and a transmon qubit at $\omega_q = 2\pi \times 3.1$ GHz coupled at rate $g = 2\pi \times 1.3$. With such a large detuning between cavity and qubit, $\omega_r/\omega_q > 10$, we are able to suppress drive induced unwanted resonant state transitions, enabling strong drives for qubit readout. We measure no resonant state transitions even when driving with more than $100$ photons and read out the qubit state with more than $100$ photons to achieve a measurement fidelity greater than $99\%$ without the aid of a quantum limited amplifier.
Abstract:Millimeter waves are emerging as an enabling technology for connecting and enhancing different quantum platforms such as Rydberg atoms, optomechanics, and superconducting qubits. In this work, we explore the interaction between millimeter wave photons and conventional transmon qubits, specifically for qubit readout. We study a circuit quantum electrodynamic (cQED) system consisting of a millimeter wave cavity at $\omega_r = 2\pi \times 34.7$ GHz and a transmon qubit at $\omega_q = 2\pi \times 3.1$ GHz coupled at rate $g = 2\pi \times 1.3$. With such a large detuning between cavity and qubit, $\omega_r/\omega_q > 10$, we are able to suppress drive induced unwanted resonant state transitions, enabling strong drives for qubit readout. We measure no resonant state transitions even when driving with more than $100$ photons and read out the qubit state with more than $100$ photons to achieve a measurement fidelity greater than $99\%$ without the aid of a quantum limited amplifier.
5 pages, 4 figures in main text. 10 pages, 11 figures, 1 table in supplemental materials
arXiv:2603.13837 [quant-ph]
(or arXiv:2603.13837v2 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2603.13837 Focus to learn more arXiv-issued DOI via DataCite
Phys. Rev. Lett. 137, 180803 (2026)
https://doi.org/10.1103/c84y-ggqs Focus to learn more DOI(s) linking to related resources
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