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arXiv:2505.21481

Probing the quantum motion of a macroscopic mechanical oscillator with a radio-frequency superconducting qubit

Kyrylo Gerashchenko, Rousseau, Rémi, Léo Balembois, Himanshu Patange, Paul Manset, Tristan Briant, P.-F. Cohadon, A. Heidmann, W. Clarke Smith, Antoine Tilloy, Zaki Leghtas, Emmanuel Flurin, T. Jacqmin, S. Deléglise

Published May 27, 2025• 0 citations
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Abstract

Long-lived mechanical resonators like drums oscillating at MHz frequencies and operating in the quantum regime are a powerful platform for quantum technologies and tests of fundamental physics. Yet, quantum control of such systems remains challenging, owing to their low energy scale and the difficulty of achieving efficient coupling to other well-controlled quantum devices. Here, we demonstrate repeated coherent interactions between a 4 MHz suspended silicon nitride membrane and a resonant superconducting heavy-fluxonium qubit. The qubit is initialized at an effective temperature of $21~\mathrm{μK}$ and read out with 77% single-shot fidelity. During the $6~\mathrm{ms}$ lifetime of the membrane the two systems swap excitations more than 300 times. After each interaction, a state-selective qubit detection is performed, implementing a stroboscopic series of weak measurements that provide information about the mechanical state. The accumulated records reconstruct the position noise spectrum of the membrane, revealing both its thermal occupation $n_\mathrm{th}\approx47$ at $10~\mathrm{mK}$ and the qubit-induced back-action. By preparing the qubit either in its ground or excited state before each interaction, we observe an imbalance between the emission and absorption spectra, proportional to $n_\mathrm{th}$ and $n_\mathrm{th}+1$, respectively-a hallmark of the non-commutation of phonon creation and annihilation operators. Since the predicted Diósi-Penrose gravitational collapse time is comparable to the measured mechanical decoherence time, our architecture enters a regime where gravity-induced decoherence could be tested directly.

DOI
10.48550/arxiv.2505.21481

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arXiv:2406.07360•Jun 11, 2024•0 citations
Long-lived mechanical resonators like drums oscillating at MHz frequencies and operating in the quantum regime are a powerful platform for quantum technologies and tests of fundamental physics. Yet, quantum control of such systems remains challenging, owing to their low energy scale and the difficulty of achieving efficient coupling to other well-controlled quantum devices. Here, we demonstrate repeated coherent interactions between a 4 MHz suspended silicon nitride membrane and a resonant superconducting heavy-fluxonium qubit. The qubit is initialized at an effective temperature of 21 μK21~\mathrm{μK}21 μK and read out with 77% single-shot fidelity. During the 6 ms6~\mathrm{ms}6 ms lifetime of the membrane the two systems swap excitations more than 300 times. After each interaction, a state-selective qubit detection is performed, implementing a stroboscopic series of weak measurements that provide information about the mechanical state. The accumulated records reconstruct the position noise spectrum of the membrane, revealing both its thermal occupation nth≈47n_\mathrm{th}\approx47nth​≈47 at 10 mK10~\mathrm{mK}10 mK and the qubit-induced back-action. By preparing the qubit either in its ground or excited state before each interaction, we observe an imbalance between the emission and absorption spectra, proportional to nthn_\mathrm{th}nth​ and nth+1n_\mathrm{th}+1nth​+1, respectively-a hallmark of the non-commutation of phonon creation and annihilation operators. Since the predicted Diósi-Penrose gravitational collapse time is comparable to the measured mechanical decoherence time, our architecture enters a regime where gravity-induced decoherence could be tested directly.
Dans cette thèse, il a été montré qu'une membrane suspendue en nitrure de silicium à 4 MHz peut être répétitivement et de façon cohérente interfacée avec un qubit heavy-fluxonium résonnant. Le qubit a été initialisé à une température effective de 21 microkelvin et détecté avec une fidélité monocoup de 77 %. Sur la durée de vie ~6 ms de la membrane, plus de 300 échanges d'excitation ont été réalisés. Au moyen de mesures faibles stroboscopiques sélectives en état après chaque interaction, le spectre de bruit de position de la membrane a été reconstruit, révélant une occupation thermique de n_th~47 quanta à 10 millikelvin et une rétroaction de mesure induite par le qubit. En préparant le qubit dans l'état fondamental ou excité, une asymétrie émission-absorption proportionnelle à n_th et n_th+1 a été observée, mettant en évidence la non-commutation des opérateurs d'échelle phononiques. Le temps de décohérence mécanique mesuré est comparable au temps d'effondrement estimé de Diósi-Penrose, plaçant cette architecture dans un régime pertinent pour des tests directs de la décohérence liée à la gravité dans la suite de ce projet.
Étude du mouvement quantique d'un oscillateur mécanique macroscopique à l'aide d'un qubit supraconducteur à radiofréquence Dans cette thèse, il a été montré qu'une membrane suspendue en nitrure de silicium à 4 MHz peut être répétitivement et de façon cohérente interfacée avec un qubit heavy-fluxonium résonnant. Le qubit a été initialisé à une température effective de 21 microkelvin et détecté avec une fidélité monocoup de 77 %. Sur la durée de vie ~6 ms de la membrane, plus de 300 échanges d'excitation ont été réalisés. Au moyen de mesures faibles stroboscopiques sélectives en état après chaque interaction, le spectre de bruit de position de la membrane a été reconstruit, révélant une occupation thermique de n_th~47 quanta à 10 millikelvin et une rétroaction de mesure induite par le qubit. En préparant le qubit dans l'état fondamental ou excité, une asymétrie émission-absorption proportionnelle à n_th et n_th+1 a été observée, mettant en évidence la non-commutation des opérateurs d'échelle phononiques. Le temps de décohérence mécanique mesuré est comparable au temps d'effondrement estimé de Diósi-Penrose, plaçant cette architecture dans un régime pertinent pour des tests directs de la décohérence liée à la gravité dans la suite de ce projet.
We present experiments aimed at the creation and study of non-Gaussian states of a mesoscopic mechanical oscillator. On the mechanical front, we have developped, fabricated and operated phononic-crystal SiN membranes, with mechanical quality factors in the 10^8 to 10^9 range. To allow resonant coupling of the membrane (typically in the MHz band) to a two-level system, we have developped a heavy fluxonium superconducting qubit architecture, with a transition frequeny as low as 1.8 MHz.. Design, fabrication and operation of the qubit in a 10 mK environment are discussed, together with a charge sensing experiment The long-term goal of these experiments is to create and explore non-Gaussian states of an electromechanical membrane.
Abstract Massive mechanical resonators operating at the quantum scale can enable a large variety of applications in quantum technologies as well as fundamental tests of quantum theory. Of crucial importance in that direction is both their integrability into state-of-the-art quantum platforms as well as the ability to prepare them in generic quantum states using well-controlled high-fidelity operations. Here, we propose a scheme for controlling a radio-frequency mechanical resonator at the quantum scale using two superconducting transmon qubits that can be integrated on the same chip. Specifically, we consider two qubits coupled via a capacitor in parallel to a superconducting quantum interference device (SQUID), which has a suspended mechanical beam embedded in one of its arms. Following a theoretical analysis of the quantum system, we find that this configuration, in combination with an in-plane magnetic field, can give rise to a tuneable three-body interaction in the single-photon strong-coupling regime, while enabling suppression of the stray qubit-qubit coupling. Using state-of-the-art parameters and qubit operations at single-excitation levels, we numerically demonstrate the possibility of ground-state cooling as well as high-fidelity preparation of mechanical quantum states and qubit-phonon entanglement, i.e. states having negative Wigner functions and obeying non-classical correlations. Our work significantly extends the quantum control toolbox of radio-frequency mechanical resonators and may serve as a promising architecture for integrating such mechanical elements with transmon-based quantum processors.
Superconducting fluxonium qubits show a highly tunable energy-level structure, with transition frequencies spanning from a few MHz to few GHz. This range is well-aligned to the operational frequencies of highly coherent micro- and nano-mechanical resonators, making fluxonium an attractive candidate for hybrid electromechanical systems. In this work, we theoretically investigate a flux-tunable electromechanical system consisting of a fluxonium qubit coupled to a suspended mechanical resonator. The coupling arises from the motion-induced modulation of magnetic flux through the fluxonium loop, enabling both transverse and longitudinal electromechanical interactions that are tunable via external magnetic fields. By optimizing the design parameters of the fluxonium qubit, we demonstrate the feasibility of achieving strong resonant single-photon coupling near the flux-frustration point. We analyze the system dynamics across different coupling regimes, identifying signatures of electromagnetically induced transparency (EIT) in the longitudinal regime and mode splitting in the transverse regime. Additionally, we show that ground-state preparation of both subsystems is possible through sideband cooling of the mechanical resonator. These results suggest that a fluxonium-based hybrid electromechanical device could be a promising platform for studying macroscopic quantum phenomena and for applications in quantum technology.
Strong nonlinear interactions between quantized excitations are an important resource for quantum technologies based on bosonic oscillator modes. However, most electromagnetic and mechanical nonlinearities arising from intrinsic material properties are far too weak compared to dissipation in the system to allow for nonlinear effects to be observed on the single-quantum level. To overcome this limitation, electromagnetic resonators in both the optical and microwave frequency regimes have been coupled to other strongly nonlinear quantum systems such as atoms and superconducting qubits, allowing for the demonstration of effects such as photon blockade and coherent quantum protocols using the Kerr effect. Here, we demonstrate the realization of the single-phonon nonlinear regime in a solid-state mechanical system. The single-phonon anharmonicity in our system exceeds the decoherence rate by a factor of 6.8, allowing us to use the lowest two energy levels of the resonator as a mechanical qubit, for which we show initialization, readout, and a complete set of direct single qubit gates. Our work adds another unique capability to a powerful quantum acoustics platform for quantum simulations, sensing, and information processing.