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A squeezed mechanical oscillator with millisecond quantum decoherence

Abstract

An enduring challenge in constructing mechanical-oscillator-based hybrid quantum systems is to ensure engineered coupling to an auxiliary degree of freedom and maintain good mechanical isolation from the environment, that is, low quantum decoherence, consisting of thermal decoherence and dephasing. Here we overcome this challenge by introducing a superconducting-circuit-based optomechanical platform that exhibits low quantum decoherence and has a large optomechanical coupling, which allows us to prepare the quantum ground and squeezed states of motion with high fidelity. We directly measure a thermal decoherence rate of 20.5 Hz (corresponding to T1 = 7.7 ms) as well as a pure dephasing rate of 0.09 Hz, yielding a 100-fold improvement in the quantum state lifetime compared with prior optomechanical systems. This enables us to reach a motional ground-state occupation of 0.07 quanta (93% fidelity) and realize mechanical squeezing of –2.7 dB below the zero-point fluctuation. Furthermore, we observe the free evolution of the mechanical squeezed state, preserving its non-classical nature over millisecond timescales. Such ultralow quantum decoherence not only increases the fidelity of quantum control and measurement of macroscopic mechanical systems but may also benefit interfacing with qubits, and places the system in a parameter regime suitable for tests of quantum gravity.

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Fig. 1: Ultracoherent circuit optomechanics.
Fig. 2: High-fidelity optomechanical ground-state cooling.
Fig. 3: Recording the motional heating rate out of the quantum ground state.
Fig. 4: Tracking the free evolution of a mechanical squeezed state.

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Data availability

The data used to produce the plots within this paper are available via Zenodo at https://doi.org/10.5281/zenodo.7833893. All other data used in this study are available from the corresponding authors on reasonable request. Source data are provided with this paper.

Code availability

The code used to produce the plots within this paper is available via Zenodo at https://doi.org/10.5281/zenodo.7833893.

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Acknowledgements

We thank MIT Lincoln Laboratory and W. D. Oliver for providing the Josephson travelling-wave parametric amplifier. We thank A. Arabmoheghi for helpful discussions on the theory of mechanical dissipation. This work was supported by the EU H2020 research and innovation programme under grant no. 101033361 (QuPhon), and from the European Research Council (ERC) grant no. 835329 (ExCOM-cCEO). This work was also supported by the Swiss National Science Foundation (SNSF) under grant no. NCCR-QSIT:51NF40_185902 and no. 204927. All the devices were fabricated in the Center of MicroNanoTechnology (CMi) at EPFL.

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Authors and Affiliations

Authors

Contributions

A.Y. conceived the experiment. S.K., M.C. and A.Y. developed the theory. A.Y. designed and simulated the devices. A.Y. developed the fabrication process with assistance from M.C. M.C. and A.Y. fabricated the samples. A.Y. and M.C. developed the experimental setup. The measurement was performed by A.Y. and M.C., with assistance from S.K. The data analysis was performed by A.Y. with assistance from S.K. S.K. introduced the phonon number calibration based on sideband asymmetry and conducted the numerical simulation for extracting the mechanical dephasing. The manuscript was written by A.Y., S.K., M.C. and T.J.K. T.J.K. supervised the project.

Corresponding author

Correspondence to Tobias J. Kippenberg.

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Extended data

Extended Data Fig. 1 Overview on the fabrication technique for highly coherent circuit optomechanics.

The main steps of the process consists of etching a trench in the substrate followed by deposition of a sacrificial layer, planarization, top layer definition, release, and finally cool down. Due to the compressive stresses, the top plate may buckle up after the release. However, the drumhead shrinks and flattens at cryogenic temperatures, resulting in a controllable gap size.

Extended Data Fig. 2 Free evolution of a mechanical squeezed state.

a, Quadrature variances and average phonon number of a squeezed state as a function of the free-evolution time. The blue, red and purple circles are the data for the quadrature variances in the squeezed and anti-squeezed axes, and the average phonon number, respectively. The black dotted lines are linear fits, while the green lines are the numerical simulation results. Error bars are corresponding to standard deviations. b, The difference of the thermal decoherence rates for the quadrature variances in the squeezed and anti-squeezed axes as a function of the pure dephasing rate. The green line shows the numerical simulation results, while the blue line is the experimentally obtained value. The shaded regions show the errors, respectively.

Source data

Supplementary information

Supplementary Information

Supplementary Figs. 1–20, Tables 1 and 2 and References.

Source data

Source Data Fig. 1

Source data for ring-down and frequency fluctuation.

Source Data Fig. 2

Source data for sideband asymmetry.

Source Data Fig. 3

Source data for optomechanical amplification.

Source Data Fig. 4

Source data for squeezing.

Source Data Extended Data Fig. 2

Source data for dephasing rate extraction.

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Youssefi, A., Kono, S., Chegnizadeh, M. et al. A squeezed mechanical oscillator with millisecond quantum decoherence. Nat. Phys. 19, 1697–1702 (2023). https://doi.org/10.1038/s41567-023-02135-y

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