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Sideband cooling of micromechanical motion to the quantum ground state


The advent of laser cooling techniques revolutionized the study of many atomic-scale systems, fuelling progress towards quantum computing with trapped ions1 and generating new states of matter with Bose–Einstein condensates2. Analogous cooling techniques3,4 can provide a general and flexible method of preparing macroscopic objects in their motional ground state. Cavity optomechanical or electromechanical systems achieve sideband cooling through the strong interaction between light and motion5,6,7,8,9,10,11,12,13,14,15. However, entering the quantum regime—in which a system has less than a single quantum of motion—has been difficult because sideband cooling has not sufficiently overwhelmed the coupling of low-frequency mechanical systems to their hot environments. Here we demonstrate sideband cooling of an approximately 10-MHz micromechanical oscillator to the quantum ground state. This achievement required a large electromechanical interaction, which was obtained by embedding a micromechanical membrane into a superconducting microwave resonant circuit. To verify the cooling of the membrane motion to a phonon occupation of 0.34 ± 0.05 phonons, we perform a near-Heisenberg-limited position measurement3 within (5.1 ± 0.4)h/2π, where h is Planck’s constant. Furthermore, our device exhibits strong coupling, allowing coherent exchange of microwave photons and mechanical phonons16. Simultaneously achieving strong coupling, ground state preparation and efficient measurement sets the stage for rapid advances in the control and detection of non-classical states of motion17,18, possibly even testing quantum theory itself in the unexplored region of larger size and mass19. Because mechanical oscillators can couple to light of any frequency, they could also serve as a unique intermediary for transferring quantum information between microwave and optical domains20.

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Figure 1: Schematic description of the experiment.
Figure 2: Displacement sensitivity in the presence of dynamical back-action.
Figure 3: Sideband cooling the mechanical mode to the ground state.


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We thank A. W. Sanders for taking the micrograph in Fig. 1 and the JILA instrument shop for fabrication and design of the cavity filter. This work was supported by NIST and the DARPA QuASAR programme. T.D. acknowledges support from the Deutsche Forschungsgemeinschft (DFG). This Letter is a contribution of the US government and not subject to copyright.

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Authors and Affiliations



J.D.T. and R.W.S. conceived the device. J.D.T. designed the circuit. J.D.T. and D.L. fabricated the devices. J.D.T. and T.D. set up the experiment, performed the measurements and analysed the data. J.D.T., T.D., R.W.S. and K.W.L. discussed the results and wrote the manuscript. All authors provided experimental support and commented on the manuscript.

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Correspondence to J. D. Teufel.

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The authors declare no competing financial interests.

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Teufel, J., Donner, T., Li, D. et al. Sideband cooling of micromechanical motion to the quantum ground state. Nature 475, 359–363 (2011).

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