Intrinsic phononic dressed states in a nanomechanical system

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Nature Physics (2026)Cite this article Nanoelectromechanical systems provide a platform for probing the quantum nature of mechanical motion in mesoscopic systems. Quantum effects are most pronounced when device vibrations are nonlinear, but it has been difficult to achieve vibrational nonlinearity at the single-phonon level. Here we report the observation of intrinsic mesoscopic vibrational states that are dressed by the interactions with a nonlinear quantum system. The nonlinearity results from the strong resonant coupling between an eigenmode of a nanoelectromechanical system resonator and a single, two-level system that is intrinsic to the device material. We control the two-level system in situ by varying the mechanical strain in the device, tuning it in and out of resonance with the nanoelectromechanical system mode. Varying the resonant drive or temperature allows a controlled ascent of the non-equidistant energy ladder of the hybridized system. Fluctuations of the two-level system on and off resonance with the mode induce switching between the dressed and bare states. These quantum effects directly emerge from the intrinsic material properties of mechanical systems without the need for complex, external quantum circuits. Our work offers insight into mesoscopic dynamics and provides the opportunity to harness nanomechanics for quantum measurements.This is a preview of subscription content, access via your institution Access Nature and 54 other Nature Portfolio journals Get Nature+, our best-value online-access subscription $32.99 / 30 days cancel any timeSubscribe to this journal Receive 12 print issues and online access $259.00 per yearonly $21.58 per issueBuy this articleUSD 39.95Prices may be subject to local taxes which are calculated during checkoutSource data are provided with this paper. The data used to generate the figures in the main text are provided in the paper and are also available via Zenodo at https://doi.org/10.5281/zenodo.15299527 (ref. 65). All other data generated or analysed during this study are available from the corresponding authors upon reasonable request.Bachtold, A., Moser, J. & Dykman, M. Mesoscopic physics of nanomechanical systems. Rev. Mod. Phys. 94, 045005 (2022).Article ADS MathSciNet Google Scholar Ekinci, K. L. & Roukes, M. L. Nanoelectromechanical systems. Rev. Sci. Instrum. 76, 061101 (2005).Schwab, K. C. & Roukes, M. L. Putting mechanics into quantum mechanics. Phys. Today 58, 36–42 (2005).Article Google Scholar MacCabe, G. S. et al. Nano-acoustic resonator with ultralong phonon lifetime. Science 370, 840–843 (2020).Article ADS Google Scholar Arrangoiz-Arriola, P. et al. Resolving the energy levels of a nanomechanical oscillator. Nature 571, 537–540 (2019).Article ADS Google Scholar Bozkurt, A. et al. A quantum electromechanical interface for long-lived phonons. Nat. Phys. 19, 1326–1332 (2023).Article Google Scholar Pistolesi, F., Cleland, A. & Bachtold, A. Proposal for a nanomechanical qubit. Phys. Rev. X 11, 031027 (2021).
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(A.H.S.-N.); and US Department of Energy, grant number DE-AC02-76SF00515 (A.H.S.-N.). M.P.M. is grateful for support from an NSERC graduate fellowship. We thank the Stanford Nanofabrication Facility (supported by National Science Foundation awards ECCS-2026822 and ECCS-1542152), Caltech’s Kavli Nanoscience Institute and Stanford’s Q-NEXT Center. We also acknowledge valuable discussions with W. Fon, S. Habermehl, U. Hatipoglu and A. Nunn, and fabrication assistance from W. Jiang, K. K. S. Multani and A. Y. Cleland.These authors contributed equally: M. Yuksel, M. P. Maksymowych.Department of Applied Physics, California Institute of Technology, Pasadena, CA, USAM. Yuksel & M. L. RoukesDepartment of Applied Physics and Ginzton Laboratory, Stanford University, Stanford, CA, USAM. P. Maksymowych, O. A. Hitchcock, F. M. Mayor, N. R. Lee & A. H. Safavi-NaeiniDepartment of Physics, Stanford University, Stanford, CA, USAO. A. HitchcockDepartment of Physics and Astronomy, Michigan State University, East Lansing, MI, USAM. I. DykmanDepartment of Physics and the Kavli Nanoscience Institute, California Institute of Technology, Pasadena, CA, USAM. L. RoukesDepartment of Bioengineering, California Institute of Technology, Pasadena, CA, USAM. L. RoukesSearch author on:PubMed Google ScholarSearch author on:PubMed Google ScholarSearch author on:PubMed Google ScholarSearch author on:PubMed Google ScholarSearch author on:PubMed Google ScholarSearch author on:PubMed Google ScholarSearch author on:PubMed Google ScholarSearch author on:PubMed Google ScholarM.Y. performed the experiments at Caltech, analysed the data and conducted the simulations. M.P.M. performed the experiments at Stanford and analysed the data. M.Y. and M.P.M. developed the theoretical framework with assistance from M.I.D., A.H.S.-N. and M.L.R. M.P.M., O.A.H., F.M.M. and N.R.L. designed and fabricated the devices at Stanford. M.Y., M.P.M. and M.I.D. wrote the paper with input from all authors. M.I.D., A.H.S.-N. and M.L.R. supervised the project.Correspondence to M. Yuksel or M. L. Roukes.A.H.S.-N. is an Amazon Scholar. The other authors declare no competing interests.Nature Physics thanks the anonymous reviewers for their contribution to the peer review of this work. Peer reviewer reports are available.Publisher’s note Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.Schematic of the horizontal dilution refrigerator measurement setup at Caltech used to acquire the data presented in the main text.The plot displays the mean squared error (MSE) as a function of the estimated phonon number n. After iterative minimization of the fitting parameters, we sweep n around the optimized neff value to quantify the uncertainty in our estimation. This sweep identifies the regions n neff where the MSE increases by 5% above its minimum value (indicated by the shaded area). Notably, the error rises more steeply for n neff as expected due to the \(\sqrt{n}\) scaling of the energy levels. As neff increases further, achieving an accurate determination becomes increasingly challenging and computationally expensive.Source dataSupplementary Figs. 1–9, Table 1, Sections 1–4, Discussion and Data.Evolution of the TLS,C1 crossing as the input power is increased from –150 dBm to –135 dBm in 1-dB increments.Source data comprising raw experimental and simulation data.Source data comprising raw experimental and simulation data.Source data comprising raw experimental and simulation data.Source data comprising raw experimental and simulation data.Source data comprising raw experimental and simulation data.Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.Reprints and permissionsYuksel, M., Maksymowych, M.P., Hitchcock, O.A. et al. Intrinsic phononic dressed states in a nanomechanical system. Nat. Phys. (2026). https://doi.org/10.1038/s41567-026-03225-3Download citationReceived: 04 September 2025Accepted: 23 February 2026Published: 14 April 2026Version of record: 14 April 2026DOI: https://doi.org/10.1038/s41567-026-03225-3Anyone you share the following link with will be able to read this content:Sorry, a shareable link is not currently available for this article. Provided by the Springer Nature SharedIt content-sharing initiative
