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Emergence of a turbulent cascade in a quantum gas
Naturevolume 539, pages72–75 (2016)Cite this article
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Abstract
A central concept in the modern understanding of turbulence is the existence of cascades of excitations from large to small length scales, or vice versa. This concept was introduced in 1941 by Kolmogorov and Obukhov1,2, and such cascades have since been observed in various systems, including interplanetary plasmas3, supernovae4, ocean waves5 and financial markets6. Despite much progress, a quantitative understanding of turbulence remains a challenge, owing to the interplay between many length scales that makes theoretical simulations of realistic experimental conditions difficult. Here we observe the emergence of a turbulent cascade in a weakly interacting homogeneous Bose gas—a quantum fluid that can be theoretically described on all relevant length scales. We prepare a Bose–Einstein condensate in an optical box7, drive it out of equilibrium with an oscillating force that pumps energy into the system at the largest length scale, study its nonlinear response to the periodic drive, and observe a gradual development of a cascade characterized by an isotropic power-law distribution in momentum space. We numerically model our experiments using the Gross–Pitaevskii equation and find excellent agreement with the measurements. Our experiments establish the uniform Bose gas as a promising new medium for investigating many aspects of turbulence, including the interplay between vortex and wave turbulence, and the relative importance of quantum and classical effects.
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Acknowledgements
We thank G. V. Shlyapnikov, B. Svistunov, S. Stringari, N. R. Cooper, J. Dalibard, M. J. Davis, R. J. Fletcher, M. W. Zwierlein, K. Fujimoto and M. Tsubota for discussions, and C. Eigen for experimental assistance. This work was supported by AFOSR, ARO, DARPA OLE, EPSRC (Grant No. EP/N011759/1) and ERC (QBox). The GeForce GTX TITAN X used for the numerical simulations was donated by the NVIDIA Corporation. N.N. and A.L.G. acknowledge support from Trinity College, Cambridge; R.P.S. acknowledges support from the Royal Society.
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Authors and Affiliations
Cavendish Laboratory, University of Cambridge, J. J. Thomson Avenue, Cambridge, CB3 0HE, UK
Nir Navon, Alexander L. Gaunt, Robert P. Smith & Zoran Hadzibabic
- Nir Navon
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Contributions
N.N. initiated the project, and took and analysed the data. A.L.G. wrote the code for the numerical simulations and analysed the results. Z.H. supervised the project. All authors contributed extensively to the interpretation of the data and the writing of the manuscript.
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Correspondence toNir Navon.
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Extended data figures and tables
Extended Data Figure 1 Momentum distributions from TOF and Bragg techniques.
a,b, Comparison ofn1D(kz) obtained using TOF expansion (solid lines) and Bragg spectroscopy (points), in the case of the initial, quasi-pure BEC (a) and the turbulent gas (b). The red dashed line ina corresponds to the Heisenberg-limited momentum distribution. All distributions are normalized to unity (
), without any adjustable parameters.
Extended Data Figure 2 Turbulent cascade in numerical simulations.
a, In-plane momentum distribution
for various shaking timests.b, Ratio of the compressible- (
c) to incompressible-flow (
i) components of the fluid-dynamical kinetic energy, with the colours corresponding to the shaking times ina. The simulation parameters for both panels areN = 8 × 104, shaking frequencyω/(2π) = 9 Hz and shaking amplitude ΔU = μ.
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Navon, N., Gaunt, A., Smith, R.et al. Emergence of a turbulent cascade in a quantum gas.Nature539, 72–75 (2016). https://doi.org/10.1038/nature20114
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