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Cavity QED with a Bose–Einstein condensate

Nature volume 450, pages 268271 (08 November 2007) | Download Citation

Abstract

Cavity quantum electrodynamics (cavity QED) describes the coherent interaction between matter and an electromagnetic field confined within a resonator structure, and is providing a useful platform for developing concepts in quantum information processing1. By using high-quality resonators, a strong coupling regime can be reached experimentally in which atoms coherently exchange a photon with a single light-field mode many times before dissipation sets in. This has led to fundamental studies with both microwave2,3 and optical resonators4. To meet the challenges posed by quantum state engineering5 and quantum information processing, recent experiments have focused on laser cooling and trapping of atoms inside an optical cavity6,7,8. However, the tremendous degree of control over atomic gases achieved with Bose–Einstein condensation9 has so far not been used for cavity QED. Here we achieve the strong coupling of a Bose–Einstein condensate to the quantized field of an ultrahigh-finesse optical cavity and present a measurement of its eigenenergy spectrum. This is a conceptually new regime of cavity QED, in which all atoms occupy a single mode of a matter-wave field and couple identically to the light field, sharing a single excitation. This opens possibilities ranging from quantum communication10,11,12 to a wealth of new phenomena that can be expected in the many-body physics of quantum gases with cavity-mediated interactions13,14.

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Acknowledgements

We thank A. Öttl for early contributions to the experiment, R. Jördens and A. Frank for developing the direct digital synthesis generators used for the optical transport, H. Ritsch and A. Imamoglu for discussions and OLAQUI and QSIT for funding. T.B. acknowledges funding by an EU Marie Curie fellowship.

Author information

Affiliations

  1. Institute for Quantum Electronics, ETH Zürich, 8093 Zürich, Switzerland

    • Ferdinand Brennecke
    • , Tobias Donner
    • , Stephan Ritter
    •  & Tilman Esslinger
  2. Laboratoire Charles Fabry, Institut d'Optique, Campus Polytechnique, RD 128, F91127 Palaiseau cedex, France

    • Thomas Bourdel
  3. Cavendish Laboratory, University of Cambridge, Cambridge CB3 0HE, UK

    • Michael Köhl

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Competing interests

The authors declare no competing financial interests.

Corresponding author

Correspondence to Tilman Esslinger.

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DOI

https://doi.org/10.1038/nature06120

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