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Research Article

Polariton lasing vs. photon lasing in a semiconductor microcavity

Hui Deng, Gregor Weihs, David Snoke, Jacqueline Bloch, and Yoshihisa Yamamoto
  1. *Quantum Entanglement Project, International Cooperative Research Project (ICORP), Japan Science and Technology Corporation, Edward L. Ginzton Laboratory, Stanford University, Stanford, CA 94305; ‡Institute of Industrial Science, Tokyo University, 4-6-1 Komaba, Meguro-ku, Tokyo 153-8904, Japan; §Department of Physics and Astronomy, University of Pittsburgh, 3841 O'Hara Street, Pittsburgh, PA 15260; ¶Laboratory of Photonic and Nanostructures, Centre National de la Recherché Scientifique, Route de Nozay, 91460 Marcoussis, France; and **NTT Basic Research Laboratories, Morinosato Wakamiya, Astugishi, 243-0198 Kanagawa, Japan

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PNAS December 23, 2003 100 (26) 15318-15323; https://doi.org/10.1073/pnas.2634328100
Hui Deng
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Gregor Weihs
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David Snoke
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Jacqueline Bloch
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Yoshihisa Yamamoto
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  1. Edited by Paul C. Martin, Harvard University, Cambridge, MA, and approved October 29, 2003 (received for review July 10, 2003)

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Abstract

Nearly one decade after the first observation of Bose–Einstein condensation in atom vapors and realization of matter-wave (atom) lasers, similar concepts have been demonstrated recently for polaritons: half-matter, half-light quasiparticles in semiconductor microcavities. The half-light nature of polaritons makes polariton lasers promising as a new source of coherent and nonclassical light with extremely low threshold energy. The half-matter nature makes polariton lasers a unique test bed for many-body theories and cavity quantum electrodynamics. In this article, we present a series of experimental studies of a polariton laser, exploring its properties as a relatively dense degenerate Bose gas and comparing it to a photon laser achieved in the same structure. The polaritons have an effective mass that is twice the cavity photon effective mass, yet seven orders of magnitude less than the hydrogen atom mass; hence, they can potentially condense at temperatures seven orders of magnitude higher than those required for atom Bose–Einstein condensations. Accompanying the phase transition, a polariton laser emits coherent light but at a threshold carrier density two orders of magnitude lower than that needed for a normal photon laser in a same structure. It also is shown that, beyond threshold, the polariton population splits to a thermal equilibrium Bose–Einstein distribution at in-plane wave number k∥ > 0 and a nonequilibrium condensate at k∥ > 0, with a chemical potential approaching to zero. The spatial distributions and polarization characteristics of polaritons also are discussed as unique signatures of a polariton laser.

Footnotes

    • ↵† To whom correspondence should be addressed at: Stanford University, 316 Via Paulo Street, Stanford, CA 94305. E-mail: dhui{at}stanford.edu.

    • This paper was submitted directly (Track II) to the PNAS office.

    • Abbreviations: BE, Bose–Einstein; BEC, BE condensation; GaAs, gallium arsenide; QW, quantum well; LP, lower polariton; UP, upper polariton.

    • Received July 10, 2003.
    • Copyright © 2003, The National Academy of Sciences
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    Polariton lasing vs. photon lasing in a semiconductor microcavity
    Hui Deng, Gregor Weihs, David Snoke, Jacqueline Bloch, Yoshihisa Yamamoto
    Proceedings of the National Academy of Sciences Dec 2003, 100 (26) 15318-15323; DOI: 10.1073/pnas.2634328100

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    Polariton lasing vs. photon lasing in a semiconductor microcavity
    Hui Deng, Gregor Weihs, David Snoke, Jacqueline Bloch, Yoshihisa Yamamoto
    Proceedings of the National Academy of Sciences Dec 2003, 100 (26) 15318-15323; DOI: 10.1073/pnas.2634328100
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    Proceedings of the National Academy of Sciences: 100 (26)
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    • Article
      • Abstract
      • Dynamic Condensation of Polaritons
      • Experimental Principles
      • Threshold Carrier Densities
      • Dispersion Characteristics
      • Momentum Space Distribution
      • Relaxation Time vs. Polariton Lifetime
      • Real Space Distribution
      • Polarization Characteristics
      • Summary
      • Footnotes
      • References
    • Figures & SI
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