2005
DOI: 10.1103/physrevlett.95.067401
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Exciton-Photon Strong-Coupling Regime for a Single Quantum Dot Embedded in a Microcavity

Abstract: We report on the observation of the strong-coupling regime between the excitonic transition of a single GaAs quantum dot and a discrete optical mode of a microdisk microcavity. Photoluminescence is performed at various temperatures to tune the quantum dot exciton with respect to the optical mode. At resonance, we observe a clear anticrossing behavior, signature of the strong-coupling regime. The vacuum Rabi splitting amounts to 400 microeV and is twice as large as the individual linewidths.

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Cited by 755 publications
(578 citation statements)
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“…A FDTD simulation of this mode predicts Q=81,000. Such a high Q-value would push a coupled dot-cavity system into the strong coupling regime [22,[93][94][95], where spontaneous emission is a reversible process such that the emitted photon could be reabsorbed by the dot before escaping the cavity. The system thus undergoes Rabi oscillations, allowing for the coherent transfer of quantum information between the photon and quantum dot.…”
Section: Microcavitiesmentioning
confidence: 99%
“…A FDTD simulation of this mode predicts Q=81,000. Such a high Q-value would push a coupled dot-cavity system into the strong coupling regime [22,[93][94][95], where spontaneous emission is a reversible process such that the emitted photon could be reabsorbed by the dot before escaping the cavity. The system thus undergoes Rabi oscillations, allowing for the coherent transfer of quantum information between the photon and quantum dot.…”
Section: Microcavitiesmentioning
confidence: 99%
“…In the case of emission lines, this effect has already been investigated experimentally in symmetric QDs, where by analyzing the exciton line shape at different temperatures a strong deviation from the expected Lorentzian profile has been observed expressed in the appearance of low-energy acoustic-phonon sidebands [31][32][33][34]. In general, it is expected that an exciton confined in a larger quantum object should exhibit a weaker interaction with phonons [31,32,34,35]. This is due to the wave vector cutoff, approximately at the inverse of the structure size.…”
Section: Introductionmentioning
confidence: 99%
“…In systems with integrated quantum emitters, predominantly the parameters of the cavity determine the interaction regime: In the weak light-matter coupling regime, the radiative lifetime of the emitter is altered by the presence of the cavity via Fermi's golden rule [6]. In contrast, if the light-matter interaction strength exceeds the cavity loss channels, the coherent regime of strong coupling is reached [7][8][9]. Both regimes have fundamental importance in the design of semiconductor devices with integrated quantum emitters (quantum dots) of the 'next generation' of photonic devices, such as efficient sources of single photons on demand [10][11][12], sources of entangled photon pairs [13], and sources of coherently generated and emitted single photons as demonstrated for atoms in optical cavities [14] .…”
Section: Introductionmentioning
confidence: 99%