Photoluminescence of a microcavity quantum dot system in the quantum strong-coupling regime
arXiv:1301.4306 · doi:10.1038/srep01180
Abstract
The Jaynes-Cummings model, describing the interaction between a single two-level system and a photonic mode, has been used to describe a large variety of systems, ranging from cavity quantum electrodynamics, trapped ions, to superconducting qubits coupled to resonators. Recently there has been renewed interest in studying the quantum strong-coupling (QSC) regime, where states with photon number greater than one are excited. This regime has been recently achieved in semiconductor nanostructures, where a quantum dot is trapped in a planar microcavity. Here we study the quantum strong-coupling regime by calculating its photoluminescence (PL) properties under a pulsed excitation. We discuss the changes in the PL as the QSC regime is reached, which transitions between a peak around the cavity resonance to a doublet. We particularly examine the variations of the PL in the time domain, under regimes of short and long pulse times relative to the microcavity decay time.
arXiv comment22 pages, 7 figures
References in corpus (7)
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- Temperature dependence of the single photon source efficiency based on QD-cQED
- Time-resolved physical spectrum in cavity quantum electrodynamics
- Photon statistics of radiation emitted by two quantum wells embedded in two optically coupled semiconductor microcavities
- Thermal coherence of the Heisenberg model with Dzyaloshinsky-Moriya interactions in an inhomogenous external field
- Cooper pair polaritons in cold fermionic atoms within a cavity