Strong light-matter coupling in the presence of lasing
arXiv:1606.05591 · doi:10.1103/PhysRevA.96.023806
Abstract
The regime of strong light-matter coupling is typically associated with weak excitation. With current realizations of cavity-QED systems, strong coupling may persevere even at elevated excitation levels sufficient to cross the threshold to lasing. In the presence of stimulated emission, the vacuum-Rabi doublet in the emission spectrum is modified and the established criterion for strong coupling no longer applies. We provide a generalized criterion for strong coupling and the corresponding emission spectrum, which includes the influence of higher Jaynes-Cummings states. The applicability is demonstrated in a theory-experiment comparison of a few-emitter quantum-dot--micropillar laser as a particular realization of the driven dissipative Jaynes-Cummings model. Furthermore, we address the question if and for which parameters true single-emitter lasing can be achieved, and provide evidence for the coexistence of strong coupling and lasing in our system in the presence of background emitter contributions.
arXiv comment12 pages, 9 figures
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- Revisiting the Siegert relation for the partially coherent regime of nanolasers
- Single site-controlled inverted pyramidal InGaAs QD-nanocavity operating at the onset of the strong coupling regime
- Controlling the gain contribution of background emitters in few-quantum-dot microlasers
- Simple yet Accurate Stochastic Approach to the Quantum Phase Noise of Nanolasers