2009/06/03 by Mathieu Munsch, M. Munsch, A. Mosset +12 · 2 citations
Engineering · Physics and Astronomy · #Common emitter #Coupling (piping) #Laser #Materials science #Optical microcavity #Optics #Optoelectronics #Photonic Crystals and Applications #Photonic and Optical Devices #Physics #Purcell effect #Quantum #Quantum dot #Quantum mechanics #Semiconductor #Semiconductor Quantum Structures and Devices #Spontaneous emission #cond-mat.mes-hall
paper · pdf · doi:10.1103/physrevb.80.115312
published as Physical Review B 80, 11 (2009) 115312
arxiv created 2009/06/03 · openalex publication_date 2009/09/10 · arxiv updated 2015/05/13 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
The light-emission rate of a single quantum dot can be drastically enhanced by embedding it in a resonant semiconductor microcavity. This phenomenon is known as the Purcell effect and the coupling strength between emitter and cavity can be quantified by the Purcell factor. The most natural way for probing the Purcell effect is a time-resolved measurement. However, this approach is not always the most convenient one and alternative approaches based on a continuous-wave measurement are often more appropriate. Various signatures of the Purcell effect can indeed be observed using continuous-wave measurements (increase in the pump rate needed to saturate the quantum dot emission, enhancement of its emission rate at saturation, and change in its radiation pattern), signatures which are encountered when a quantum dot is put on resonance with the cavity mode. All these observations potentially allow one to estimate the Purcell factor. In this paper, we carry out these different types of measurements for a single quantum dot in a pillar microcavity and we compare their reliability. We include in the data analysis the presence of independent, nonresonant emitters in the microcavity environment, which are responsible for a part of the observed fluorescence.