Resonantly driven coherent oscillations in a solid-state quantum emitter

By E. Flagg, A. Muller, J. Robertson, S. Founta, Dennis Deppe, M. Xiao, Wenquan Ma, Gregory J. Salamo, C. Shih. 2009

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Cascaded single-photon emission from the Mollow triplet sidebands of a quantum dot (2011, methodology): “The signal around zero delay exhibits clear antibunching with a normalized value of g((2))(t)1⁄4 0.”
Interfacing single photons and single quantum dots with photonic nanostructures (2013, unknown): “…for the photon autocorrelation function is obtained by extending the textbook calculation of Scully and Zubairy (2001) to include dephasing (Flagg et al., 2009), g(2)(τ) = (43) 1− e−(3γ/4+γdp/2)τ ( cos(µτ) + 3γ + 2γdp 4µ sin(µτ) ) , where µ = √ 4 |Ωp|2 − (γ/4− γdp/2)2 is the effective Rabi…”
Non-resonant dot–cavity coupling and its potential for resonant single-quantum-dot spectroscopy (2009, methodology): “The experimental data has been fitted by a theoretical model [21] to describe the emission saturation of a resonantly excited two-level system (see also methods section).”
Quantum dot Rabi rotations beyond the weak exciton–phonon coupling regime (2010, background): “Experimentally, it is generally the excitonic population ρXX that is measured, through photocurrent detection [8, 11] or microcavity-asissted photon emission [13, 14], for example.”