Abstract
While the advanced coherent control of qubits is now routinely carried out in low frequency (GHz) systems like single spins, it is far more challenging to achieve for two-level systems in the optical domain. This is because the latter evolve typically in the THz range, calling for tools of ultrafast, coherent, nonlinear optics. Using four-wave mixing micro-spectroscopy, we here measure the optically driven dynamics of a single exciton quantum state confined in a semiconductor quantum dot. In a combined experimental and theoretical approach, we reveal the intrinsic Rabi oscillation dynamics by monitoring both central exciton quantities, i.e., its occupation and the microscopic coherence, as resolved by the four-wave mixing technique. In the frequency domain this oscillation generates the Autler-Townes splitting of the light-exciton dressed states, directly seen in the four-wave mixing spectra. We further demonstrate that the coupling to acoustic phonons strongly influences the FWM dynamics on the picosecond timescale, because it leads to transitions between the dressed states.
Highlights
The coherent control of individual spins and excitons in quantum dots (QDs) has been the scope of semiconductor quantum optics since many years
We have recently shown that the pulse areas θi of the driving laser fields in four-wave mixing (FWM) experiments have a strong influence on the system’s dynamics between the pulses
By driving the system with sub- and super-ps laser pulses and applying two- and three-pulse FWM techniques, we could isolate the dynamics of the microscopic polarization and the exciton occupation, respectively
Summary
The coherent control of individual spins and excitons in quantum dots (QDs) has been the scope of semiconductor quantum optics since many years. To unveil the potential lying in QDs and other single photon emitters for high-speed optical quantum technology, it is urgent to bring the manipulation schemes to perfection This is nowadays approached using individual spins in electrically defined [1] and epitaxial [2, 3] QDs, as well as in color centers in diamond [4, 5], which is conditioned by setting up robust spin-photon interfacing. This difficulty can be mitigated using QD excitons: because of their direct coupling to light, the related coherent control protocols operate on the picosecond (ps) timescale [6]. That these Rabi oscillations have to be differentiated from Rabi rotations [1, 9, 10, 26,27,28, 30, 31]
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