2013
DOI: 10.1103/physrevb.87.045313
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Fifth-order nonlinear optical response of excitonic states in an InAs quantum dot ensemble measured with two-dimensional spectroscopy

Abstract: Exciton, trion and biexciton dephasing rates are measured within the inhomogeneous distribution of an InAs quantum dot (QD) ensemble using two-dimensional Fourier-transform spectroscopy. The dephasing rate of each excitonic state is similar for all QDs in the ensemble and the rates are independent of excitation density. An additional spectral feature -too weak to be observed in the time-integrated four-wave mixing signal -appears at high excitation density and is attributed to the χ (5) biexcitonic nonlinear r… Show more

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Cited by 47 publications
(28 citation statements)
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“…However, singledot experiments, which require long signal integration times, still suffer from spectral diffusion effects that mask the intrinsic recombination dynamics [4,13,14]. These limitations can be avoided by investigating QD ensembles using spin noise spectroscopy [15,16] or nonlinear optical spectroscopy techniques, such as spectral hole burning [17][18][19], four-wave mixing [20], or coherent multidimensional spectroscopy [21,22]. An ultralong coherence time up to ∼1.5 ns, corresponding to a sub-μeV dephasing rate, has been measured for the positively charged exciton in InAs QDs at cryogenic temperature [23].…”
Section: Introductionmentioning
confidence: 99%
“…However, singledot experiments, which require long signal integration times, still suffer from spectral diffusion effects that mask the intrinsic recombination dynamics [4,13,14]. These limitations can be avoided by investigating QD ensembles using spin noise spectroscopy [15,16] or nonlinear optical spectroscopy techniques, such as spectral hole burning [17][18][19], four-wave mixing [20], or coherent multidimensional spectroscopy [21,22]. An ultralong coherence time up to ∼1.5 ns, corresponding to a sub-μeV dephasing rate, has been measured for the positively charged exciton in InAs QDs at cryogenic temperature [23].…”
Section: Introductionmentioning
confidence: 99%
“…For the experimental investigations we implement a heterodyne spectral interferometry technique [15] to retrieve polarization-resolved four-wave mixing (FWM) signals. While FWM has often been used to infer exciton dynamics in QWs [16] or for QD ensembles [17], for single QDs the experiments are more challenging because of the weak signal intensity. This longstanding issue has recently been solved by exploiting photonic nanostructures to enhance non-linear responses.…”
Section: Introductionmentioning
confidence: 99%
“…A particularly successful example is the Multidimensional Optical Nonlinear Spectrometer (MONSTR) experiment [34,46], combining active feedback with an ultrastable platform. The MONSTR has been able to capture coherence time and measure homogeneous linewidths of semiconductor QWs [7,47] and QD ensembles [48,49]. In this kind of experiment where mechanical delay lines are used, liquid crystal retarders can be added to implement phase-cycling algorithms as a way to further isolate the FWM signal from other contributions [34].…”
Section: Box Geometrymentioning
confidence: 99%
“…A power dependence to check that the signal intensity scales with P 3 (with P the average power in the excitation beams) is needed to ensure that the observed signal is dominated by third-order contributions -and can be used to separate higher-order contributions within a two-dimensional spectrum [49].…”
Section: Box Geometrymentioning
confidence: 99%