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Intra-dot relaxation and dephasing rates from time-resolved photoluminescence from InAs quantum dot ensembles
Authors:Alexej Chernikov  Swantje Horst  Stephan W. Koch  Sangam Chatterjee  Wolfgang W. Rühle  Julian Sweet  Benjamin Richards  Josh Hendrickson  Galina Khitrova  Hyatt M. Gibbs  Dimitri Litvinov  Dagmar Gerthsen  Martin Wegener
Affiliation:1. Institute of Veterinary Physiology, Vetsuisse Faculty and the Zürich Center for Integrative Human Physiology, University of Zürich, 8057 Zürich, Switzerland;2. Institute for Molecular Cell Biology and Research Centre for Molecular Imaging and Screening, Saarland University, 66421 Homburg/Saar, Germany;3. Clinic for Internal Medicine III, Saarland University, 66421 Homburg/Saar, Germany;4. Institute for Human Genetics, Saarland University, 66421 Homburg/Saar, Germany;5. Anatomy, Saarland University, 66421 Homburg/Saar, Germany
Abstract:An ensemble of InAs quantum dots with ground state transition energies centered at 1.216 eV and density 1011dots/cm2 has been studied by time-resolved photoluminescence (PL). The wavelength of the 100-fs excitation pulse was tuned through the ground (excited) state transitions, resulting in resonant (optical phonon sideband) PL. The decay of the PL was time resolved with a streak camera in the interval 1.5–3 ns to avoid scattered laser light. The intensity of the PL was recorded with its polarization both parallel with and perpendicular to the excitation polarization (along one of the crystal’s cleave axes); the ratio is 2.22 at low temperatures and low excitation. A phenomenological rate equation analysis is made, separating the excitations into two classes, one polarized along the excitation polarization and the other unpolarized (either that way immediately after the excitation pulse or scattered from the first class). Excellent fits to the data lead to the conclusion that both classes decay radiatively with a lifetime of 1 ns, and a transfer from the polarized to the unpolarized species takes place with a distribution time of 12 ns at low temperatures and low excitation, dropping rapidly toward zero for temperatures above 30 K and for intense excitation levels. The polarization of a coherently excited ground state exciton should dephase with a rate equal to the sum of the radiative rate plus the inverse of this distribution time.
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