State-filling and magneto-photoluminescence of excited states in InGaAs/GaAs self-assembled quantum dots
β Scribed by S. Raymond; S. Fafard; P.J. Poole; A. Wojs; P. Hawrylak; C. Gould; S. Sachrajda; S. Charbonneau; D. Leonard; R. Leon; P.M. Petroff; J.L. Merz
- Publisher
- Elsevier Science
- Year
- 1997
- Tongue
- English
- Weight
- 569 KB
- Volume
- 21
- Category
- Article
- ISSN
- 0749-6036
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β¦ Synopsis
We present the first radiative lifetime measurements and magneto-photoluminescence results of excited states in InGaAs/GaAs semiconductor self-assembled quantum dots. By increasing the photo-excitation intensity, excited state interband transitions up to n = 5 can be observed in the emission spectrum. The dynamics of the interband transitions and the inter-sublevel relaxation in these zero-dimensional energy levels lead to state-filling of the lower-energy states, allowing the quasi-Fermi level to be raised by more than 200 meV due to the combined large inter-sublevel spacing and the low density of states. The decay time of each energy level obtained under various excitation conditions is used to evaluate the inter-sublevel thermalization time. Finally, the emission spectrum of the dots filled with an average of about eight excitons is measured in magnetic fields up to 13 Tesla. The dependences of the spectrum as a function of carrier density and magnetic field are compared to calculations and interpreted in terms of coherent many-exciton states and their destruction by the magnetic field.
π SIMILAR VOLUMES
We have characterized self-assembled InAs quantum dots grown on the top of a single InGaAs/GaAs quantum well (QD's:QW) by measuring photoluminescence (PL) spectra as an effective technique. We have found that the linewidths of the PL peaks for the QD's:QW are narrower than that for the InAs quantum
We present a theoretical study of the optical anisotropy in the emission spectra from multiexciton complexes in InAs/GaAs selfassembled quantum dots by empirical tight-binding and configuration-interaction approaches. The linear polarization in the multiexciton emission is calculated as a function o