H.A. Nickel 1 ) (a), G.S. Herold (a), T. Yeo (a), G. Kioseoglou (a), Z.X. Jiang (a), B.D. McCombe (a), A. Petrou (a), D. Broido (b), and W. Schaff (c)
Many body effects and internal transitions of confined excitons in GaAs and CdTe quantum wells
β Scribed by C.J. Meining; H.A. Nickel; A.B. Dzyubenko; A. Petrou; M. Furis; D.R. Yakovlev; B.D. McCombe
- Publisher
- Elsevier Science
- Year
- 2003
- Tongue
- English
- Weight
- 626 KB
- Volume
- 127
- Category
- Article
- ISSN
- 0038-1098
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β¦ Synopsis
Many body effects contribute significantly to the energy states of electron -hole pairs confined in quantum wells in the presence of excess electrons. We present results of optically detected resonance spectroscopy of the internal transitions of photo-excited electron -hole pairs in the presence of excess electrons for GaAs QWs and CdTe QWs. Compared to the case of isolated negatively charged excitons, excess electrons produce a large blue shift of the internal transitions in modulation-doped GaAs quantum wells (QWs) for filling factor , 2, and similar effects are found in CdTe QWs. For filling factor .2 no internal transitions are observed. These measurements demonstrate the strong effects of electron -electron correlations on the internal transitions of charged excitons in these quasi-2D systems and the importance of magnetic translation invariance. In the presence of excess electrons, the observed internal transitions are those of a magnetoplasmon bound to a mobile valence band hole.
π SIMILAR VOLUMES
Studies of shallow donor impurities confined in semiconductor quantum-well (QW) structures are reviewed, concentrating on recent experimental (far infrared spectroscopy) and theoretical investigations of negative donor ions (D Β± Β± ) and the effects of excess electrons on the donor-related transition
## Abstract The effects of intense laser radiation on the exciton states in GaAsβGa~1β__x__~Al~__x__~As quantum wells are studied with the inclusion of applied dc electric fields oriented along the growth direction of the system. The calculations are made within the effective mass and parabolic ban