2022
DOI: 10.1002/adom.202201082
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Optical Manipulation of the Rashba Effect in Germanium Quantum Wells

Abstract: The Rashba effect in Ge/Si0.15Ge0.85 multiple quantum wells embedded in a p‐i‐n diode is studied through polarization and time‐resolved photoluminescence. In addition to a sizeable redshift arising from the quantum‐confined Stark effect, a threefold enhancement of the circular polarization degree of the direct transition is obtained by increasing the pump power over a 2 kW cm−2 range. This marked variation reflects an efficient modulation of the spin population and is further supported by dedicated investigati… Show more

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Cited by 4 publications
(8 citation statements)
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“…The weaker peak shifted to higher energies by 27 meV is the corresponding no-phonon (NP) cL1 − HH1 emission. 12,15,17 Additionally, the low-energy tail of a broad emission from defect states is superimposed on such indirect-gap transitions. Finally, the peak at 0.945 eV is due to the cΓ1 − HH1 optical transition at the center of the Brillouin zone.…”
Section: Resultsmentioning
confidence: 99%
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“…The weaker peak shifted to higher energies by 27 meV is the corresponding no-phonon (NP) cL1 − HH1 emission. 12,15,17 Additionally, the low-energy tail of a broad emission from defect states is superimposed on such indirect-gap transitions. Finally, the peak at 0.945 eV is due to the cΓ1 − HH1 optical transition at the center of the Brillouin zone.…”
Section: Resultsmentioning
confidence: 99%
“…2(a) shows that the ratio between the indirect LA and NP transitions changes markedly with the external bias. 12 The former decreases more rapidly than the latter, opening intriguing questions about electron-phonon interaction. Finally, it can be noticed that the defect tail appears to have lost its spectral weight, thus suggesting a suppression of the carrier recombination events from the defects states.…”
Section: Resultsmentioning
confidence: 99%
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