1990
DOI: 10.1103/physrevb.42.9472
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Localization effects, energy relaxation, and electron and hole dispersion in selectively dopedn-typeAlyGa<

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Cited by 18 publications
(8 citation statements)
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“…is the reduced mass. The electron effective mass is derived to be of m e * = (0.068 ± 0.003)m 0 (m 0 is the free electron mass), close to the value determined by Butov et al [34], but typically higher of that determined from the Shubnikov-de-Haas measurements.…”
Section: B Pl In Magnetic Fieldsupporting
confidence: 81%
See 1 more Smart Citation
“…is the reduced mass. The electron effective mass is derived to be of m e * = (0.068 ± 0.003)m 0 (m 0 is the free electron mass), close to the value determined by Butov et al [34], but typically higher of that determined from the Shubnikov-de-Haas measurements.…”
Section: B Pl In Magnetic Fieldsupporting
confidence: 81%
“…This deviation observed at low temperature is immediately connected with fluctuations of the local potential energy in the quantum well. According to Butov et al [34] at low excitation densities and low temperatures, the photoexcited holes occupy predominantly the low-energy states within the broadened Landau levels, and the transition energy is smaller than the gap between the corresponding electron and hole LL. The width of the n-th LL, Γ n , is determined by both magnitude of the fluctuations and their sizes.…”
Section: B Pl In Magnetic Fieldmentioning
confidence: 98%
“…[38]. One can see that simultaneously with the depletion of the electron LLs at high B an increase of the LL linewidth at even ν takes place (Fig.…”
Section: Introductionmentioning
confidence: 82%
“…Such nonlinearities of j j E -at even values of ν were explained by the many-body effects [37]. From linear fits of j j E -one can find the reduced transition mass as was found in [38] for InGaAs/GaAs QWs with In content 0 13 0 18,…”
Section: Introductionmentioning
confidence: 91%
“…In discussing the spatial randomness, three kinds of disorder source are to be considered. 21,22 One is the electrostatic random potential V remote as mentioned above. Although V remote affects the 2DEG state and depends strongly on the electron density, the contribution of V remote to the PL emission energy is small in our sample because the spatial length scale of this fluctuation s(= 250 nm) is much larger than the X − radius and the random energy shift cancels out in the emission energy after the electron-hole recombination.…”
mentioning
confidence: 99%