1976
DOI: 10.1103/physrevb.13.5410
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Impact ionization of excitons in GaAs

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Cited by 90 publications
(28 citation statements)
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“…The excitonic PL spectra consist of a series of lines: [Be, X], X e1−hh1 and X e1−lh1 . The binding energy of bound exciton E(X e1−hh1 ) − E[Be, X] ≈ 3.85 meV nicely coincides with other experimental findings for GaAs/AlAs (3.7 meV) [9], and for GaAs/Al 0.33 Ga 0.67 As (3.8 meV) [11] quantum wells, which is larger than for GaAs (2.9 meV) [12]. Modeling the lineshape Γ we assumed that the excitonic PL line width broaden- Fig.…”
Section: Photoluminescence Spectra and Discussionsupporting
confidence: 88%
“…The excitonic PL spectra consist of a series of lines: [Be, X], X e1−hh1 and X e1−lh1 . The binding energy of bound exciton E(X e1−hh1 ) − E[Be, X] ≈ 3.85 meV nicely coincides with other experimental findings for GaAs/AlAs (3.7 meV) [9], and for GaAs/Al 0.33 Ga 0.67 As (3.8 meV) [11] quantum wells, which is larger than for GaAs (2.9 meV) [12]. Modeling the lineshape Γ we assumed that the excitonic PL line width broaden- Fig.…”
Section: Photoluminescence Spectra and Discussionsupporting
confidence: 88%
“…We attribute the brightening effect to the elimination of nearsurface fields in the GaAs and InP samples under optical illumination [58]. There is evidence that very small fields, on the order of V/cm, can substantially quench fluorescence [59]. We do not observe this effect in CdTe, which is a true bulk sample rather than a few-micron-thick film.…”
Section: Appendix C: Surface Depletion Effectsmentioning
confidence: 56%
“…5 The effect of an external magnetic field on filaments has been investigated by a scanning laser microscope. [9][10][11] Ryabushkin et al 12 reported a strong spatial variation, in a direction perpendicular to the current flow, of photoluminescence emitted by n-GaAs epitaxial layers in the filamentary current regime. Irradiation destabilizes the current flow especially at the filament borders.…”
Section: H Kostialmentioning
confidence: 99%