2005
DOI: 10.1063/1.1885173
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Influence of trapping on the exciton dynamics of AlxGa1−xAs films

Abstract: We present a systematic study on the exciton relaxation in high purity AlGaAs epilayers. The time for the excitonic photoluminescence to reach its maximum intensity (tmax) shows a non-monotonic dependence on excitation density which is attributed to a competition between exciton localization and carrier-carrier scattering. A phenomenological four level model fully describes the influence of exciton localization on tmax. This localization effect is enhanced by the increase of the Al content in the alloy and dis… Show more

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Cited by 6 publications
(6 citation statements)
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“…For n < 3x10 15 cm -3 and T L up to 30 K, the monotonic increase of t r with density is related to the trapping of free excitons in bound states. 17 For higher excitation densities, the steady decrease of t r with increasing density arises from the fast relaxation of excitons induced by exciton-exciton scattering. 7 The second group, T L > 49 K (open symbols), corresponds to the metallic phase, with the onset of the PL dominated by the fast component (electron-hole pair recombination).…”
Section: Resultsmentioning
confidence: 99%
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“…For n < 3x10 15 cm -3 and T L up to 30 K, the monotonic increase of t r with density is related to the trapping of free excitons in bound states. 17 For higher excitation densities, the steady decrease of t r with increasing density arises from the fast relaxation of excitons induced by exciton-exciton scattering. 7 The second group, T L > 49 K (open symbols), corresponds to the metallic phase, with the onset of the PL dominated by the fast component (electron-hole pair recombination).…”
Section: Resultsmentioning
confidence: 99%
“…38 At a lattice temperature of 5 K the spectrum displays the characteristic excitonic emission (1.512-1.516 eV range) and electron-acceptor recombination structures at lower energies, which have been discussed in detail in Ref. 17. For temperatures up to a critical temperature, T c = 49 K, the spectra are dominated by the excitonic emission.…”
Section: Methodsmentioning
confidence: 91%
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“…10 In addition, this carrier migration between localized states may account for the long rise times in the x ¼ 0.40 TRPL spectra, depicted by the initial divergence from the fitted behavior. 36,37 Furthermore, the relaxation of cool excitons may also have to contend with localized states brought about by compositional disorder, which can conceivably account for the two-fold increase in s 2 for x ¼ 0.40 with respect to that for x ¼ 0.13. This assertion is based on the fact that localization is analogous to impurity-related binding of excitons and the radiative lifetime of bound excitons increases with binding energy.…”
Section: Resultsmentioning
confidence: 99%
“…7−9 Therefore, the exciton can be observed even at room temperature, which is unusual compared with 3D semiconducting materials, such as GaAs. 10,11 Additionally, the monolayer TMDC shows a direct band gap at K and K' points in the Brillouin zone, which can be expected for applying optical transistors, 12,13 light-emitting diodes, 6,14,15 photovoltaics, 16−18 and valley-dependent optoelectronics. 19−22 One drawback of the optical behavior in the monolayer TMDCs is the low optoelectronic quality.…”
Section: ■ Introductionmentioning
confidence: 96%