1989
DOI: 10.1063/1.101962
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Capture of photoexcited carriers by a laser structure

Abstract: The capture of photoexcited carriers in different laser structures is investigated by subpicosecond luminescence spectroscopy. The capture time at 20 and 80 K is monitored by the decay of the luminescence of the confinement layers. It is found to range between 2 and 3 ps for both linear and parabolic grading, and to be much longer in nongraded structures. The improvement of the capture in the case of graded structures is due to the quasi-electric field experienced by the carriers, and might allow the devices t… Show more

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Cited by 45 publications
(6 citation statements)
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“…Indeed, when carriers need more time to access the quantum structure than they need to leave it, the temporal response shows the arrival time as a decay time and the leaving time as a rise time. This also assumes very short trapping times in the different quantum structures, in very good agreement with other measurements [14].…”
Section: Vqw Emissionsupporting
confidence: 78%
“…Indeed, when carriers need more time to access the quantum structure than they need to leave it, the temporal response shows the arrival time as a decay time and the leaving time as a rise time. This also assumes very short trapping times in the different quantum structures, in very good agreement with other measurements [14].…”
Section: Vqw Emissionsupporting
confidence: 78%
“…A correlation between the upper limit of the modulation bandwidth and structural parameters, like the width of the separate-confinement heterostructure ͑SCH͒, has been established by measuring modulation response in the small signal regime, 1,2 or by using optical modulation. 6 Investigations were performed on undoped structures at low temperatures. 4 Time-resolved photoluminescence ͑PL͒ has proven to be especially suitable to study carrier transport in bulk and QW semiconductor structures.…”
mentioning
confidence: 99%
“…In addition, a slight increase in the PL linewidth for both the exciton and the biexciton is observed at similar densities in Fig. 3b, which can be ascribed to collisional-induced broadening 19 . Figure 3b also depicts the determined bandgap energy that characteristically shifts to lower energy with increasing n because of bandgap renormalization (BGR).…”
Section: Nature Communications | Doimentioning
confidence: 61%
“…2c) features a characteristic plateau-like QW emission that extends from the biexciton emission energy continuously up to the barrier energy. The saturation of the emission amplitude at early delays is the direct signature of k-space filling of the constant 2D density-of-states and indicates the presence of a degenerate e-h plasma in the QW 19 . For the high-injection PL spectra at early time delays, that is within the first 300 ps, an e-h plasma lineshape fitting following the model discussed in refs 11,20 was employed (cf.…”
Section: Resultsmentioning
confidence: 99%