2010
DOI: 10.1002/pssc.200983278
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Cathodoluminescence of wide‐band‐gap II‐VI quaternary alloys

Abstract: Cathodoluminescence has been applied to study 1‐μm‐thick Zn1‐xMgxSySe1‐y alloys grown by molecular beam epitaxy. The observed cathodoluminescence spectra show the main band transition at 2.9 eV and a broad defect band around 2.2 eV. The analysis of the band intensities at different electron‐beam current densities shows different saturation behaviour of the defect band intensities for the samples. The saturation intensity and the luminescence lifetime correlate with the defect luminescence intensity and concent… Show more

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“…Since the probability of a carrier to be trapped into defects will be proportional with the number of available empty defect states, the trapping dynamics will vary with the occupation of the defect states by electrons. Thus, an excitation-density dependent trapping dynamics is expected, which has a similar origin as observed in other defect-related phenomena showing saturation behaviors at high excitation intensities [19]. Figure 2 shows the dependence of the pump-probe signal on the pump intensity for the LD-A sample.…”
Section: Resultssupporting
confidence: 72%
“…Since the probability of a carrier to be trapped into defects will be proportional with the number of available empty defect states, the trapping dynamics will vary with the occupation of the defect states by electrons. Thus, an excitation-density dependent trapping dynamics is expected, which has a similar origin as observed in other defect-related phenomena showing saturation behaviors at high excitation intensities [19]. Figure 2 shows the dependence of the pump-probe signal on the pump intensity for the LD-A sample.…”
Section: Resultssupporting
confidence: 72%