2014
DOI: 10.1088/0022-3727/47/6/065103
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A versatile phenomenological model for the S-shaped temperature dependence of photoluminescence energy for an accurate determination of the exciton localization energy in bulk and quantum well structures

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Cited by 42 publications
(23 citation statements)
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“…The reduction in the peak intensity is attributed to the increase in nonradiative recombination of carriers due to thermal quenching. 24 As shown in Fig. 4(c), E a energy also increases as the AlN composition increases in the MQW (E a % 16 meV, 16 meV, 18 meV, and 25 meV, for samples D, C, B, and A, respectively).…”
mentioning
confidence: 73%
“…The reduction in the peak intensity is attributed to the increase in nonradiative recombination of carriers due to thermal quenching. 24 As shown in Fig. 4(c), E a energy also increases as the AlN composition increases in the MQW (E a % 16 meV, 16 meV, 18 meV, and 25 meV, for samples D, C, B, and A, respectively).…”
mentioning
confidence: 73%
“…Beyond this temperature, free carrier recombination dominates, and the regular temperature-induced band gap shrinkage occurs due to the electron-phonon interaction and lattice relaxation. Although the overall temperature behavior of the PL in thin films and nanowires is the same, in the nanowires, an additional red-blue shift is observed around 50 K. Such an additional feature is normally reported to be due to splitting of the heavy hole (HH) and light hole (LH) leading to the corresponding excitonic transitions [ 24 ]. However, the PL spectra shown in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…At lower powers an S-shaped dependence develops (Fig. 8), commonly attributed to potential fluctuations in the InGaAs QW layer [26][27][28]. Though there is little difference between the QW and SML temperature dependencies [29], it can be seen that the S-shaped curve is slightly more pronounced for the QW.…”
Section: Comparison With Quantum Well Samplementioning
confidence: 99%