2007
DOI: 10.1016/j.jlumin.2007.03.009
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Kinetic effects in recombination of optical excitations in disordered quantum heterostructures: Theory and experiment

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Cited by 9 publications
(20 citation statements)
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References 28 publications
(57 reference statements)
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“…3 is the theoretical fit to experimental data points represented by solid circles ͑b͒. 20,21 As the temperature increases, the carriers in lower lying localized states are thermalised to occupy higher energy localized states and the carriers approach to an equilibrium energy distribution resulting in narrowing of PL line width 20 in the temperature range 100 K Ͻ T Ͻ 150 K at excitation intensity of 4 kW/ cm 2 . ͑1͒ and ͑2͒, indicating the dominance of temperature-induced band gap shrinkage.…”
Section: Resultsmentioning
confidence: 99%
“…3 is the theoretical fit to experimental data points represented by solid circles ͑b͒. 20,21 As the temperature increases, the carriers in lower lying localized states are thermalised to occupy higher energy localized states and the carriers approach to an equilibrium energy distribution resulting in narrowing of PL line width 20 in the temperature range 100 K Ͻ T Ͻ 150 K at excitation intensity of 4 kW/ cm 2 . ͑1͒ and ͑2͒, indicating the dominance of temperature-induced band gap shrinkage.…”
Section: Resultsmentioning
confidence: 99%
“…The theoretical approach is based on a kinetic Monte Carlo algorithm. It has been successfully applied to reproduce both time-resolved 12 and time-integrated spectra, 13,14 in particular also for the Ga͑AsBi͒/GaAs material system. 11 Here, this model is based on the assumption that the valence band disorder results in a landscape of localized states.…”
mentioning
confidence: 99%
“…At low temperatures below 100 K, carriers hop between the localized states randomly distributed in space and energy resulting in a rapid increase in the FWHM of the PL emission band. 29,30 As temperature increases further, the carriers in lower lying localized states are thermally activated to occupy higher energy localized states and gradually approach to an equilibrium energy distribution, which leads to a decrease of FWHM of PL emission band 29 in the temperature range of 100 K < T < 200 K. At sufficiently high temperatures (beyond 200 K), the FWHM increases again in accordance with the thermal broadening of PL line shape. 31 However, in unalloyed semiconductors with the absence of carrier localization, the FWHM increases monotonically with temperature which can be expressed by the following relation: 32 CðTÞ ¼ Cð0Þ þ aT þ b=½expð hx LO =k B TÞ À 1;…”
Section: Resultsmentioning
confidence: 89%