2003
DOI: 10.1016/s0925-3467(03)00140-x
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Radiative N-localized recombination and confinement in GaAsN/GaAs epilayers and quantum well structures

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Cited by 21 publications
(10 citation statements)
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“…However, at low temperatures a theoretical (Varshni) model fails to fit the experimental data. At 10 K, the shift between theoretical and experimental values, may be due to the recombination of photogenerated carriers trapped by localized states within BGaAs as previously observed in GaAsN [14,15]. This phenomenon is observed in GaAsN, which exhibit an anomalous behaviour.…”
Section: Resultssupporting
confidence: 60%
“…However, at low temperatures a theoretical (Varshni) model fails to fit the experimental data. At 10 K, the shift between theoretical and experimental values, may be due to the recombination of photogenerated carriers trapped by localized states within BGaAs as previously observed in GaAsN [14,15]. This phenomenon is observed in GaAsN, which exhibit an anomalous behaviour.…”
Section: Resultssupporting
confidence: 60%
“…The PL peak blue shift with increasing temperature below 60 K for sample A, as shown in Fig. 2(a), has been reported in ternary (GaAsBi, 16 GaInP 2 , 17 and GaAsN 18 ), quantum well (QW) (GaSb/GaAs, 19 InAs/GaSb, 20 and GaAsSbN/GaAs 21,22 ) and SL (InAs/GaSb, 23 InGaAs/GaAsSb, 24 InGaN/AlGaN 25 ) materials. Two explanations have been assigned to this behavior in the literature.…”
Section: Discussionsupporting
confidence: 61%
“…We note that the PL peak energies decrease with temperature but the shift is smaller than observed in GaAs material [7] . An "S-Shape" phenomenon appears for the highly Si-doped sample(c) in the temperature range of 10-130 K; it is attributed to the recombination of photogenerated carriers trapped by localized states in GaAsN, as previously observed by Dumont et al [18] . The PL peak energies at high temperature were fitted using the BoseEinstein statistical expression [19] :…”
Section: Resultssupporting
confidence: 73%