2013
DOI: 10.1063/1.4835055
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Influence of radiative and non-radiative recombination on the minority carrier lifetime in midwave infrared InAs/InAsSb superlattices

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Cited by 101 publications
(46 citation statements)
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“…In a recent study, the recombination mechanism limiting the minority carrier lifetime in these superlattices was identified as the radiative lifetime [7]. In that study, the SRH and Auger lifetimes were estimated to $10 ls and $50 ls, respectively, at 77 K, whereas the radiative lifetime was in the order of 3 ls [7]. The terms in Eq.…”
Section: Contents Lists Available At Sciencedirectmentioning
confidence: 98%
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“…In a recent study, the recombination mechanism limiting the minority carrier lifetime in these superlattices was identified as the radiative lifetime [7]. In that study, the SRH and Auger lifetimes were estimated to $10 ls and $50 ls, respectively, at 77 K, whereas the radiative lifetime was in the order of 3 ls [7]. The terms in Eq.…”
Section: Contents Lists Available At Sciencedirectmentioning
confidence: 98%
“…The InAs/ InAsSb SL structure and the growth conditions were nominally the same as described in detail in Ref. [7]. The SLs bandgaps and minority carrier lifetimes were measured by photoluminescence (PL) and optical modulation response (OMR).…”
Section: Contents Lists Available At Sciencedirectmentioning
confidence: 99%
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“…However, in the extrinsic region the dominant recombination mechanisms are radiative and SRH, assuming the SRH lifetime does not depend on carrier concentration, for higher doping condition the radiative processes are expected to become dominant. 2 Noteworthy is the behavior of the Auger(e-e) in the extrinsic region of the semiconductor. This behavior is attributed to the observation that the Auger lifetime s Auger = Const.…”
Section: Measured and Modeled Recombination Lifetimementioning
confidence: 99%
“…25,26 Furthermore, trends of increase followed by decrease at 77-300 K are also reported in n type InAs/InAs 0.72 Sb 0.28 superlattice and HgCdTe due to competitive relaxation via different channels. [27][28][29] In terms of temperature, the SRH, Auger and radiative lifetimes can be described by Refs. 25-28,30 τ SRH =P 1 T 1/2 , τ Rad =P 2 T 3/2 , and τ Auger = P 3 ( equation (1), µ = m e /m h , m e and m h are the electron and hole effective masses, respectively.…”
Section: F Photoluminescence Lifetimesmentioning
confidence: 99%