2018 IEEE 18th International Conference on Nanotechnology (IEEE-NANO) 2018
DOI: 10.1109/nano.2018.8626250
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Computational design of metamorphic In(N)AsSb mid-infrared light-emitting diodes

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Cited by 2 publications
(10 citation statements)
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“…To facilitate comparison to experiment we perform SE calculations at a fixed carrier density n = 10 15 cm −3 per QW, a low value selected to replicate a typical carrier density associated with optical excitation in the PL measurements for the structures under investigation. Full details of the theoretical model-which is based upon that we have previously developed to analyse the properties of 1.3 µm metamorphic QW lasers, as well as near-and mid-infrared dilute bismide QW lasers [27][28][29][30]-will be presented in [31]. We assume ideal, compressively strained InAs 1−x Sb x QWs of thickness 10.5 nm, surrounded by unstrained Al 0.125 In 0.875 As barriers.…”
Section: Theoretical Modelmentioning
confidence: 99%
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“…To facilitate comparison to experiment we perform SE calculations at a fixed carrier density n = 10 15 cm −3 per QW, a low value selected to replicate a typical carrier density associated with optical excitation in the PL measurements for the structures under investigation. Full details of the theoretical model-which is based upon that we have previously developed to analyse the properties of 1.3 µm metamorphic QW lasers, as well as near-and mid-infrared dilute bismide QW lasers [27][28][29][30]-will be presented in [31]. We assume ideal, compressively strained InAs 1−x Sb x QWs of thickness 10.5 nm, surrounded by unstrained Al 0.125 In 0.875 As barriers.…”
Section: Theoretical Modelmentioning
confidence: 99%
“…Extending the emission wavelength beyond 4 µm would then require careful QW design and optim isation. For example, via incorporation of nitrogen (N) to form dilute nitride InN z (As 1−x Sb x ) 1−z QWs, where the band anti-crossing interaction associated with N impurity states brings about a simultaneous reduction of the band gap and lattice constant [38,39], allowing increased flexibility via strain engineering and allowing for the design of metamorphic type-I QWs having large CB offsets and emission wavelengths 4 µm [31,40].…”
Section: Structurementioning
confidence: 99%
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“…Before proceeding, we emphasise the link between Eqs. (10) and (11) and the widely employed Kane model for BTBT in a direct-gap semiconductor. 39,40 Given Kane's use of a semi-classical wave function phase in his analysis of BTBT, his approximate result for T (and hence G) is formally equivalent to Eqs.…”
Section: B Btbt Transmission Coefficient and Generation Ratementioning
confidence: 99%
“…39,40 Given Kane's use of a semi-classical wave function phase in his analysis of BTBT, his approximate result for T (and hence G) is formally equivalent to Eqs. (10) and (11). 41 Indeed, Kane's analytical result for T can be straightforwardly obtained from Eq.…”
Section: B Btbt Transmission Coefficient and Generation Ratementioning
confidence: 99%