2013
DOI: 10.1117/12.2018427
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MWIR InAsSb barrier detector data and analysis

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Cited by 14 publications
(9 citation statements)
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“…41 Utilization of InAsSb absorber on GaAs substrates instead of HgCdTe absorber enables fabrication of MWIR low-cost, large-format HOT FPAs. Souza and co-workers [42][43][44] The measured dark current density in the pyramidal structured diodes is reduced by a factor of 3 in comparison with conventional diodes with the bulk absorber, which is consistent with volume reduction due to the creation of the absorber topology. High detectivity (>10 10 cmHz 1/2 /W) and high internal quantum efficiency (>90%) have been achieved over the entire 0.5 lm to 5.0 lm spectral range.…”
Section: Photon Trapping Detectorssupporting
confidence: 69%
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“…41 Utilization of InAsSb absorber on GaAs substrates instead of HgCdTe absorber enables fabrication of MWIR low-cost, large-format HOT FPAs. Souza and co-workers [42][43][44] The measured dark current density in the pyramidal structured diodes is reduced by a factor of 3 in comparison with conventional diodes with the bulk absorber, which is consistent with volume reduction due to the creation of the absorber topology. High detectivity (>10 10 cmHz 1/2 /W) and high internal quantum efficiency (>90%) have been achieved over the entire 0.5 lm to 5.0 lm spectral range.…”
Section: Photon Trapping Detectorssupporting
confidence: 69%
“…Photon trapping detectors have been demonstrated independently in II-VI 38,39,41 and III-V [41][42][43][44] based epitaxial materials. Sub-wavelength in size semiconductor pillar arrays within a single detector have been designed and structured as an ensemble of 3D photonic structure units using either a top-down or bottom-up process scheme to significantly increase absorption and quantum efficiency.…”
Section: Photon Trapping Detectorsmentioning
confidence: 99%
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“…Figure 9 shows an example of the similar nBn structure considered theoretically by Martyniuk and Rogalski [28] and the I−V characteristics as a function of temperature taken from Ref. 29. The alloy composition of x = 0.195 for the InAs 1-x Sb x absorber layer provided a cutoff wavelength 4.9 μm at 150 K. J dark is 1.0×10 -3 A/cm 2 at 200 K and 3.0×10 -6 A/cm 2 at 150 K. The detectors are dominated by diffusion currents at -1.0 V bias where the quantum effi− ciency peaks.…”
Section: Mwir Inassb Barrier Detectorsmentioning
confidence: 99%
“…The alloy compositions of x = 0.09 to 0.2 for the InAs1-xSbx absorber layers provided the λcut-off wavelengths of ~4.1 to ~5.0 μm at 150 K, respectively. The current-voltage characteristics were taken from [155]. The dark current density for nBn InAs0.805Sb0.195 structure was 1.0 × 10 −3 A/cm 2 at 200 K and 3.0 × 10 −6 A/cm 2 at 150 K. In nBn InAsSb detector, the depletion current is totally suppressed (see Figure 47c) because there is no depletion region.…”
Section: Barrier Detectorsmentioning
confidence: 99%