1997
DOI: 10.1117/12.271212
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<title>Sb-based infrared materials and photodetectors for the near-room-temperature applications</title>

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Cited by 3 publications
(8 citation statements)
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“…On the assumption that the photons with energy lower than E g, GaSb all cross GaSb without any weakening, the main absorption appears in the Ga 0. 8 The maximum value of D * is obtained at l = 2.32 mm for the N 1 ±n 2 ±p structure with the frontside illuminated case and for the P 1 ±p 2 ±n structure with the backside illuminated case. In the following, the detectivity for the above two cases is calculated at l = 2.32 mm.…”
Section: Resultsmentioning
confidence: 99%
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“…On the assumption that the photons with energy lower than E g, GaSb all cross GaSb without any weakening, the main absorption appears in the Ga 0. 8 The maximum value of D * is obtained at l = 2.32 mm for the N 1 ±n 2 ±p structure with the frontside illuminated case and for the P 1 ±p 2 ±n structure with the backside illuminated case. In the following, the detectivity for the above two cases is calculated at l = 2.32 mm.…”
Section: Resultsmentioning
confidence: 99%
“…8 which all photons with the energy lower than the material bandgap are assumed to cross this material and to reach the next material without any loss. That is, the weakening of the incident light due to impurity absorption and lattice scattering etc.…”
Section: Resultsmentioning
confidence: 99%
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“…Photoconductors. Uncooled and Peltier-cooled long wavelength photoconductors were obtained at the Center of Quantum Devices [75][76][77]. The devices are based on p-InAsSb/ p-InSb heterostructures, MOCVD-grown on InSb-buffered GaAs substrates.…”
Section: Bulk Inassb Detectorsmentioning
confidence: 99%