2017
DOI: 10.1117/12.2249126
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Multi-wavelength mid-IR light source for gas sensing

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Cited by 7 publications
(1 citation statement)
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“…For instance, emitters in the 2.35–2.6 μm range are useful for sensing temperature and gas molecules such as CO, H 2 O, SO 2 , and HF. These applications call for broadband emitters such as light emitting diodes (LEDs), particularly for spectroscopic detection of these critical gases generated in a chemical plant or for their atmospheric monitoring. , The commercially available LEDs emitting at the 2–5 μm wavelength range are dominated by III–V compound semiconductors. The III–V LEDs that exhibit an emission peak below 2.35 μm are predominately made of GaInAsSb/AlGaAsSb, whereas InAsSb/InAsSbP is used for those emitting above 2.6 μm. However, these III–V devices suffer an inherent emission gap in the 2.35–2.6 μm range due to material limitations . Additionally, the III–V LEDs emitting at wavelengths longer than 2.6 μm exhibit significantly lower output power if operated in continuous wave mode as compared to pulse mode. , Although GaSb-based lasers and superluminescent LEDs possess higher tunability of the emitted wavelength, their narrow band emission remains less favorable for spectroscopic gas detection. , Notwithstanding the progress in developing III–V LEDs, these materials remain costly, and their direct growth on silicon is typically associated with a degradation of device performance, thus hindering their integration in large-scale applications.…”
Section: Introductionmentioning
confidence: 99%
“…For instance, emitters in the 2.35–2.6 μm range are useful for sensing temperature and gas molecules such as CO, H 2 O, SO 2 , and HF. These applications call for broadband emitters such as light emitting diodes (LEDs), particularly for spectroscopic detection of these critical gases generated in a chemical plant or for their atmospheric monitoring. , The commercially available LEDs emitting at the 2–5 μm wavelength range are dominated by III–V compound semiconductors. The III–V LEDs that exhibit an emission peak below 2.35 μm are predominately made of GaInAsSb/AlGaAsSb, whereas InAsSb/InAsSbP is used for those emitting above 2.6 μm. However, these III–V devices suffer an inherent emission gap in the 2.35–2.6 μm range due to material limitations . Additionally, the III–V LEDs emitting at wavelengths longer than 2.6 μm exhibit significantly lower output power if operated in continuous wave mode as compared to pulse mode. , Although GaSb-based lasers and superluminescent LEDs possess higher tunability of the emitted wavelength, their narrow band emission remains less favorable for spectroscopic gas detection. , Notwithstanding the progress in developing III–V LEDs, these materials remain costly, and their direct growth on silicon is typically associated with a degradation of device performance, thus hindering their integration in large-scale applications.…”
Section: Introductionmentioning
confidence: 99%