2016
DOI: 10.1117/12.2233537
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Candidate 10 micron HgCdTe arrays for the NEOCam space mission

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Cited by 5 publications
(3 citation statements)
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“…The arrays have cut-off wavelengths of ∼ 10 µm, low read noise, high quantum efficiency (QE), and have operabilities (well depth of more than 44,000 e − and dark current less than 200 e − /s ) > 90% up to temperatures of 42 K, and have been proton irradiated and demonstrated the ability to withstand the cosmic ray radiation that they are expected to receive in space. [12][13][14] These devices have reached NASA Technical Readiness Level-6.…”
Section: Prior Development / Neocammentioning
confidence: 99%
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“…The arrays have cut-off wavelengths of ∼ 10 µm, low read noise, high quantum efficiency (QE), and have operabilities (well depth of more than 44,000 e − and dark current less than 200 e − /s ) > 90% up to temperatures of 42 K, and have been proton irradiated and demonstrated the ability to withstand the cosmic ray radiation that they are expected to receive in space. [12][13][14] These devices have reached NASA Technical Readiness Level-6.…”
Section: Prior Development / Neocammentioning
confidence: 99%
“…irradiated and demonstrated the ability to withstand the cosmic ray radiation that they are expected to receive in space. [12][13][14] These devices have reached NASA Technical Readiness Level-6.…”
Section: Prior Development / Neocammentioning
confidence: 99%
“…Hawaii-1RG (H1RG) multiplexers [8][9][10] were chosen for the entire project because of the low power dissipation, ideal for passively cooled space missions, in addition to the small spread in the zero-bias point compared to other muxes. All four detector arrays had cutoff wavelengths ranging from 12.4 to 12.8 µm, measured at a temperature of 30 K. Two of the arrays (H1RG-18367 and 18508) had the same design as the LW10 detector arrays designed for the proposed NEOCam mission 7,11,12 extrapolated to longer wavelengths by decreasing the mole fraction of cadmium to mercury in the HgCdTe alloy, 13 while the other two arrays (H1RG-18369 and 18509) had two different TIS proprietary designs with the goal of mitigating quantum tunneling dark currents. 5,[14][15][16] The median dark current per pixel for three of the four arrays was below 1 e − /s at a temperature of 28 K and 150 mV of applied reverse bias, with a median well depth of ∼ 43 ke − .…”
Section: Lw13 Phase Summarymentioning
confidence: 99%