2015
DOI: 10.1007/s11664-015-3824-3
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Linear-Mode HgCdTe Avalanche Photodiodes for Photon-Counting Applications

Abstract: An overview of recent improvements in our understanding of, and the maturity of, linear-mode photon counting with the HgCdTe electron-initiated avalanche photodiode is presented. In 2010 DRS fabricated an experimental 2 9 8 array with (64 lm) 2 pixels which enabled, for the first time, linear-mode photon counting by use of the MWIR cutoff HgCdTe electron-initiated avalanche photodiode. The device had a high single-photon signal-to-noise ratio of 13.7, an excess noise factor of 1.3-1.4, a 7 ns minimum time betw… Show more

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Cited by 24 publications
(38 citation statements)
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“…4 are close to theoretical predictions and simulations. 4 Greater than OD4 is equivalent to optical transmission less than 10 -4 or < 0.01%. OD stands for "Optical Density".…”
Section: Resultsmentioning
confidence: 99%
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“…4 are close to theoretical predictions and simulations. 4 Greater than OD4 is equivalent to optical transmission less than 10 -4 or < 0.01%. OD stands for "Optical Density".…”
Section: Resultsmentioning
confidence: 99%
“…Right: 16-pixel mean PDE vs. FER showing ≥50% PDE across all pixels on both arrays at a FER of <200 kHz (A8327-14)[4].…”
mentioning
confidence: 99%
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“…5 DRS also produced a set of 2 × 8 pixel prototype APD arrays with lower dark current and higher APD gains, which enabled LMPC. 1,6 Recently, DRS successfully integrated a 2 × 8-pixel HgCdTe APD FPA with a microlens array and a mini-Stirling cooler into an integrated detector cooler assembly (IDCA). 7,8 These new HgCdTe APD arrays and the IDCAs were characterized at both DRS and NASA GSFC and underwent environmental tests.…”
Section: Introductionmentioning
confidence: 99%