2015
DOI: 10.1117/12.2179216
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Low-dark current p-on-n MCT detector in long and very long-wavelength infrared

Abstract: This paper presents recent developments done at CEA-LETI Infrared Laboratory on processing and characterization of p-on-n HgCdTe (MCT) planar infrared focal plane arrays (FPAs) in LWIR and VLWIR spectral bands. These FPAs have been grown using liquid phase epitaxy (LPE) on a lattice matched CdZnTe substrate. This technology presents lower dark current and lower serial resistance in comparison with n-on-p vacancy doped architecture and is well adapted for low flux detection or high operating temperature. This a… Show more

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Cited by 13 publications
(9 citation statements)
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“…Nowadays, thermal imaging relies primarily on bulk epitaxial semiconductor materials. In mid-wave infrared (MWIR, 3-5 µm) and long-wave infrared (LWIR, 8-12 µm), it is dominated by narrow bandgap semiconductor material such as InSb [18], HgCgTe [19,20], quantum-wells [21] and type-II superlattices [22,23]. However, these materials were typically prepared by molecular beam epitaxy or chemical vapor deposition, which leads to high fabrication and processing costs.…”
Section: Synthesis Of Infrared Cqdsmentioning
confidence: 99%
“…Nowadays, thermal imaging relies primarily on bulk epitaxial semiconductor materials. In mid-wave infrared (MWIR, 3-5 µm) and long-wave infrared (LWIR, 8-12 µm), it is dominated by narrow bandgap semiconductor material such as InSb [18], HgCgTe [19,20], quantum-wells [21] and type-II superlattices [22,23]. However, these materials were typically prepared by molecular beam epitaxy or chemical vapor deposition, which leads to high fabrication and processing costs.…”
Section: Synthesis Of Infrared Cqdsmentioning
confidence: 99%
“…This phenomenon has been already observed on p-on-n architecture. 6 This is due to the fact that the diffusion length (capability to the electronic charge to diffuse into HgCdTe material) decreases strongly at low temperature. The consequence of this is a decrease of the fill factor of the photodiode and so a decrease of the photoresponse.…”
Section: Resultsmentioning
confidence: 99%
“…Very recently in 2015, several points have been added to this curve (represented by four colored diamond symbols in Figure 9) for extremely long cutoff wavelength (between 15.5µm and up to 17.3µm at 78K). The mid response cutoffs measured on such diodes perfectly follows the expected Hansen's law [ 14 ] down to 50K, giving values ranging from 17.5µm up to 19.7µm at 50K, with a classical wideband uniform spectral QE, from MWIR to LWIR and VLWIR [ 17 ], corresponding to cadmium composition below 0.2 (0.1957 to 01917).…”
Section: Figure 6 : Arrhenius Plot With Dark Current Data For Mwir-lwmentioning
confidence: 94%
“…Using a given a given set of geometries (diodes with diameter ranging between 120µm to 10µm), the general principle is to search a lateral collection length consistent with a photonic current density independent on the diode diameter. This method is in fact an efficient way to estimate this diffusion length Ld at different temperatures [ 15 ]. Figure 8 shows the evolution of the estimated Ld as function of the temperature.…”
Section: Figure 6 : Arrhenius Plot With Dark Current Data For Mwir-lwmentioning
confidence: 99%