Mid-wavelength infrared p-on-n Hg1-xCdxTe heterostructure detectors: 30-120 kelvin state-of-the-art performance

Authors report on Hg1-xCdxTe mid-wavelength ir (MWIR) detectors grown by MBE on CdZnTe substrates. I-V characteristics of HgCdTe-MWIR devices and temperature dependence of focal-plane array (FPA) dark current have been investigated and compared with the most recent InSb published data. These MWIR p-...

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Veröffentlicht in:Journal of electronic materials 2003-07, Vol.32 (7), p.803-809
Hauptverfasser: ZANDIAN, Majid, GARNETT, J. D, ARIAS, J. M, VURAL, K, HALL, Donald N. B, DEWAMES, R. E, CARMODY, M, PASKO, J. G, FARRIS, M, CABELLI, C. A, COOPER, D. E, HILDEBRANDT, G, CHOW, J
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container_end_page 809
container_issue 7
container_start_page 803
container_title Journal of electronic materials
container_volume 32
creator ZANDIAN, Majid
GARNETT, J. D
ARIAS, J. M
VURAL, K
HALL, Donald N. B
DEWAMES, R. E
CARMODY, M
PASKO, J. G
FARRIS, M
CABELLI, C. A
COOPER, D. E
HILDEBRANDT, G
CHOW, J
description Authors report on Hg1-xCdxTe mid-wavelength ir (MWIR) detectors grown by MBE on CdZnTe substrates. I-V characteristics of HgCdTe-MWIR devices and temperature dependence of focal-plane array (FPA) dark current have been investigated and compared with the most recent InSb published data. These MWIR p-on-n Hg1-xCdxTe/CdZnTe heterostructure detectors give outstanding performance, and at 68 K, they are limited by diffusion currents. For temperatures lower than 68 K, in the near small-bias region, another current is dominant. This current has lower sensitivity to temperature and most likely is of tunneling origin. High-performance MWIR devices and arrays were fabricated with median RoA values of 3.96 x 1010 OMEGA-cm2 at 78 K and 1.27 x 1012 OMEGA-cm2 at 60 K; the quantum efficiency (QE) without an antireflection (AR) coating was 73% for a cutoff wavelength of 5.3 mum at 78 K. The QE measurement was performed with a narrow pass filter centered at 3.5 mum. Many large-format MWIR 1024 x 1024 FPAs were fabricated and tested as a function of temperature to confirm the ultra-low dark currents observed in individual devices. The 1024 x 1024 array operability and AR-coated QE at 78 K were 99.48% and 88.3%, resp. A comparison of these results with the state-of-the-art InSb-detector data suggests MWIR-HgCdTe devices have significantly higher performance in the 30-120 K temperature range. The InSb detectors are dominated by generation-recombination currents in the 60-120 K temperature range because of a defect center in the energy gap, whereas MWIR-HgCdTe detectors do not exhibit G-R-type currents in this temperature range and are limited by diffusion currents. 9 refs.
doi_str_mv 10.1007/s11664-003-0074-6
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D ; ARIAS, J. M ; VURAL, K ; HALL, Donald N. B ; DEWAMES, R. E ; CARMODY, M ; PASKO, J. G ; FARRIS, M ; CABELLI, C. A ; COOPER, D. E ; HILDEBRANDT, G ; CHOW, J</creator><creatorcontrib>ZANDIAN, Majid ; GARNETT, J. D ; ARIAS, J. M ; VURAL, K ; HALL, Donald N. B ; DEWAMES, R. E ; CARMODY, M ; PASKO, J. G ; FARRIS, M ; CABELLI, C. A ; COOPER, D. E ; HILDEBRANDT, G ; CHOW, J</creatorcontrib><description>Authors report on Hg1-xCdxTe mid-wavelength ir (MWIR) detectors grown by MBE on CdZnTe substrates. I-V characteristics of HgCdTe-MWIR devices and temperature dependence of focal-plane array (FPA) dark current have been investigated and compared with the most recent InSb published data. These MWIR p-on-n Hg1-xCdxTe/CdZnTe heterostructure detectors give outstanding performance, and at 68 K, they are limited by diffusion currents. For temperatures lower than 68 K, in the near small-bias region, another current is dominant. This current has lower sensitivity to temperature and most likely is of tunneling origin. High-performance MWIR devices and arrays were fabricated with median RoA values of 3.96 x 1010 OMEGA-cm2 at 78 K and 1.27 x 1012 OMEGA-cm2 at 60 K; the quantum efficiency (QE) without an antireflection (AR) coating was 73% for a cutoff wavelength of 5.3 mum at 78 K. The QE measurement was performed with a narrow pass filter centered at 3.5 mum. Many large-format MWIR 1024 x 1024 FPAs were fabricated and tested as a function of temperature to confirm the ultra-low dark currents observed in individual devices. The 1024 x 1024 array operability and AR-coated QE at 78 K were 99.48% and 88.3%, resp. A comparison of these results with the state-of-the-art InSb-detector data suggests MWIR-HgCdTe devices have significantly higher performance in the 30-120 K temperature range. The InSb detectors are dominated by generation-recombination currents in the 60-120 K temperature range because of a defect center in the energy gap, whereas MWIR-HgCdTe detectors do not exhibit G-R-type currents in this temperature range and are limited by diffusion currents. 9 refs.</description><identifier>ISSN: 0361-5235</identifier><identifier>EISSN: 1543-186X</identifier><identifier>DOI: 10.1007/s11664-003-0074-6</identifier><identifier>CODEN: JECMA5</identifier><language>eng</language><publisher>New York, NY: Institute of Electrical and Electronics Engineers</publisher><subject>Applied sciences ; Bolometer; infrared, submillimeter wave, microwave and radiowave receivers and detectors ; Electronics ; Exact sciences and technology ; Infrared, submillimeter wave, microwave and radiowave instruments, equipment and techniques ; Instruments, apparatus, components and techniques common to several branches of physics and astronomy ; Microelectronic fabrication (materials and surfaces technology) ; Optoelectronic devices ; Physics ; Semiconductor electronics. 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For temperatures lower than 68 K, in the near small-bias region, another current is dominant. This current has lower sensitivity to temperature and most likely is of tunneling origin. High-performance MWIR devices and arrays were fabricated with median RoA values of 3.96 x 1010 OMEGA-cm2 at 78 K and 1.27 x 1012 OMEGA-cm2 at 60 K; the quantum efficiency (QE) without an antireflection (AR) coating was 73% for a cutoff wavelength of 5.3 mum at 78 K. The QE measurement was performed with a narrow pass filter centered at 3.5 mum. Many large-format MWIR 1024 x 1024 FPAs were fabricated and tested as a function of temperature to confirm the ultra-low dark currents observed in individual devices. The 1024 x 1024 array operability and AR-coated QE at 78 K were 99.48% and 88.3%, resp. A comparison of these results with the state-of-the-art InSb-detector data suggests MWIR-HgCdTe devices have significantly higher performance in the 30-120 K temperature range. The InSb detectors are dominated by generation-recombination currents in the 60-120 K temperature range because of a defect center in the energy gap, whereas MWIR-HgCdTe detectors do not exhibit G-R-type currents in this temperature range and are limited by diffusion currents. 9 refs.</abstract><cop>New York, NY</cop><pub>Institute of Electrical and Electronics Engineers</pub><doi>10.1007/s11664-003-0074-6</doi><tpages>7</tpages></addata></record>
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subjects Applied sciences
Bolometer
infrared, submillimeter wave, microwave and radiowave receivers and detectors
Electronics
Exact sciences and technology
Infrared, submillimeter wave, microwave and radiowave instruments, equipment and techniques
Instruments, apparatus, components and techniques common to several branches of physics and astronomy
Microelectronic fabrication (materials and surfaces technology)
Optoelectronic devices
Physics
Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices
title Mid-wavelength infrared p-on-n Hg1-xCdxTe heterostructure detectors: 30-120 kelvin state-of-the-art performance
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