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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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. Microelectronics. Optoelectronics. Solid state devices</subject><ispartof>Journal of electronic materials, 2003-07, Vol.32 (7), p.803-809</ispartof><rights>2003 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c335t-b0862a3d81a7f5c33005938af39b042835d5a2f3a4eea9f78fbba6dc328b38c33</citedby><cites>FETCH-LOGICAL-c335t-b0862a3d81a7f5c33005938af39b042835d5a2f3a4eea9f78fbba6dc328b38c33</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>309,310,314,776,780,785,786,23910,23911,25119,27903,27904</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=15015615$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>ZANDIAN, Majid</creatorcontrib><creatorcontrib>GARNETT, J. D</creatorcontrib><creatorcontrib>ARIAS, J. M</creatorcontrib><creatorcontrib>VURAL, K</creatorcontrib><creatorcontrib>HALL, Donald N. B</creatorcontrib><creatorcontrib>DEWAMES, R. E</creatorcontrib><creatorcontrib>CARMODY, M</creatorcontrib><creatorcontrib>PASKO, J. G</creatorcontrib><creatorcontrib>FARRIS, M</creatorcontrib><creatorcontrib>CABELLI, C. A</creatorcontrib><creatorcontrib>COOPER, D. E</creatorcontrib><creatorcontrib>HILDEBRANDT, G</creatorcontrib><creatorcontrib>CHOW, J</creatorcontrib><title>Mid-wavelength infrared p-on-n Hg1-xCdxTe heterostructure detectors: 30-120 kelvin state-of-the-art performance</title><title>Journal of electronic materials</title><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><subject>Applied sciences</subject><subject>Bolometer; infrared, submillimeter wave, microwave and radiowave receivers and detectors</subject><subject>Electronics</subject><subject>Exact sciences and technology</subject><subject>Infrared, submillimeter wave, microwave and radiowave instruments, equipment and techniques</subject><subject>Instruments, apparatus, components and techniques common to several branches of physics and astronomy</subject><subject>Microelectronic fabrication (materials and surfaces technology)</subject><subject>Optoelectronic devices</subject><subject>Physics</subject><subject>Semiconductor electronics. Microelectronics. Optoelectronics. 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Solid state devices</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>ZANDIAN, Majid</creatorcontrib><creatorcontrib>GARNETT, J. D</creatorcontrib><creatorcontrib>ARIAS, J. M</creatorcontrib><creatorcontrib>VURAL, K</creatorcontrib><creatorcontrib>HALL, Donald N. B</creatorcontrib><creatorcontrib>DEWAMES, R. E</creatorcontrib><creatorcontrib>CARMODY, M</creatorcontrib><creatorcontrib>PASKO, J. G</creatorcontrib><creatorcontrib>FARRIS, M</creatorcontrib><creatorcontrib>CABELLI, C. A</creatorcontrib><creatorcontrib>COOPER, D. 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E</au><au>HILDEBRANDT, G</au><au>CHOW, J</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Mid-wavelength infrared p-on-n Hg1-xCdxTe heterostructure detectors: 30-120 kelvin state-of-the-art performance</atitle><jtitle>Journal of electronic materials</jtitle><date>2003-07-01</date><risdate>2003</risdate><volume>32</volume><issue>7</issue><spage>803</spage><epage>809</epage><pages>803-809</pages><issn>0361-5235</issn><eissn>1543-186X</eissn><coden>JECMA5</coden><abstract>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.</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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