Negative luminescence from large-area HgCdTe photodiode arrays with 4.8-6.0-/spl mu/m cutoff wavelengths
We demonstrate the substantial suppression of infrared (IR) blackbody emission from HgCdTe photodiode arrays with cutoff wavelengths of 4.8, 5.5, and 6.0 /spl mu/m. At room temperature, a reverse bias induces internal negative luminescence (NL) efficiencies of 95%, 93%, and 88%, respectively, which...
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Veröffentlicht in: | IEEE journal of quantum electronics 2005-02, Vol.41 (2), p.227-233 |
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creator | Lindle, J.R. Bewley, W.W. Vurgaftman, I. Chul Soo Kim Meyer, J.R. Johnson, J.L. Thomas, M.L. Piquette, E.C. Tennant, W.E. |
description | We demonstrate the substantial suppression of infrared (IR) blackbody emission from HgCdTe photodiode arrays with cutoff wavelengths of 4.8, 5.5, and 6.0 /spl mu/m. At room temperature, a reverse bias induces internal negative luminescence (NL) efficiencies of 95%, 93%, and 88%, respectively, which correspond to apparent cooling of the surface temperatures by 60, 59, and 49 K. Reverse-bias saturation current densities for the three devices were 0.11, 0.7, and 32 A/cm/sup 2/. Measurement and analysis of the material transmission characteristics indicate that the small residual inefficiencies may be limited by a parasitic absorption process. The 4.8 and 5.5 /spl mu/m photodiodes were fabricated into 18 /spl times/ 2 arrays with total areas of 5 mm /spl times/ 5 mm. In both cases, all 36 array elements were fully operable, and had similar electrical and NL properties. Effective fill factors were /spl ap/100%, since carrier diffusion led to the extraction of carriers from regions between the elements. These results show that efficient, low-power NL devices with active areas in the square-inch range are now feasible for such applications as the cold shielding of infrared focal-plane arrays. |
doi_str_mv | 10.1109/JQE.2004.839721 |
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At room temperature, a reverse bias induces internal negative luminescence (NL) efficiencies of 95%, 93%, and 88%, respectively, which correspond to apparent cooling of the surface temperatures by 60, 59, and 49 K. Reverse-bias saturation current densities for the three devices were 0.11, 0.7, and 32 A/cm/sup 2/. Measurement and analysis of the material transmission characteristics indicate that the small residual inefficiencies may be limited by a parasitic absorption process. The 4.8 and 5.5 /spl mu/m photodiodes were fabricated into 18 /spl times/ 2 arrays with total areas of 5 mm /spl times/ 5 mm. In both cases, all 36 array elements were fully operable, and had similar electrical and NL properties. Effective fill factors were /spl ap/100%, since carrier diffusion led to the extraction of carriers from regions between the elements. These results show that efficient, low-power NL devices with active areas in the square-inch range are now feasible for such applications as the cold shielding of infrared focal-plane arrays.</description><identifier>ISSN: 0018-9197</identifier><identifier>EISSN: 1558-1713</identifier><identifier>DOI: 10.1109/JQE.2004.839721</identifier><identifier>CODEN: IEJQA7</identifier><language>eng</language><publisher>IEEE</publisher><subject>Absorption ; Charge carrier processes ; Cooling ; Current density ; Infrared (IR) light-emitting diode ; Light emitting diodes ; Luminescence ; midwave IR photodiode ; negative luminescence (NL) ; Photodiodes ; Semiconductor diodes ; Temperature</subject><ispartof>IEEE journal of quantum electronics, 2005-02, Vol.41 (2), p.227-233</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c1060-324dfe2a01e748712ca7acad3f7590049de0ef0006c022fb661d5d80952646aa3</citedby><cites>FETCH-LOGICAL-c1060-324dfe2a01e748712ca7acad3f7590049de0ef0006c022fb661d5d80952646aa3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/1386480$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,796,27923,27924,54757</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/1386480$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Lindle, J.R.</creatorcontrib><creatorcontrib>Bewley, W.W.</creatorcontrib><creatorcontrib>Vurgaftman, I.</creatorcontrib><creatorcontrib>Chul Soo Kim</creatorcontrib><creatorcontrib>Meyer, J.R.</creatorcontrib><creatorcontrib>Johnson, J.L.</creatorcontrib><creatorcontrib>Thomas, M.L.</creatorcontrib><creatorcontrib>Piquette, E.C.</creatorcontrib><creatorcontrib>Tennant, W.E.</creatorcontrib><title>Negative luminescence from large-area HgCdTe photodiode arrays with 4.8-6.0-/spl mu/m cutoff wavelengths</title><title>IEEE journal of quantum electronics</title><addtitle>JQE</addtitle><description>We demonstrate the substantial suppression of infrared (IR) blackbody emission from HgCdTe photodiode arrays with cutoff wavelengths of 4.8, 5.5, and 6.0 /spl mu/m. At room temperature, a reverse bias induces internal negative luminescence (NL) efficiencies of 95%, 93%, and 88%, respectively, which correspond to apparent cooling of the surface temperatures by 60, 59, and 49 K. Reverse-bias saturation current densities for the three devices were 0.11, 0.7, and 32 A/cm/sup 2/. Measurement and analysis of the material transmission characteristics indicate that the small residual inefficiencies may be limited by a parasitic absorption process. The 4.8 and 5.5 /spl mu/m photodiodes were fabricated into 18 /spl times/ 2 arrays with total areas of 5 mm /spl times/ 5 mm. In both cases, all 36 array elements were fully operable, and had similar electrical and NL properties. Effective fill factors were /spl ap/100%, since carrier diffusion led to the extraction of carriers from regions between the elements. These results show that efficient, low-power NL devices with active areas in the square-inch range are now feasible for such applications as the cold shielding of infrared focal-plane arrays.</description><subject>Absorption</subject><subject>Charge carrier processes</subject><subject>Cooling</subject><subject>Current density</subject><subject>Infrared (IR) light-emitting diode</subject><subject>Light emitting diodes</subject><subject>Luminescence</subject><subject>midwave IR photodiode</subject><subject>negative luminescence (NL)</subject><subject>Photodiodes</subject><subject>Semiconductor diodes</subject><subject>Temperature</subject><issn>0018-9197</issn><issn>1558-1713</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNpF0FFLwzAQB_AgCs7psw--5AukvaRt2j7KmE4ZijCfy5lc2kq7jqTb8NvbMcGn4-D-d9yPsXsJkZRQxq8fy0gBpFGRlLmSF2wms6wQMpfJJZsByEKUssyv2U0I31ObpgXMWPNGNY7tgXi379stBUNbQ9z5oecd-poEekK-qhd2Q3zXDONg28ESR-_xJ_BjOzZ8uil0BCIOu473-7jnZj8OzvEjHqijbT024ZZdOewC3f3VOft8Wm4WK7F-f35ZPK6FkaBBJCq1jhSCpDwtcqkM5mjQJi7Pyum70hKQAwBtQCn3pbW0mS2gzJRONWIyZ_F5r_FDCJ5ctfNtj_6nklCdoKoJqjpBVWeoKfFwTrRE9D-dFHoSSn4BE01jqA</recordid><startdate>200502</startdate><enddate>200502</enddate><creator>Lindle, J.R.</creator><creator>Bewley, W.W.</creator><creator>Vurgaftman, I.</creator><creator>Chul Soo Kim</creator><creator>Meyer, J.R.</creator><creator>Johnson, J.L.</creator><creator>Thomas, M.L.</creator><creator>Piquette, E.C.</creator><creator>Tennant, W.E.</creator><general>IEEE</general><scope>97E</scope><scope>RIA</scope><scope>RIE</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>200502</creationdate><title>Negative luminescence from large-area HgCdTe photodiode arrays with 4.8-6.0-/spl mu/m cutoff wavelengths</title><author>Lindle, J.R. ; Bewley, W.W. ; Vurgaftman, I. ; Chul Soo Kim ; Meyer, J.R. ; Johnson, J.L. ; Thomas, M.L. ; Piquette, E.C. ; Tennant, W.E.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c1060-324dfe2a01e748712ca7acad3f7590049de0ef0006c022fb661d5d80952646aa3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2005</creationdate><topic>Absorption</topic><topic>Charge carrier processes</topic><topic>Cooling</topic><topic>Current density</topic><topic>Infrared (IR) light-emitting diode</topic><topic>Light emitting diodes</topic><topic>Luminescence</topic><topic>midwave IR photodiode</topic><topic>negative luminescence (NL)</topic><topic>Photodiodes</topic><topic>Semiconductor diodes</topic><topic>Temperature</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Lindle, J.R.</creatorcontrib><creatorcontrib>Bewley, W.W.</creatorcontrib><creatorcontrib>Vurgaftman, I.</creatorcontrib><creatorcontrib>Chul Soo Kim</creatorcontrib><creatorcontrib>Meyer, J.R.</creatorcontrib><creatorcontrib>Johnson, J.L.</creatorcontrib><creatorcontrib>Thomas, M.L.</creatorcontrib><creatorcontrib>Piquette, E.C.</creatorcontrib><creatorcontrib>Tennant, W.E.</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 2005-present</collection><collection>IEEE All-Society Periodicals Package (ASPP) 1998-Present</collection><collection>IEEE Electronic Library (IEL)</collection><collection>CrossRef</collection><jtitle>IEEE journal of quantum electronics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Lindle, J.R.</au><au>Bewley, W.W.</au><au>Vurgaftman, I.</au><au>Chul Soo Kim</au><au>Meyer, J.R.</au><au>Johnson, J.L.</au><au>Thomas, M.L.</au><au>Piquette, E.C.</au><au>Tennant, W.E.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Negative luminescence from large-area HgCdTe photodiode arrays with 4.8-6.0-/spl mu/m cutoff wavelengths</atitle><jtitle>IEEE journal of quantum electronics</jtitle><stitle>JQE</stitle><date>2005-02</date><risdate>2005</risdate><volume>41</volume><issue>2</issue><spage>227</spage><epage>233</epage><pages>227-233</pages><issn>0018-9197</issn><eissn>1558-1713</eissn><coden>IEJQA7</coden><abstract>We demonstrate the substantial suppression of infrared (IR) blackbody emission from HgCdTe photodiode arrays with cutoff wavelengths of 4.8, 5.5, and 6.0 /spl mu/m. At room temperature, a reverse bias induces internal negative luminescence (NL) efficiencies of 95%, 93%, and 88%, respectively, which correspond to apparent cooling of the surface temperatures by 60, 59, and 49 K. Reverse-bias saturation current densities for the three devices were 0.11, 0.7, and 32 A/cm/sup 2/. Measurement and analysis of the material transmission characteristics indicate that the small residual inefficiencies may be limited by a parasitic absorption process. The 4.8 and 5.5 /spl mu/m photodiodes were fabricated into 18 /spl times/ 2 arrays with total areas of 5 mm /spl times/ 5 mm. In both cases, all 36 array elements were fully operable, and had similar electrical and NL properties. Effective fill factors were /spl ap/100%, since carrier diffusion led to the extraction of carriers from regions between the elements. These results show that efficient, low-power NL devices with active areas in the square-inch range are now feasible for such applications as the cold shielding of infrared focal-plane arrays.</abstract><pub>IEEE</pub><doi>10.1109/JQE.2004.839721</doi><tpages>7</tpages></addata></record> |
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subjects | Absorption Charge carrier processes Cooling Current density Infrared (IR) light-emitting diode Light emitting diodes Luminescence midwave IR photodiode negative luminescence (NL) Photodiodes Semiconductor diodes Temperature |
title | Negative luminescence from large-area HgCdTe photodiode arrays with 4.8-6.0-/spl mu/m cutoff wavelengths |
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