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Dependence of the Performance of Single Photon Avalanche Diodes on the Multiplication Region Width
The dependence of the performance of separate-absorption-multiplication (SAM) single-photon avalanche diodes (SPADs) on the width of the multiplication region is theoretically investigated. The theory is applied to SAM SPADs with InP homojunction multiplication regions and InAlAs-InP heterojunction...
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Published in: | IEEE journal of quantum electronics 2008-12, Vol.44 (12), p.1188-1195 |
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container_title | IEEE journal of quantum electronics |
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creator | Ramirez, D.A. Hayat, M.M. Itzler, M.A. |
description | The dependence of the performance of separate-absorption-multiplication (SAM) single-photon avalanche diodes (SPADs) on the width of the multiplication region is theoretically investigated. The theory is applied to SAM SPADs with InP homojunction multiplication regions and InAlAs-InP heterojunction multiplication regions. In both cases the absorber layer is InGaAs. Two scenarios for the dark counts are considered: (i) low-temperature operation, when the number of dark carriers is dominated by field-assisted mechanisms of band-to-band tunneling and tunneling through defects; and (ii) room-temperature operation, when the number of dark carriers in the multiplication region is dominated by the generation/recombination mechanism. The analysis utilizes a generalized theory for breakdown probability, which takes into account the random locations where dark and photogenerated carriers are produced in each layer. Depending upon the detector temperature, as the width of the multiplication region is increased the effects from the reduction in the number of dark carriers due to field-assisted generation mechanisms are counteracted by the effects from the elevation in the number of generation/recombination dark carriers. Thus, there exists an optimal width of the multiplication region that achieves the best performance of the SPAD. |
doi_str_mv | 10.1109/JQE.2008.2003140 |
format | article |
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The theory is applied to SAM SPADs with InP homojunction multiplication regions and InAlAs-InP heterojunction multiplication regions. In both cases the absorber layer is InGaAs. Two scenarios for the dark counts are considered: (i) low-temperature operation, when the number of dark carriers is dominated by field-assisted mechanisms of band-to-band tunneling and tunneling through defects; and (ii) room-temperature operation, when the number of dark carriers in the multiplication region is dominated by the generation/recombination mechanism. The analysis utilizes a generalized theory for breakdown probability, which takes into account the random locations where dark and photogenerated carriers are produced in each layer. Depending upon the detector temperature, as the width of the multiplication region is increased the effects from the reduction in the number of dark carriers due to field-assisted generation mechanisms are counteracted by the effects from the elevation in the number of generation/recombination dark carriers. Thus, there exists an optimal width of the multiplication region that achieves the best performance of the SPAD.</description><identifier>ISSN: 0018-9197</identifier><identifier>EISSN: 1558-1713</identifier><identifier>DOI: 10.1109/JQE.2008.2003140</identifier><identifier>CODEN: IEJQA7</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Avalanche breakdown ; Avalanche photodiodes ; Avalanche photodiodes (APDs) ; breakdown probability ; dark count rate ; dead space ; Dependence ; detection efficiency ; Detectors ; Diodes ; Electric breakdown ; Geiger mode ; heterostructure APDs ; III-V semiconductor materials ; impact ionization ; Laser modes ; Radiative recombination ; Silicon ; single-photon detection ; Tunneling</subject><ispartof>IEEE journal of quantum electronics, 2008-12, Vol.44 (12), p.1188-1195</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2008</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c398t-1d079543051f00504c77c3e8dfb7ff8f66099aca5ce54266acae08835e0cffd13</citedby><cites>FETCH-LOGICAL-c398t-1d079543051f00504c77c3e8dfb7ff8f66099aca5ce54266acae08835e0cffd13</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/4675825$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,27922,27923,54794</link.rule.ids></links><search><creatorcontrib>Ramirez, D.A.</creatorcontrib><creatorcontrib>Hayat, M.M.</creatorcontrib><creatorcontrib>Itzler, M.A.</creatorcontrib><title>Dependence of the Performance of Single Photon Avalanche Diodes on the Multiplication Region Width</title><title>IEEE journal of quantum electronics</title><addtitle>JQE</addtitle><description>The dependence of the performance of separate-absorption-multiplication (SAM) single-photon avalanche diodes (SPADs) on the width of the multiplication region is theoretically investigated. The theory is applied to SAM SPADs with InP homojunction multiplication regions and InAlAs-InP heterojunction multiplication regions. In both cases the absorber layer is InGaAs. Two scenarios for the dark counts are considered: (i) low-temperature operation, when the number of dark carriers is dominated by field-assisted mechanisms of band-to-band tunneling and tunneling through defects; and (ii) room-temperature operation, when the number of dark carriers in the multiplication region is dominated by the generation/recombination mechanism. The analysis utilizes a generalized theory for breakdown probability, which takes into account the random locations where dark and photogenerated carriers are produced in each layer. Depending upon the detector temperature, as the width of the multiplication region is increased the effects from the reduction in the number of dark carriers due to field-assisted generation mechanisms are counteracted by the effects from the elevation in the number of generation/recombination dark carriers. Thus, there exists an optimal width of the multiplication region that achieves the best performance of the SPAD.</description><subject>Avalanche breakdown</subject><subject>Avalanche photodiodes</subject><subject>Avalanche photodiodes (APDs)</subject><subject>breakdown probability</subject><subject>dark count rate</subject><subject>dead space</subject><subject>Dependence</subject><subject>detection efficiency</subject><subject>Detectors</subject><subject>Diodes</subject><subject>Electric breakdown</subject><subject>Geiger mode</subject><subject>heterostructure APDs</subject><subject>III-V semiconductor materials</subject><subject>impact ionization</subject><subject>Laser modes</subject><subject>Radiative recombination</subject><subject>Silicon</subject><subject>single-photon detection</subject><subject>Tunneling</subject><issn>0018-9197</issn><issn>1558-1713</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2008</creationdate><recordtype>article</recordtype><recordid>eNo9UMtOwzAQtBBIlMIdiUvEPWUdx4lzrNryUhFvcbRSZ926SuPgOEj8PY5acdnZnZ3ZlYaQSwoTSqG4eXxdTBIAMRRGUzgiI8q5iGlO2TEZAVARF7TIT8lZ123DmKYCRmQ1xxabChuFkdWR32D0gk5btysP1Ltp1nVgN9bbJpr-lHXYBNnc2Aq7KHCD6amvvWlro0pvAvWG6wG-TOU35-REl3WHFwcck8_bxcfsPl4-3z3MpstYsUL4mFaQFzxlwKkG4JCqPFcMRaVXudZCZxkURalKrpCnSZaFFkEIxhGU1hVlY3K9v9s6-91j5-XW9q4JL6XIkoQCZIMI9iLlbNc51LJ1Zle6X0lBDkHKEKQcgpSHIIPlam8xiPgvT7Oci4SzPyfDbsY</recordid><startdate>20081201</startdate><enddate>20081201</enddate><creator>Ramirez, D.A.</creator><creator>Hayat, M.M.</creator><creator>Itzler, M.A.</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</general><scope>97E</scope><scope>RIA</scope><scope>RIE</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>20081201</creationdate><title>Dependence of the Performance of Single Photon Avalanche Diodes on the Multiplication Region Width</title><author>Ramirez, D.A. ; Hayat, M.M. ; Itzler, M.A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c398t-1d079543051f00504c77c3e8dfb7ff8f66099aca5ce54266acae08835e0cffd13</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2008</creationdate><topic>Avalanche breakdown</topic><topic>Avalanche photodiodes</topic><topic>Avalanche photodiodes (APDs)</topic><topic>breakdown probability</topic><topic>dark count rate</topic><topic>dead space</topic><topic>Dependence</topic><topic>detection efficiency</topic><topic>Detectors</topic><topic>Diodes</topic><topic>Electric breakdown</topic><topic>Geiger mode</topic><topic>heterostructure APDs</topic><topic>III-V semiconductor materials</topic><topic>impact ionization</topic><topic>Laser modes</topic><topic>Radiative recombination</topic><topic>Silicon</topic><topic>single-photon detection</topic><topic>Tunneling</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ramirez, D.A.</creatorcontrib><creatorcontrib>Hayat, M.M.</creatorcontrib><creatorcontrib>Itzler, M.A.</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><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>IEEE journal of quantum electronics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ramirez, D.A.</au><au>Hayat, M.M.</au><au>Itzler, M.A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Dependence of the Performance of Single Photon Avalanche Diodes on the Multiplication Region Width</atitle><jtitle>IEEE journal of quantum electronics</jtitle><stitle>JQE</stitle><date>2008-12-01</date><risdate>2008</risdate><volume>44</volume><issue>12</issue><spage>1188</spage><epage>1195</epage><pages>1188-1195</pages><issn>0018-9197</issn><eissn>1558-1713</eissn><coden>IEJQA7</coden><abstract>The dependence of the performance of separate-absorption-multiplication (SAM) single-photon avalanche diodes (SPADs) on the width of the multiplication region is theoretically investigated. The theory is applied to SAM SPADs with InP homojunction multiplication regions and InAlAs-InP heterojunction multiplication regions. In both cases the absorber layer is InGaAs. Two scenarios for the dark counts are considered: (i) low-temperature operation, when the number of dark carriers is dominated by field-assisted mechanisms of band-to-band tunneling and tunneling through defects; and (ii) room-temperature operation, when the number of dark carriers in the multiplication region is dominated by the generation/recombination mechanism. The analysis utilizes a generalized theory for breakdown probability, which takes into account the random locations where dark and photogenerated carriers are produced in each layer. Depending upon the detector temperature, as the width of the multiplication region is increased the effects from the reduction in the number of dark carriers due to field-assisted generation mechanisms are counteracted by the effects from the elevation in the number of generation/recombination dark carriers. Thus, there exists an optimal width of the multiplication region that achieves the best performance of the SPAD.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/JQE.2008.2003140</doi><tpages>8</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Avalanche breakdown Avalanche photodiodes Avalanche photodiodes (APDs) breakdown probability dark count rate dead space Dependence detection efficiency Detectors Diodes Electric breakdown Geiger mode heterostructure APDs III-V semiconductor materials impact ionization Laser modes Radiative recombination Silicon single-photon detection Tunneling |
title | Dependence of the Performance of Single Photon Avalanche Diodes on the Multiplication Region Width |
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