Subthreshold Operation of Photodiode-Gated Transistors Enabling High-Gain Optical Sensing and Imaging Applications
In optical sensors and imagers, high gain that leads to high sensitivity and high signal to noise ratio (SNR) is often desirable. One popular approach is avalanche photomultiplication initiated by impact ionization in an avalanche photodiode or similar devices and the other approach is active pixel...
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Veröffentlicht in: | IEEE journal of the Electron Devices Society 2020, Vol.8, p.1236-1241 |
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creator | Wang, Kai Qi, Yihong Hu, Yunfeng Xu, Yangbing Xu, Yitong Liu, Jinming Zhou, Xianda |
description | In optical sensors and imagers, high gain that leads to high sensitivity and high signal to noise ratio (SNR) is often desirable. One popular approach is avalanche photomultiplication initiated by impact ionization in an avalanche photodiode or similar devices and the other approach is active pixel sensor (APS) with in-pixel amplifier. However, the former requires high electric field which induces high shot noise and the latter needs a multiple-transistor pixel circuit which compromises the fill factor and consequently, reduces the SNR. This work proposes and summarizes our recent efforts taken to achieve high gain optical sensors through subthreshold operation of photodiode-gated transistors. |
doi_str_mv | 10.1109/JEDS.2020.3022711 |
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One popular approach is avalanche photomultiplication initiated by impact ionization in an avalanche photodiode or similar devices and the other approach is active pixel sensor (APS) with in-pixel amplifier. However, the former requires high electric field which induces high shot noise and the latter needs a multiple-transistor pixel circuit which compromises the fill factor and consequently, reduces the SNR. 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This work proposes and summarizes our recent efforts taken to achieve high gain optical sensors through subthreshold operation of photodiode-gated transistors.</description><subject>active pixel sensor</subject><subject>Active pixel sensors</subject><subject>Avalanche diodes</subject><subject>Circuits</subject><subject>Electric fields</subject><subject>High gain</subject><subject>Logic gates</subject><subject>MOSFET</subject><subject>Optical measuring instruments</subject><subject>Optical sensors</subject><subject>Photoconductivity</subject><subject>photodiode-gated transistors</subject><subject>Photodiodes</subject><subject>Pixels</subject><subject>Semiconductor devices</subject><subject>Sensors</subject><subject>Shot noise</subject><subject>Signal to noise ratio</subject><subject>subthreshold operation</subject><subject>Thin film transistors</subject><subject>Threshold voltage</subject><subject>Transistors</subject><issn>2168-6734</issn><issn>2168-6734</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><sourceid>ESBDL</sourceid><sourceid>RIE</sourceid><sourceid>DOA</sourceid><recordid>eNpNUUtLxDAQLqLgovsDxEvBc9c82jQ5LrrqiqCw6zmkybTNUpuadA_-e1MrYg7JMN9jhnxJcoXRCmMkbp8397sVQQStKCKkxPgkWRDMeMZKmp_-q8-TZQgHFA_HTDC2SPzuWI2th9C6zqSvA3g1Wtenrk7fWjc6Y52B7FGNYNK9V32wYXQ-pJteVZ3tm_TJNm3EbR_Fo9WqS3cQWRFRvUm3H6qZ6vUwdBGcrMNlclarLsDy971I3h82-7un7OX1cXu3fsl0jsiYcYQKJiqtoTJ1zjTPRUVLVnHAnBWaaKCUYyBQYEaMEAxrwgxVSBgg8aIXyXb2NU4d5ODth_Jf0ikrfxrON1L5uHIHEkrKOFaq0kWR8xJzQKzWolCmiv9bs-h1M3sN3n0eIYzy4I6-j-tLkheliPocRRaeWdq7EDzUf1MxklNSckpKTknJ36Si5nrWWAD44wvMS0E5_Qa0fo9F</recordid><startdate>2020</startdate><enddate>2020</enddate><creator>Wang, Kai</creator><creator>Qi, Yihong</creator><creator>Hu, Yunfeng</creator><creator>Xu, Yangbing</creator><creator>Xu, Yitong</creator><creator>Liu, Jinming</creator><creator>Zhou, Xianda</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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One popular approach is avalanche photomultiplication initiated by impact ionization in an avalanche photodiode or similar devices and the other approach is active pixel sensor (APS) with in-pixel amplifier. However, the former requires high electric field which induces high shot noise and the latter needs a multiple-transistor pixel circuit which compromises the fill factor and consequently, reduces the SNR. This work proposes and summarizes our recent efforts taken to achieve high gain optical sensors through subthreshold operation of photodiode-gated transistors.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/JEDS.2020.3022711</doi><tpages>6</tpages><orcidid>https://orcid.org/0000-0001-9702-6642</orcidid><orcidid>https://orcid.org/0000-0003-2006-5760</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | active pixel sensor Active pixel sensors Avalanche diodes Circuits Electric fields High gain Logic gates MOSFET Optical measuring instruments Optical sensors Photoconductivity photodiode-gated transistors Photodiodes Pixels Semiconductor devices Sensors Shot noise Signal to noise ratio subthreshold operation Thin film transistors Threshold voltage Transistors |
title | Subthreshold Operation of Photodiode-Gated Transistors Enabling High-Gain Optical Sensing and Imaging Applications |
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