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Nanoscale Accumulated Body Si nMOSFETs
Narrow- and short-channel inversion-mode nMOSFETs with an accumulated body are experimentally demonstrated down to {W} \times {L} = \textsf {17} -nm \times37 -nm scale. Accumulation of holes on the p-type body is achieved by applying a negative bias on an independently controlled p+ polysilicon si...
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Published in: | IEEE transactions on electron devices 2018-04, Vol.65 (4), p.1283-1289 |
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creator | Akbulut, Mustafa B. Dirisaglik, Faruk Cywar, Adam Faraclas, Azer Pence, Douglas Patel, Jyotica Steen, Steven Nunes, Ron W. Silva, Helena Gokirmak, Ali |
description | Narrow- and short-channel inversion-mode nMOSFETs with an accumulated body are experimentally demonstrated down to {W} \times {L} = \textsf {17} -nm \times37 -nm scale. Accumulation of holes on the p-type body is achieved by applying a negative bias on an independently controlled p+ polysilicon side-gate structure surrounding the FET body. Affecting the channel from two sides, electrical characteristics of the transistor can be modified, especially the threshold voltage ( {V} _{T} ). {V} _{T} sensitivity to the side-gate bias ( {V} _{\textsf {side}} ) shows a strong dependence on the device width for {W} < \textsf {40} nm, exponentially increasing to above 1 V/V for {W} = \textsf {17} nm. This sensitivity is significantly larger than what is predicted by 3-D Technology Computer Aided Design simulations. The devices exhibit very low leakage, good subthreshold slope, and improved drain-induced barrier lowering with the accumulation of the body. |
doi_str_mv | 10.1109/TED.2018.2809643 |
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Accumulation of holes on the p-type body is achieved by applying a negative bias on an independently controlled p+ polysilicon side-gate structure surrounding the FET body. Affecting the channel from two sides, electrical characteristics of the transistor can be modified, especially the threshold voltage (<inline-formula> <tex-math notation="LaTeX">{V} _{T} </tex-math></inline-formula>). <inline-formula> <tex-math notation="LaTeX">{V} _{T} </tex-math></inline-formula> sensitivity to the side-gate bias (<inline-formula> <tex-math notation="LaTeX">{V} _{\textsf {side}} </tex-math></inline-formula>) shows a strong dependence on the device width for <inline-formula> <tex-math notation="LaTeX">{W} < \textsf {40} </tex-math></inline-formula> nm, exponentially increasing to above 1 V/V for <inline-formula> <tex-math notation="LaTeX">{W} = \textsf {17} </tex-math></inline-formula> nm. This sensitivity is significantly larger than what is predicted by 3-D Technology Computer Aided Design simulations. The devices exhibit very low leakage, good subthreshold slope, and improved drain-induced barrier lowering with the accumulation of the body.]]></description><identifier>ISSN: 0018-9383</identifier><identifier>EISSN: 1557-9646</identifier><identifier>DOI: 10.1109/TED.2018.2809643</identifier><identifier>CODEN: IETDAI</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Accumulation ; Back biasing ; Bias ; CAD ; Computer aided design ; Computer simulation ; Dielectrics ; Fabrication ; FETs ; Field effect transistors ; leakage currents ; Logic gates ; MOSFET ; Semiconductor devices ; Sensitivity ; Silicon ; silicon devices ; Threshold voltage</subject><ispartof>IEEE transactions on electron devices, 2018-04, Vol.65 (4), p.1283-1289</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2018</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c333t-7806a7e0a2f9ad37ed64302d57a59f239d06f8f39ea8bb1b03cd44cd05efd0433</citedby><cites>FETCH-LOGICAL-c333t-7806a7e0a2f9ad37ed64302d57a59f239d06f8f39ea8bb1b03cd44cd05efd0433</cites><orcidid>0000-0003-4660-5980</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/8310906$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,54796</link.rule.ids></links><search><creatorcontrib>Akbulut, Mustafa B.</creatorcontrib><creatorcontrib>Dirisaglik, Faruk</creatorcontrib><creatorcontrib>Cywar, Adam</creatorcontrib><creatorcontrib>Faraclas, Azer</creatorcontrib><creatorcontrib>Pence, Douglas</creatorcontrib><creatorcontrib>Patel, Jyotica</creatorcontrib><creatorcontrib>Steen, Steven</creatorcontrib><creatorcontrib>Nunes, Ron W.</creatorcontrib><creatorcontrib>Silva, Helena</creatorcontrib><creatorcontrib>Gokirmak, Ali</creatorcontrib><title>Nanoscale Accumulated Body Si nMOSFETs</title><title>IEEE transactions on electron devices</title><addtitle>TED</addtitle><description><![CDATA[Narrow- and short-channel inversion-mode nMOSFETs with an accumulated body are experimentally demonstrated down to <inline-formula> <tex-math notation="LaTeX">{W} \times {L} = \textsf {17} </tex-math></inline-formula>-nm <inline-formula> <tex-math notation="LaTeX">\times37 </tex-math></inline-formula>-nm scale. Accumulation of holes on the p-type body is achieved by applying a negative bias on an independently controlled p+ polysilicon side-gate structure surrounding the FET body. Affecting the channel from two sides, electrical characteristics of the transistor can be modified, especially the threshold voltage (<inline-formula> <tex-math notation="LaTeX">{V} _{T} </tex-math></inline-formula>). <inline-formula> <tex-math notation="LaTeX">{V} _{T} </tex-math></inline-formula> sensitivity to the side-gate bias (<inline-formula> <tex-math notation="LaTeX">{V} _{\textsf {side}} </tex-math></inline-formula>) shows a strong dependence on the device width for <inline-formula> <tex-math notation="LaTeX">{W} < \textsf {40} </tex-math></inline-formula> nm, exponentially increasing to above 1 V/V for <inline-formula> <tex-math notation="LaTeX">{W} = \textsf {17} </tex-math></inline-formula> nm. This sensitivity is significantly larger than what is predicted by 3-D Technology Computer Aided Design simulations. The devices exhibit very low leakage, good subthreshold slope, and improved drain-induced barrier lowering with the accumulation of the body.]]></description><subject>Accumulation</subject><subject>Back biasing</subject><subject>Bias</subject><subject>CAD</subject><subject>Computer aided design</subject><subject>Computer simulation</subject><subject>Dielectrics</subject><subject>Fabrication</subject><subject>FETs</subject><subject>Field effect transistors</subject><subject>leakage currents</subject><subject>Logic gates</subject><subject>MOSFET</subject><subject>Semiconductor devices</subject><subject>Sensitivity</subject><subject>Silicon</subject><subject>silicon devices</subject><subject>Threshold voltage</subject><issn>0018-9383</issn><issn>1557-9646</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNo9kLtPwzAQxi0EEqGwI7FEQmJLOOdixx5LKQ-p0KFltlw_pFRpUuJm6H-Pq1RM9_p9d_ZHyD2FnFKQz-v5a14AFXkhQPISL0hCGauymPNLkkAcZRIFXpObELax5GVZJOTpW7ddMLpx6dSYYTc0-uBs-tLZY7qq0_ZruXqbr8MtufK6Ce7uHCfkJ7ZnH9li-f45my4yg4iHrBLAdeVAF15qi5Wz8SVQWFZpJn2B0gL3wqN0Wmw2dANobFkaC8x5CyXihDyOe_d99zu4cFDbbujbeFLFzzFKOWM0UjBSpu9C6J1X-77e6f6oKKiTGyq6cRIIdXYjSh5GSe2c-8cFRhg4_gFjdliI</recordid><startdate>20180401</startdate><enddate>20180401</enddate><creator>Akbulut, Mustafa B.</creator><creator>Dirisaglik, Faruk</creator><creator>Cywar, Adam</creator><creator>Faraclas, Azer</creator><creator>Pence, Douglas</creator><creator>Patel, Jyotica</creator><creator>Steen, Steven</creator><creator>Nunes, Ron W.</creator><creator>Silva, Helena</creator><creator>Gokirmak, Ali</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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Accumulation of holes on the p-type body is achieved by applying a negative bias on an independently controlled p+ polysilicon side-gate structure surrounding the FET body. Affecting the channel from two sides, electrical characteristics of the transistor can be modified, especially the threshold voltage (<inline-formula> <tex-math notation="LaTeX">{V} _{T} </tex-math></inline-formula>). <inline-formula> <tex-math notation="LaTeX">{V} _{T} </tex-math></inline-formula> sensitivity to the side-gate bias (<inline-formula> <tex-math notation="LaTeX">{V} _{\textsf {side}} </tex-math></inline-formula>) shows a strong dependence on the device width for <inline-formula> <tex-math notation="LaTeX">{W} < \textsf {40} </tex-math></inline-formula> nm, exponentially increasing to above 1 V/V for <inline-formula> <tex-math notation="LaTeX">{W} = \textsf {17} </tex-math></inline-formula> nm. This sensitivity is significantly larger than what is predicted by 3-D Technology Computer Aided Design simulations. The devices exhibit very low leakage, good subthreshold slope, and improved drain-induced barrier lowering with the accumulation of the body.]]></abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TED.2018.2809643</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0003-4660-5980</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Accumulation Back biasing Bias CAD Computer aided design Computer simulation Dielectrics Fabrication FETs Field effect transistors leakage currents Logic gates MOSFET Semiconductor devices Sensitivity Silicon silicon devices Threshold voltage |
title | Nanoscale Accumulated Body Si nMOSFETs |
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