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High-Speed and Low-Power Ultradeep-Submicrometer III-V Heterojunctionless Tunnel Field-Effect Transistor
Tunnel field-effect transistor (TFET) devices are gaining attention because of good scalability and they have very low leakage current. However, they suffer from low ON-current and high threshold voltage. In this paper, we present III-V heterojunctionless TFET (H-JLTFET) for circuit applications. Th...
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Published in: | IEEE transactions on electron devices 2014-02, Vol.61 (2), p.479-486 |
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creator | Asthana, Pranav Kumar Ghosh, Bahniman Goswami, Yogesh Tripathi, Ball Mukund Mani |
description | Tunnel field-effect transistor (TFET) devices are gaining attention because of good scalability and they have very low leakage current. However, they suffer from low ON-current and high threshold voltage. In this paper, we present III-V heterojunctionless TFET (H-JLTFET) for circuit applications. This paper elaborates on interfacing of III-V with group IV semiconductors for heterojunction. Implementing heterojunction and bandgap engineering, we found that devices have significantly improved performance with very high speed even at very low operating voltage. As there is no doping junction present, future scaling could be feasible along with much higher speed of charge carriers than in silicon. GaAs:Si, Si:Si0.3Ge0.7, Si:InAs, and GaAs:Ge, H-JLTFET interface for 20-nm gate length (EOT=2 nm) and dielectric, HfO2 at VGS=1 V and temperature of 300 K have ION of 0.02-12.5 mA/μm, ION/IOFF of 10 5 -10 12 , and subthreshold swing (average) of 16-74 mV/decade. |
doi_str_mv | 10.1109/TED.2013.2295238 |
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However, they suffer from low ON-current and high threshold voltage. In this paper, we present III-V heterojunctionless TFET (H-JLTFET) for circuit applications. This paper elaborates on interfacing of III-V with group IV semiconductors for heterojunction. Implementing heterojunction and bandgap engineering, we found that devices have significantly improved performance with very high speed even at very low operating voltage. As there is no doping junction present, future scaling could be feasible along with much higher speed of charge carriers than in silicon. GaAs:Si, Si:Si0.3Ge0.7, Si:InAs, and GaAs:Ge, H-JLTFET interface for 20-nm gate length (EOT=2 nm) and dielectric, HfO2 at VGS=1 V and temperature of 300 K have ION of 0.02-12.5 mA/μm, ION/IOFF of 10 5 -10 12 , and subthreshold swing (average) of 16-74 mV/decade.</description><identifier>ISSN: 0018-9383</identifier><identifier>EISSN: 1557-9646</identifier><identifier>DOI: 10.1109/TED.2013.2295238</identifier><identifier>CODEN: IETDAI</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Devices ; Field effect transistors ; Gallium arsenide ; hetero junctionless tunnel field-effect transistor (H-JLTFET) ; Heterojunctions ; High speed ; high-speed devices ; indium arsenide ; junctionless tunnel field-effect transistor (JLTFET) ; Junctions ; Logic gates ; Photonic band gap ; Semiconductor devices ; Semiconductors ; Silicon ; Transistors ; tunnel field-effect transistor (TFET) ; Tunneling ; Tunnels (transportation)</subject><ispartof>IEEE transactions on electron devices, 2014-02, Vol.61 (2), p.479-486</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. 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However, they suffer from low ON-current and high threshold voltage. In this paper, we present III-V heterojunctionless TFET (H-JLTFET) for circuit applications. This paper elaborates on interfacing of III-V with group IV semiconductors for heterojunction. Implementing heterojunction and bandgap engineering, we found that devices have significantly improved performance with very high speed even at very low operating voltage. As there is no doping junction present, future scaling could be feasible along with much higher speed of charge carriers than in silicon. GaAs:Si, Si:Si0.3Ge0.7, Si:InAs, and GaAs:Ge, H-JLTFET interface for 20-nm gate length (EOT=2 nm) and dielectric, HfO2 at VGS=1 V and temperature of 300 K have ION of 0.02-12.5 mA/μm, ION/IOFF of 10 5 -10 12 , and subthreshold swing (average) of 16-74 mV/decade.</description><subject>Devices</subject><subject>Field effect transistors</subject><subject>Gallium arsenide</subject><subject>hetero junctionless tunnel field-effect transistor (H-JLTFET)</subject><subject>Heterojunctions</subject><subject>High speed</subject><subject>high-speed devices</subject><subject>indium arsenide</subject><subject>junctionless tunnel field-effect transistor (JLTFET)</subject><subject>Junctions</subject><subject>Logic gates</subject><subject>Photonic band gap</subject><subject>Semiconductor devices</subject><subject>Semiconductors</subject><subject>Silicon</subject><subject>Transistors</subject><subject>tunnel field-effect transistor (TFET)</subject><subject>Tunneling</subject><subject>Tunnels (transportation)</subject><issn>0018-9383</issn><issn>1557-9646</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNpdkEFrGzEQRkVpoG7Se6GXhVxykaORtCvpWBKnNhhayLZXoWpHzZr1ypF2Cfn3leOQQ04z8_FmGB4hX4EtAZi5ble3S85ALDk3NRf6A1lAXStqGtl8JAvGQFMjtPhEPue8K2MjJV-Qh3X_74HeHxC7yo1dtY1P9Fd8wlT9HqbkOsQDvZ__7nuf4h6nkm82G_qnWh_7uJtHP_VxHDDnqp3HEYfqrseho6sQ0E9Vm9yY-zzFdEHOghsyfnmt56S9W7U3a7r9-WNz831LvTBsKu8qFYyUaIQKIDoMovGB65ICk8rp0Hjv647VTDsmQXeNAccZogxCe3FOrk5nDyk-zpgnu--zx2FwI8Y5W2gUSG24YgW9fIfu4pzG8pwFaUCCgheKnagiIOeEwR5Sv3fp2QKzR_O2mLdH8_bVfFn5dlrpEfENb1RhFBf_AQEkfqA</recordid><startdate>20140201</startdate><enddate>20140201</enddate><creator>Asthana, Pranav Kumar</creator><creator>Ghosh, Bahniman</creator><creator>Goswami, Yogesh</creator><creator>Tripathi, Ball Mukund Mani</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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However, they suffer from low ON-current and high threshold voltage. In this paper, we present III-V heterojunctionless TFET (H-JLTFET) for circuit applications. This paper elaborates on interfacing of III-V with group IV semiconductors for heterojunction. Implementing heterojunction and bandgap engineering, we found that devices have significantly improved performance with very high speed even at very low operating voltage. As there is no doping junction present, future scaling could be feasible along with much higher speed of charge carriers than in silicon. GaAs:Si, Si:Si0.3Ge0.7, Si:InAs, and GaAs:Ge, H-JLTFET interface for 20-nm gate length (EOT=2 nm) and dielectric, HfO2 at VGS=1 V and temperature of 300 K have ION of 0.02-12.5 mA/μm, ION/IOFF of 10 5 -10 12 , and subthreshold swing (average) of 16-74 mV/decade.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TED.2013.2295238</doi><tpages>8</tpages></addata></record> |
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subjects | Devices Field effect transistors Gallium arsenide hetero junctionless tunnel field-effect transistor (H-JLTFET) Heterojunctions High speed high-speed devices indium arsenide junctionless tunnel field-effect transistor (JLTFET) Junctions Logic gates Photonic band gap Semiconductor devices Semiconductors Silicon Transistors tunnel field-effect transistor (TFET) Tunneling Tunnels (transportation) |
title | High-Speed and Low-Power Ultradeep-Submicrometer III-V Heterojunctionless Tunnel Field-Effect Transistor |
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