Performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using TCAD tool

Abstract In this paper, we propose an n-type double gate junctionless field-effect-transistor using recessed silicon channel. The recessed silicon channel reduces the channel thickness between the underlap regions, results in lowering the number of charge carriers in the silicon channel, and therefo...
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Autor*in:	Kumar, Sandeep [verfasserIn] Chatterjee, Arun Kumar Pandey, Rishikesh

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2021

Schlagwörter:	FET Junctionless Double Gate Short Channel Effects Recessed

Anmerkung:	© The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021

Übergeordnetes Werk:	Enthalten in: Journal of computational electronics - Dordrecht : Springer Science + Business Media B.V., 2002, 20(2021), 6 vom: 15. Sept., Seite 2317-2330
Übergeordnetes Werk:	volume:20 ; year:2021 ; number:6 ; day:15 ; month:09 ; pages:2317-2330

Links:	Volltext

DOI / URN:	10.1007/s10825-021-01774-9

Katalog-ID:	SPR045783764

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520			\|a Abstract In this paper, we propose an n-type double gate junctionless field-effect-transistor using recessed silicon channel. The recessed silicon channel reduces the channel thickness between the underlap regions, results in lowering the number of charge carriers in the silicon channel, and therefore, diminishing the OFF-current in the device. The proposed device shows similar electrical characteristics with improved transconductance, as compared to the conventional double gate junctionless field-effect-transistor. The effect of channel length scaling on the performance have been investigated, and it has been found that the recessed junctionless device shows higher ON-to-OFF current ratio, lower subthreshold swing and better immunity against the short channel effects, namely threshold voltage roll-off and drain-induced-barrier-lowering. For a channel length of 20 nm the OFF-current of the order of 1.20 × $ 10^{–14} $ A/µm, ON-to-OFF current ratio of the order of 6.01 × $ 10^{10} $, subthreshold swing of the value of 67 mV/dec, and DIBL of 37.8 mV $ V^{−1} $ has been achieved with the proposed junctionless device, in comparison of conventional double gate junctionless FET. The performance of proposed device with respect to the variations in depth and length of recessed silicon area, has also been presented as a roadmap for further tuning of its electrical behaviour. Comparatively, steeper DC transfer characteristics and improved rail-to-rail swing in transient behaviour has been reported with the designed complementary metal–oxide–semiconductor inverter, based on recessed double gate junctionless FET. The proposed recessed silicon channel double gate junctionless field-effect-transistor has been simulated using TCAD tool.
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912			\|a GBV_ILN_100
912			\|a GBV_ILN_101
912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_120
912			\|a GBV_ILN_138
912			\|a GBV_ILN_150
912			\|a GBV_ILN_151
912			\|a GBV_ILN_152
912			\|a GBV_ILN_161
912			\|a GBV_ILN_170
912			\|a GBV_ILN_171
912			\|a GBV_ILN_187
912			\|a GBV_ILN_213
912			\|a GBV_ILN_224
912			\|a GBV_ILN_230
912			\|a GBV_ILN_250
912			\|a GBV_ILN_281
912			\|a GBV_ILN_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_602
912			\|a GBV_ILN_636
912			\|a GBV_ILN_702
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912			\|a GBV_ILN_2004
912			\|a GBV_ILN_2005
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912			\|a GBV_ILN_2007
912			\|a GBV_ILN_2008
912			\|a GBV_ILN_2009
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912			\|a GBV_ILN_2011
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912			\|a GBV_ILN_2015
912			\|a GBV_ILN_2020
912			\|a GBV_ILN_2021
912			\|a GBV_ILN_2025
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912			\|a GBV_ILN_2031
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912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2059
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2064
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912			\|a GBV_ILN_2106
912			\|a GBV_ILN_2107
912			\|a GBV_ILN_2108
912			\|a GBV_ILN_2110
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allfields	10.1007/s10825-021-01774-9 doi (DE-627)SPR045783764 (SPR)s10825-021-01774-9-e DE-627 ger DE-627 rakwb eng Kumar, Sandeep verfasserin aut Performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using TCAD tool 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021 Abstract In this paper, we propose an n-type double gate junctionless field-effect-transistor using recessed silicon channel. The recessed silicon channel reduces the channel thickness between the underlap regions, results in lowering the number of charge carriers in the silicon channel, and therefore, diminishing the OFF-current in the device. The proposed device shows similar electrical characteristics with improved transconductance, as compared to the conventional double gate junctionless field-effect-transistor. The effect of channel length scaling on the performance have been investigated, and it has been found that the recessed junctionless device shows higher ON-to-OFF current ratio, lower subthreshold swing and better immunity against the short channel effects, namely threshold voltage roll-off and drain-induced-barrier-lowering. For a channel length of 20 nm the OFF-current of the order of 1.20 × $ 10^{–14} $ A/µm, ON-to-OFF current ratio of the order of 6.01 × $ 10^{10} $, subthreshold swing of the value of 67 mV/dec, and DIBL of 37.8 mV $ V^{−1} $ has been achieved with the proposed junctionless device, in comparison of conventional double gate junctionless FET. The performance of proposed device with respect to the variations in depth and length of recessed silicon area, has also been presented as a roadmap for further tuning of its electrical behaviour. Comparatively, steeper DC transfer characteristics and improved rail-to-rail swing in transient behaviour has been reported with the designed complementary metal–oxide–semiconductor inverter, based on recessed double gate junctionless FET. The proposed recessed silicon channel double gate junctionless field-effect-transistor has been simulated using TCAD tool. FET (dpeaa)DE-He213 Junctionless (dpeaa)DE-He213 Double Gate (dpeaa)DE-He213 Short Channel Effects (dpeaa)DE-He213 Recessed (dpeaa)DE-He213 Chatterjee, Arun Kumar aut Pandey, Rishikesh aut Enthalten in Journal of computational electronics Dordrecht : Springer Science + Business Media B.V., 2002 20(2021), 6 vom: 15. Sept., Seite 2317-2330 (DE-627)340872063 (DE-600)2065612-9 1572-8137 nnns volume:20 year:2021 number:6 day:15 month:09 pages:2317-2330 https://dx.doi.org/10.1007/s10825-021-01774-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 20 2021 6 15 09 2317-2330
spelling	10.1007/s10825-021-01774-9 doi (DE-627)SPR045783764 (SPR)s10825-021-01774-9-e DE-627 ger DE-627 rakwb eng Kumar, Sandeep verfasserin aut Performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using TCAD tool 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021 Abstract In this paper, we propose an n-type double gate junctionless field-effect-transistor using recessed silicon channel. The recessed silicon channel reduces the channel thickness between the underlap regions, results in lowering the number of charge carriers in the silicon channel, and therefore, diminishing the OFF-current in the device. The proposed device shows similar electrical characteristics with improved transconductance, as compared to the conventional double gate junctionless field-effect-transistor. The effect of channel length scaling on the performance have been investigated, and it has been found that the recessed junctionless device shows higher ON-to-OFF current ratio, lower subthreshold swing and better immunity against the short channel effects, namely threshold voltage roll-off and drain-induced-barrier-lowering. For a channel length of 20 nm the OFF-current of the order of 1.20 × $ 10^{–14} $ A/µm, ON-to-OFF current ratio of the order of 6.01 × $ 10^{10} $, subthreshold swing of the value of 67 mV/dec, and DIBL of 37.8 mV $ V^{−1} $ has been achieved with the proposed junctionless device, in comparison of conventional double gate junctionless FET. The performance of proposed device with respect to the variations in depth and length of recessed silicon area, has also been presented as a roadmap for further tuning of its electrical behaviour. Comparatively, steeper DC transfer characteristics and improved rail-to-rail swing in transient behaviour has been reported with the designed complementary metal–oxide–semiconductor inverter, based on recessed double gate junctionless FET. The proposed recessed silicon channel double gate junctionless field-effect-transistor has been simulated using TCAD tool. FET (dpeaa)DE-He213 Junctionless (dpeaa)DE-He213 Double Gate (dpeaa)DE-He213 Short Channel Effects (dpeaa)DE-He213 Recessed (dpeaa)DE-He213 Chatterjee, Arun Kumar aut Pandey, Rishikesh aut Enthalten in Journal of computational electronics Dordrecht : Springer Science + Business Media B.V., 2002 20(2021), 6 vom: 15. Sept., Seite 2317-2330 (DE-627)340872063 (DE-600)2065612-9 1572-8137 nnns volume:20 year:2021 number:6 day:15 month:09 pages:2317-2330 https://dx.doi.org/10.1007/s10825-021-01774-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 20 2021 6 15 09 2317-2330
allfields_unstemmed	10.1007/s10825-021-01774-9 doi (DE-627)SPR045783764 (SPR)s10825-021-01774-9-e DE-627 ger DE-627 rakwb eng Kumar, Sandeep verfasserin aut Performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using TCAD tool 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021 Abstract In this paper, we propose an n-type double gate junctionless field-effect-transistor using recessed silicon channel. The recessed silicon channel reduces the channel thickness between the underlap regions, results in lowering the number of charge carriers in the silicon channel, and therefore, diminishing the OFF-current in the device. The proposed device shows similar electrical characteristics with improved transconductance, as compared to the conventional double gate junctionless field-effect-transistor. The effect of channel length scaling on the performance have been investigated, and it has been found that the recessed junctionless device shows higher ON-to-OFF current ratio, lower subthreshold swing and better immunity against the short channel effects, namely threshold voltage roll-off and drain-induced-barrier-lowering. For a channel length of 20 nm the OFF-current of the order of 1.20 × $ 10^{–14} $ A/µm, ON-to-OFF current ratio of the order of 6.01 × $ 10^{10} $, subthreshold swing of the value of 67 mV/dec, and DIBL of 37.8 mV $ V^{−1} $ has been achieved with the proposed junctionless device, in comparison of conventional double gate junctionless FET. The performance of proposed device with respect to the variations in depth and length of recessed silicon area, has also been presented as a roadmap for further tuning of its electrical behaviour. Comparatively, steeper DC transfer characteristics and improved rail-to-rail swing in transient behaviour has been reported with the designed complementary metal–oxide–semiconductor inverter, based on recessed double gate junctionless FET. The proposed recessed silicon channel double gate junctionless field-effect-transistor has been simulated using TCAD tool. FET (dpeaa)DE-He213 Junctionless (dpeaa)DE-He213 Double Gate (dpeaa)DE-He213 Short Channel Effects (dpeaa)DE-He213 Recessed (dpeaa)DE-He213 Chatterjee, Arun Kumar aut Pandey, Rishikesh aut Enthalten in Journal of computational electronics Dordrecht : Springer Science + Business Media B.V., 2002 20(2021), 6 vom: 15. Sept., Seite 2317-2330 (DE-627)340872063 (DE-600)2065612-9 1572-8137 nnns volume:20 year:2021 number:6 day:15 month:09 pages:2317-2330 https://dx.doi.org/10.1007/s10825-021-01774-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 20 2021 6 15 09 2317-2330
allfieldsGer	10.1007/s10825-021-01774-9 doi (DE-627)SPR045783764 (SPR)s10825-021-01774-9-e DE-627 ger DE-627 rakwb eng Kumar, Sandeep verfasserin aut Performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using TCAD tool 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021 Abstract In this paper, we propose an n-type double gate junctionless field-effect-transistor using recessed silicon channel. The recessed silicon channel reduces the channel thickness between the underlap regions, results in lowering the number of charge carriers in the silicon channel, and therefore, diminishing the OFF-current in the device. The proposed device shows similar electrical characteristics with improved transconductance, as compared to the conventional double gate junctionless field-effect-transistor. The effect of channel length scaling on the performance have been investigated, and it has been found that the recessed junctionless device shows higher ON-to-OFF current ratio, lower subthreshold swing and better immunity against the short channel effects, namely threshold voltage roll-off and drain-induced-barrier-lowering. For a channel length of 20 nm the OFF-current of the order of 1.20 × $ 10^{–14} $ A/µm, ON-to-OFF current ratio of the order of 6.01 × $ 10^{10} $, subthreshold swing of the value of 67 mV/dec, and DIBL of 37.8 mV $ V^{−1} $ has been achieved with the proposed junctionless device, in comparison of conventional double gate junctionless FET. The performance of proposed device with respect to the variations in depth and length of recessed silicon area, has also been presented as a roadmap for further tuning of its electrical behaviour. Comparatively, steeper DC transfer characteristics and improved rail-to-rail swing in transient behaviour has been reported with the designed complementary metal–oxide–semiconductor inverter, based on recessed double gate junctionless FET. The proposed recessed silicon channel double gate junctionless field-effect-transistor has been simulated using TCAD tool. FET (dpeaa)DE-He213 Junctionless (dpeaa)DE-He213 Double Gate (dpeaa)DE-He213 Short Channel Effects (dpeaa)DE-He213 Recessed (dpeaa)DE-He213 Chatterjee, Arun Kumar aut Pandey, Rishikesh aut Enthalten in Journal of computational electronics Dordrecht : Springer Science + Business Media B.V., 2002 20(2021), 6 vom: 15. Sept., Seite 2317-2330 (DE-627)340872063 (DE-600)2065612-9 1572-8137 nnns volume:20 year:2021 number:6 day:15 month:09 pages:2317-2330 https://dx.doi.org/10.1007/s10825-021-01774-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 20 2021 6 15 09 2317-2330
allfieldsSound	10.1007/s10825-021-01774-9 doi (DE-627)SPR045783764 (SPR)s10825-021-01774-9-e DE-627 ger DE-627 rakwb eng Kumar, Sandeep verfasserin aut Performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using TCAD tool 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021 Abstract In this paper, we propose an n-type double gate junctionless field-effect-transistor using recessed silicon channel. The recessed silicon channel reduces the channel thickness between the underlap regions, results in lowering the number of charge carriers in the silicon channel, and therefore, diminishing the OFF-current in the device. The proposed device shows similar electrical characteristics with improved transconductance, as compared to the conventional double gate junctionless field-effect-transistor. The effect of channel length scaling on the performance have been investigated, and it has been found that the recessed junctionless device shows higher ON-to-OFF current ratio, lower subthreshold swing and better immunity against the short channel effects, namely threshold voltage roll-off and drain-induced-barrier-lowering. For a channel length of 20 nm the OFF-current of the order of 1.20 × $ 10^{–14} $ A/µm, ON-to-OFF current ratio of the order of 6.01 × $ 10^{10} $, subthreshold swing of the value of 67 mV/dec, and DIBL of 37.8 mV $ V^{−1} $ has been achieved with the proposed junctionless device, in comparison of conventional double gate junctionless FET. The performance of proposed device with respect to the variations in depth and length of recessed silicon area, has also been presented as a roadmap for further tuning of its electrical behaviour. Comparatively, steeper DC transfer characteristics and improved rail-to-rail swing in transient behaviour has been reported with the designed complementary metal–oxide–semiconductor inverter, based on recessed double gate junctionless FET. The proposed recessed silicon channel double gate junctionless field-effect-transistor has been simulated using TCAD tool. FET (dpeaa)DE-He213 Junctionless (dpeaa)DE-He213 Double Gate (dpeaa)DE-He213 Short Channel Effects (dpeaa)DE-He213 Recessed (dpeaa)DE-He213 Chatterjee, Arun Kumar aut Pandey, Rishikesh aut Enthalten in Journal of computational electronics Dordrecht : Springer Science + Business Media B.V., 2002 20(2021), 6 vom: 15. Sept., Seite 2317-2330 (DE-627)340872063 (DE-600)2065612-9 1572-8137 nnns volume:20 year:2021 number:6 day:15 month:09 pages:2317-2330 https://dx.doi.org/10.1007/s10825-021-01774-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 20 2021 6 15 09 2317-2330
language	English
source	Enthalten in Journal of computational electronics 20(2021), 6 vom: 15. Sept., Seite 2317-2330 volume:20 year:2021 number:6 day:15 month:09 pages:2317-2330
sourceStr	Enthalten in Journal of computational electronics 20(2021), 6 vom: 15. Sept., Seite 2317-2330 volume:20 year:2021 number:6 day:15 month:09 pages:2317-2330
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	FET Junctionless Double Gate Short Channel Effects Recessed
isfreeaccess_bool	false
container_title	Journal of computational electronics
authorswithroles_txt_mv	Kumar, Sandeep @@aut@@ Chatterjee, Arun Kumar @@aut@@ Pandey, Rishikesh @@aut@@
publishDateDaySort_date	2021-09-15T00:00:00Z
hierarchy_top_id	340872063
id	SPR045783764
language_de	englisch
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author	Kumar, Sandeep
spellingShingle	Kumar, Sandeep misc FET misc Junctionless misc Double Gate misc Short Channel Effects misc Recessed Performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using TCAD tool
authorStr	Kumar, Sandeep
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topic_title	Performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using TCAD tool FET (dpeaa)DE-He213 Junctionless (dpeaa)DE-He213 Double Gate (dpeaa)DE-He213 Short Channel Effects (dpeaa)DE-He213 Recessed (dpeaa)DE-He213
topic	misc FET misc Junctionless misc Double Gate misc Short Channel Effects misc Recessed
topic_unstemmed	misc FET misc Junctionless misc Double Gate misc Short Channel Effects misc Recessed
topic_browse	misc FET misc Junctionless misc Double Gate misc Short Channel Effects misc Recessed
format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
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title	Performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using TCAD tool
ctrlnum	(DE-627)SPR045783764 (SPR)s10825-021-01774-9-e
title_full	Performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using TCAD tool
author_sort	Kumar, Sandeep
journal	Journal of computational electronics
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author_browse	Kumar, Sandeep Chatterjee, Arun Kumar Pandey, Rishikesh
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format_se	Elektronische Aufsätze
author-letter	Kumar, Sandeep
doi_str_mv	10.1007/s10825-021-01774-9
title_sort	performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using tcad tool
title_auth	Performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using TCAD tool
abstract	Abstract In this paper, we propose an n-type double gate junctionless field-effect-transistor using recessed silicon channel. The recessed silicon channel reduces the channel thickness between the underlap regions, results in lowering the number of charge carriers in the silicon channel, and therefore, diminishing the OFF-current in the device. The proposed device shows similar electrical characteristics with improved transconductance, as compared to the conventional double gate junctionless field-effect-transistor. The effect of channel length scaling on the performance have been investigated, and it has been found that the recessed junctionless device shows higher ON-to-OFF current ratio, lower subthreshold swing and better immunity against the short channel effects, namely threshold voltage roll-off and drain-induced-barrier-lowering. For a channel length of 20 nm the OFF-current of the order of 1.20 × $ 10^{–14} $ A/µm, ON-to-OFF current ratio of the order of 6.01 × $ 10^{10} $, subthreshold swing of the value of 67 mV/dec, and DIBL of 37.8 mV $ V^{−1} $ has been achieved with the proposed junctionless device, in comparison of conventional double gate junctionless FET. The performance of proposed device with respect to the variations in depth and length of recessed silicon area, has also been presented as a roadmap for further tuning of its electrical behaviour. Comparatively, steeper DC transfer characteristics and improved rail-to-rail swing in transient behaviour has been reported with the designed complementary metal–oxide–semiconductor inverter, based on recessed double gate junctionless FET. The proposed recessed silicon channel double gate junctionless field-effect-transistor has been simulated using TCAD tool. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021
abstractGer	Abstract In this paper, we propose an n-type double gate junctionless field-effect-transistor using recessed silicon channel. The recessed silicon channel reduces the channel thickness between the underlap regions, results in lowering the number of charge carriers in the silicon channel, and therefore, diminishing the OFF-current in the device. The proposed device shows similar electrical characteristics with improved transconductance, as compared to the conventional double gate junctionless field-effect-transistor. The effect of channel length scaling on the performance have been investigated, and it has been found that the recessed junctionless device shows higher ON-to-OFF current ratio, lower subthreshold swing and better immunity against the short channel effects, namely threshold voltage roll-off and drain-induced-barrier-lowering. For a channel length of 20 nm the OFF-current of the order of 1.20 × $ 10^{–14} $ A/µm, ON-to-OFF current ratio of the order of 6.01 × $ 10^{10} $, subthreshold swing of the value of 67 mV/dec, and DIBL of 37.8 mV $ V^{−1} $ has been achieved with the proposed junctionless device, in comparison of conventional double gate junctionless FET. The performance of proposed device with respect to the variations in depth and length of recessed silicon area, has also been presented as a roadmap for further tuning of its electrical behaviour. Comparatively, steeper DC transfer characteristics and improved rail-to-rail swing in transient behaviour has been reported with the designed complementary metal–oxide–semiconductor inverter, based on recessed double gate junctionless FET. The proposed recessed silicon channel double gate junctionless field-effect-transistor has been simulated using TCAD tool. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021
abstract_unstemmed	Abstract In this paper, we propose an n-type double gate junctionless field-effect-transistor using recessed silicon channel. The recessed silicon channel reduces the channel thickness between the underlap regions, results in lowering the number of charge carriers in the silicon channel, and therefore, diminishing the OFF-current in the device. The proposed device shows similar electrical characteristics with improved transconductance, as compared to the conventional double gate junctionless field-effect-transistor. The effect of channel length scaling on the performance have been investigated, and it has been found that the recessed junctionless device shows higher ON-to-OFF current ratio, lower subthreshold swing and better immunity against the short channel effects, namely threshold voltage roll-off and drain-induced-barrier-lowering. For a channel length of 20 nm the OFF-current of the order of 1.20 × $ 10^{–14} $ A/µm, ON-to-OFF current ratio of the order of 6.01 × $ 10^{10} $, subthreshold swing of the value of 67 mV/dec, and DIBL of 37.8 mV $ V^{−1} $ has been achieved with the proposed junctionless device, in comparison of conventional double gate junctionless FET. The performance of proposed device with respect to the variations in depth and length of recessed silicon area, has also been presented as a roadmap for further tuning of its electrical behaviour. Comparatively, steeper DC transfer characteristics and improved rail-to-rail swing in transient behaviour has been reported with the designed complementary metal–oxide–semiconductor inverter, based on recessed double gate junctionless FET. The proposed recessed silicon channel double gate junctionless field-effect-transistor has been simulated using TCAD tool. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021
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container_issue	6
title_short	Performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using TCAD tool
url	https://dx.doi.org/10.1007/s10825-021-01774-9
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author2	Chatterjee, Arun Kumar Pandey, Rishikesh
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doi_str	10.1007/s10825-021-01774-9
up_date	2024-07-03T18:15:43.595Z
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fullrecord_marcxml	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR045783764</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230509095655.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">211213s2021 xx \|\|\|\|\|o 00\| \|\|eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s10825-021-01774-9</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR045783764</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s10825-021-01774-9-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Kumar, Sandeep</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using TCAD tool</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2021</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In this paper, we propose an n-type double gate junctionless field-effect-transistor using recessed silicon channel. The recessed silicon channel reduces the channel thickness between the underlap regions, results in lowering the number of charge carriers in the silicon channel, and therefore, diminishing the OFF-current in the device. The proposed device shows similar electrical characteristics with improved transconductance, as compared to the conventional double gate junctionless field-effect-transistor. The effect of channel length scaling on the performance have been investigated, and it has been found that the recessed junctionless device shows higher ON-to-OFF current ratio, lower subthreshold swing and better immunity against the short channel effects, namely threshold voltage roll-off and drain-induced-barrier-lowering. For a channel length of 20 nm the OFF-current of the order of 1.20 × $ 10^{–14} $ A/µm, ON-to-OFF current ratio of the order of 6.01 × $ 10^{10} $, subthreshold swing of the value of 67 mV/dec, and DIBL of 37.8 mV $ V^{−1} $ has been achieved with the proposed junctionless device, in comparison of conventional double gate junctionless FET. The performance of proposed device with respect to the variations in depth and length of recessed silicon area, has also been presented as a roadmap for further tuning of its electrical behaviour. Comparatively, steeper DC transfer characteristics and improved rail-to-rail swing in transient behaviour has been reported with the designed complementary metal–oxide–semiconductor inverter, based on recessed double gate junctionless FET. The proposed recessed silicon channel double gate junctionless field-effect-transistor has been simulated using TCAD tool.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">FET</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Junctionless</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Double Gate</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Short Channel Effects</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Recessed</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Chatterjee, Arun Kumar</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Pandey, Rishikesh</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Journal of computational electronics</subfield><subfield code="d">Dordrecht : Springer Science + Business Media B.V., 2002</subfield><subfield code="g">20(2021), 6 vom: 15. 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Performance enhancement of recessed silicon channel double gate junctionless field-effect-transistor using TCAD tool

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