2011
DOI: 10.1109/ted.2011.2159797
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Silicon Nanowire Tunnel FETs: Low-Temperature Operation and Influence of High- $k$ Gate Dielectric

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Cited by 52 publications
(29 citation statements)
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“…The ON current is around 0:02 lA=lm at V GS ¼ À4 V and V DS ¼ À0:5 V. We observe also that all the transfer characteristics show an average subthreshold swing ðSS avg Þ near 320 mV/dec, which is larger than 60 mV/decade. These results are relatively close to those presented in references [11][12][13]. In fact, Vallett et al have shown that using 5 nm of SiO 2 and 20 nm of HfO 2 as a gate stack oxide, they have obtained an I on current around 20 nA with a SS of about 370 mV/dec for V DS ¼ À0:5 V and V GS ¼ À12 V [13].…”
Section: Electrical Characterization At Roomsupporting
confidence: 89%
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“…The ON current is around 0:02 lA=lm at V GS ¼ À4 V and V DS ¼ À0:5 V. We observe also that all the transfer characteristics show an average subthreshold swing ðSS avg Þ near 320 mV/dec, which is larger than 60 mV/decade. These results are relatively close to those presented in references [11][12][13]. In fact, Vallett et al have shown that using 5 nm of SiO 2 and 20 nm of HfO 2 as a gate stack oxide, they have obtained an I on current around 20 nA with a SS of about 370 mV/dec for V DS ¼ À0:5 V and V GS ¼ À12 V [13].…”
Section: Electrical Characterization At Roomsupporting
confidence: 89%
“…In order to optimize the electrical performance of the TFET (I on current, I on =I off ratio, SS...), it is necessary to control the abruptness of the tunnel junction, the doping level of the source/drain contact and the interface traps close to tunnelling junction. Lot of attention has been devoted to the fabrication of tunnel FET devices using nanowires fabricated by top-down and bottom-up approaches [7][8][9][10][11][12][13], in order to obtain a good electrical performance.…”
Section: Introductionmentioning
confidence: 99%
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“…The tunnel FET has been identified as a promising candidate for low-power electronics as it can overcome the MOS limitations coming from the non-scalability of the inverse subthreshold slope (SS) [Chang et al 2010]. As demonstrated in Moselund et al [2011], nanowires are ideal to achieve a good tunnel FET as it requires the highest degree of electrostatic control. In particular, the key parameters to achieve good performance are the tunnel junction abruptness, the effective band gap at the tunneling junction, gate control over the channel, and overall device geometry.…”
Section: Low-power High-performances Devices: Towards Thin Devicesmentioning
confidence: 99%
“…Its working principle is based on the band-to-band tunnelling of carriers. This is made possible by proper band engineering, achieved in top-gated FET operated in reverse bias, with p-i-n þ [74,129] or p-n-n þ [130] channel doping ( Fig. 7(b)).…”
Section: Steep-ss Nanowire Devicesmentioning
confidence: 99%