2019
DOI: 10.1109/ted.2019.2900995
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Deep Sub-60 mV/decade Subthreshold Swing in AlGaN/GaN FinMISHFETs with M-Plane Sidewall Channel

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Cited by 15 publications
(11 citation statements)
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“…This high positive oxide charge density in the sloped device lowers V TH of the sidewall MOS channel to increase I OFF . The SS of steep sidewall device is as low as 37 mV/dec due to the simultaneous turning on of 2DEG channel and MOS channel and the effective channel width modulation as discussed before [17]. On the other hand, the sloped sidewall device exhibits a relatively larger SS of 63 mV/dec, which could be explained by the existence of non-negligible C dep caused by the undepleted part at the wide fin bottom and relatively large C it, SiO 2 /GaN due to a rough sidewall surface [25], which increases both SS con and SS W(V G ) , while the C dep can be ignored for the device with a steep sidewall because the entire fin is narrow and completely depleted from the electric field of the sidewall gate at off-state.…”
Section: Resultsmentioning
confidence: 74%
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“…This high positive oxide charge density in the sloped device lowers V TH of the sidewall MOS channel to increase I OFF . The SS of steep sidewall device is as low as 37 mV/dec due to the simultaneous turning on of 2DEG channel and MOS channel and the effective channel width modulation as discussed before [17]. On the other hand, the sloped sidewall device exhibits a relatively larger SS of 63 mV/dec, which could be explained by the existence of non-negligible C dep caused by the undepleted part at the wide fin bottom and relatively large C it, SiO 2 /GaN due to a rough sidewall surface [25], which increases both SS con and SS W(V G ) , while the C dep can be ignored for the device with a steep sidewall because the entire fin is narrow and completely depleted from the electric field of the sidewall gate at off-state.…”
Section: Resultsmentioning
confidence: 74%
“…On the other hand, the narrow FinFET with W fin of 45 nm has a sharper and higher g m peak as can be seen in Figure 2c, which means that the V TH of the 2DEG channel and MOS channel are almost the same and hence both channels simultaneously turn on/off and the effective channel width of the device can be modulated with the gate voltage, which results in very small SS as low as 56 mV/dec, smaller than the theoretical Boltzmann limit of 60 mV/dec. As discussed in our previous work [17], the 2DEG channel will be generated at the center of the 2DEG channel and laterally spread until occupying the whole 2DEG channel as V G increases from the V TH of the 2DEG channel to just above it. Then, the MOS channel will instantaneously turn on because there is only a tiny V TH difference between the top 2DEG channel and the sidewall MOS channel.…”
Section: Resultsmentioning
confidence: 75%
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