接触电阻
材料科学
跨导
光电子学
肖特基势垒
晶体管
兴奋剂
氧化物
场效应晶体管
阈下斜率
阈下传导
阈值电压
等效串联电阻
半导体
频道(广播)
纳米技术
图层(电子)
电压
电气工程
冶金
二极管
工程类
作者
Chin‐Sheng Pang,Ruiping Zhou,Xiangkai Liu,Peng Wu,Terry Y.T. Hung,Shiqi Guo,Mona Zaghloul,Sergiy Krylyuk,Albert V. Davydov,Joerg Appenzeller,Zhihong Chen
出处
期刊:Small
[Wiley]
日期:2021-06-10
卷期号:17 (28): e2100940-e2100940
被引量:32
标识
DOI:10.1002/smll.202100940
摘要
Abstract Schottky barrier (SB) transistors operate distinctly different from conventional metal‐oxide semiconductor field‐effect transistors, in a unique way that the gate impacts the carrier injection from the metal source/drain contacts into the channel region. While it has been long recognized that this can have severe implications for device characteristics in the subthreshold region, impacts of contact gating of SB in the on‐state of the devices, which affects evaluation of intrinsic channel properties, have been yet comprehensively studied. Due to the fact that contact resistance ( R C ) is always gate‐dependent in a typical back‐gated device structure, the traditional approach of deriving field‐effect mobility from the maximum transconductance ( g m ) is in principle not correct and can even overestimate the mobility. In addition, an exhibition of two different threshold voltages for the channel and the contact region leads to another layer of complexity in determining the true carrier concentration calculated from Q = C OX * ( V G – V TH ). Through a detailed experimental analysis, the effect of different effective oxide thicknesses, distinct SB heights, and doping‐induced reductions in the SB width are carefully evaluated to gain a better understanding of their impact on important device metrics.
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