压电栅极阻挡的亚玻尔兹曼晶体管

R. Jana, G. Snider, D. Jena
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引用次数: 3

摘要

场效应晶体管(fet)的缩放受到高功耗密度和ic中产生的热量的限制[1]。这是由于亚阈值斜率(SS)的不可扩展性,即将漏极电流改变一个数量级所需的栅极电压;在经典玻尔兹曼FET开关中,该值被限制在SS=kTln(10)~ 60mv /dec[2-3]。隧道场效应管正在研究亚玻尔兹曼开关。但即使是传统的场效应管也有可能利用铁电栅极材料实现亚玻尔兹曼开关[3]。可以在施加的栅极偏置电压Vg上放大内部通道表面电位Ψs;栅极绝缘子采用负差分电容(NDC)。然后“体因子”降低到单位以下,即m =∂Vg /∂Ψs <;因此,阈下斜率(SS=m×60 mV/dec)可以降低到60 mV/dec以下。在这项工作中,我们表明这种内部增益机制也可以存在于压电栅材料中,例如AIN/GaN异质结构中。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Sub-Boltzmann transistors with piezoelectric gate barriers
Scaling of field-effect transistors (FETs) is limited by the high power dissipation density, and the resulting heat generation in ICs [1]. This is due to the non-scalability of subthreshold slope (SS), i.e. the gate voltage required to change the drain current by an order of magnitude; the value is limited to SS=kTln(10)~60 mV/dec in a classical Boltzmann FET switch [2-3]. Tunneling FETs are being investigated for sub-Boltzmann switching. But even a conventional FET can potentially achieve sub-Boltzmann switching taking advantage of ferroelectric gates materials [3]. It is possible to amplify the internal channel surface potential, Ψs over the applied gate bias voltage, Vg; using negative differential capacitance (NDC) in the gate insulator. The “body factor” then reduces below unity i.e. m = ∂Vg / ∂Ψs <; 1, and hence the subthreshold slope (SS=m×60 mV/dec) can be lowered below 60 mV/dec. In this work, we show that such internal gain mechanism can also exist in piezoelectric gate materials, such as in AIN/GaN heterostructures.
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