纳米线无结晶体管的量子漂移扩散和量子能量平衡模拟

O. Badami, N. Kumar, D. Saha, S. Ganguly
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引用次数: 0

摘要

多栅极MOSFET (MuGFET)随着传统MOSFET的缩放结束而得到了极大的关注。在可能的架构中,栅极全能纳米线(NW)晶体管提供了对通道的最佳栅极控制。为了模拟通道长度小于10nm的GAA纳米线器件,同时保持与器件工程师熟悉的漂移扩散框架的连接,我们开发了一个量子校正输运模拟器,其中包括量子漂移扩散(QDD)和量子能量平衡(QEB)。这种形式被应用到NW无结晶体管(JLT)的例子中,这是对NW- mosfet的一个有趣的修改,通过用n+区域的条代替n+-p-n+结构获得,这保证了更小的可变性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Quantum Drift-Diffusion and Quantum Energy Balance simulation of nanowire junctionless transistors
Multiple gate MOSFETs (MuGFET) have gained significant attention as the scaling of the conventional MOSFET comes to an end. Of the possible architectures, the gate-all-around nanowire (NW) transistor offers the best gate control over the channel. In order to model GAA nanowire devices for channel lengths less than 10nm, while preserving a connection to the drift-diffusion framework familiar to device engineers, we have developed a quantum-corrected transport simulator that includes Quantum Drift-Diffusion (QDD) and Quantum Energy Balance (QEB). This formalism is applied to the example of the NW junctionless transistor (JLT), an interesting modification to the NW-MOSFET obtained by replacing the n+-p-n+ structure by a bar of n+ region, that promises smaller variability.
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