Impact of quantum confinement on transport and the electrostatic driven performance of silicon nanowire transistors at the scaling limit

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• 作者：Talib Al-Ameri^a ; ^b ; ^{t.ali.1@research.gla.ac.uk} ; Vihar P. Georgiev^a ; Toufik Sadi^a ; Yijiao Wang^a ; ^c ; Fikru Adamu-Lema^a ; Xingsheng Wang^d ; Salvatore M. Amoroso^d ; Ewan Towie^d ; Andrew Brown^d ; Asen Asenov^a ; ^d
• 关键词：CMOS ; Electrostatics ; Nanowire transistors ; Performance ; Quantum effects ; TCAD
• 刊名：Solid-State Electronics
• 出版年：2017
• 出版时间：March 2017
• 年：2017
• 卷：129
• 期：Complete
• 页码：73-80
• 全文大小：2467 K
• 卷排序：129

文摘

In this work we investigate the impact of quantum mechanical effects on the device performance of n-type silicon nanowire transistors (NWT) for possible future CMOS applications at the scaling limit. For the purpose of this paper, we created Si NWTs with two channel crystallographic orientations 〈1 1 0〉 and 〈1 0 0〉 and six different cross-section profiles. In the first part, we study the impact of quantum corrections on the gate capacitance and mobile charge in the channel. The mobile charge to gate capacitance ratio, which is an indicator of the intrinsic performance of the NWTs, is also investigated. The influence of the rotating of the NWTs cross-sectional geometry by 90° on charge distribution in the channel is also studied. We compare the correlation between the charge profile in the channel and cross-sectional dimension for circular transistor with four different cross-sections diameters: 5 nm, 6 nm, 7 nm and 8 nm. In the second part of this paper, we expand the computational study by including different gate lengths for some of the Si NWTs. As a result, we establish a correlation between the mobile charge distribution in the channel and the gate capacitance, drain-induced barrier lowering (DIBL) and the subthreshold slope (SS). All calculations are based on a quantum mechanical description of the mobile charge distribution in the channel. This description is based on the solution of the Schrödinger equation in NWT cross sections along the current path, which is mandatory for nanowires with such ultra-scale dimensions.