Scaling Challenges of Nanosheet Field-Effect Transistors Into Sub-2 nm Nodes

IF 4.6 Q2 MATERIALS SCIENCE, BIOMATERIALS ACS Applied Bio Materials Pub Date : 2024-06-18 DOI:10.1109/JEDS.2024.3416200
Murad G. K. Alabdullah;M. A. Elmessary;D. Nagy;N. Seoane;A. J. García-Loureiro;K. Kalna
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Abstract

The scaling of nanosheet (NS) field effect transistors (FETs) from the 12 nm gate length to the ultimate gate length of 10 nm for sub-2 nm nodes brings additional technological challenges. Here, 3D finite element Monte Carlo simulations are employed to explore how to alter the NS architecture to increase the drive current ( ${I}_{\mathrm {\mathbf { DD}}}$ ) because the gate scaling to 10 nm results in a decline of the current (by $\mathbf {10.7}$ %). ${I}_{\mathrm {\mathbf {DD}}}$ of the 10 nm gate length NS FET will increase by 11% if the maximum n-type source/drain doping reaches $1\times 10^{20} \mathrm {cm^{-3}}$ , or increase by $\mathbf {3.8}$ % if the high- $\kappa $ dielectric layer equivalent oxide thickness (EOT) is less than $\mathbf {1.0}$ nm. The reduction in the channel width below 40 nm or the reduction in the channel thickness below 5 nm will substantially decrease IDD. The sub-threshold figures of merit like the sub-threshold slope (SS) will decrease from 75 to 73 mV/dec, while the drain-induced barrier lowering (DIBL) will increase from 32 to 77 mV/V. Finally, the effect of strain to increase the drive current is strongly limited by quantum confinement. ${I}_{\mathrm {\mathbf {DD}}}$ will increase by 3% and by 14% in the 10 nm gate NS FET with the $\langle 110\rangle $ and $\langle 100\rangle $ channel orientations, respectively, when a strain of $\mathbf {0.5}$ % is applied to the channel, with a negligible increase for larger strain values ( $\mathbf {0.7}$ % and $\mathbf {1.0}$ %).
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将纳米片场效应晶体管扩展到 2 纳米以下节点所面临的挑战
纳米片(NS)场效应晶体管(FET)的栅极长度从 12 nm 增加到 10 nm,为 2 nm 以下节点带来了额外的技术挑战。由于栅极扩展到 10 纳米会导致电流下降(下降了 $\mathbf {10.7}$%),因此这里采用了三维有限元蒙特卡罗模拟来探索如何改变 NS 架构以增加驱动电流(${I}_{\mathrm {\mathbf { DD}}$ )。 如果 n 型源极/漏极的最大掺杂量达到 $1\times 10^{20} ,10 nm 栅极长度的 NS FET 的 ${I}_{mathrm {\mathbf {DD}}$ 将增加 11%。}\mathrm {cm^{-3}}$ ,或者如果高 $\kappa $ 介质层等效氧化物厚度 (EOT) 小于 $\mathbf {1.0}$ nm,则通道宽度将增加 $\mathbf {3.8}$ %。将沟道宽度减小到 40 nm 以下或将沟道厚度减小到 5 nm 以下将大大降低 IDD。阈下斜率(SS)等阈下性能指标将从 75 mV/dec 下降到 73 mV/dec,而漏极诱导势垒降低(DIBL)将从 32 mV/V 上升到 77 mV/V。最后,应变对增加驱动电流的影响受到量子约束的强烈限制。 当在沟道上施加 $\mathbf {0.5}$ % 的应变时,在沟道方向为 $\langle 110\rangle $ 和 $\langle 100\rangle $ 的 10 nm 栅极 NS FET 中,${I}_\{mathrm {\mathbf {DD}}$ 将分别增加 3% 和 14%,而当应变值较大时($\mathbf {0.7}$ % 和 $\mathbf {1.0}$ %),增加幅度可以忽略不计。)
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
ACS Applied Bio Materials
ACS Applied Bio Materials Chemistry-Chemistry (all)
CiteScore
9.40
自引率
2.10%
发文量
464
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