FET缩放还剩多少时间?

D. Mamaluy, X. Gao, B. Tierney
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引用次数: 1

摘要

在Frank Wanlass于1963年发明了CMOS缩放技术之后,几乎立即预测到了CMOS缩放的最终终结。实际上,在20世纪70年代、80年代和90年代就讨论过缩减规模的许多可能限制。2003年,Zhirnov等人根据海森堡不确定性和兰道尔原理估计,“二进制逻辑开关”的最小特征尺寸约为1.5nm。从那时起,已经有许多论文[2,4,5]讨论了由于光刻,功率-热,材料和其他技术而不是基本的物理限制而导致CMOS缩放的可能结束。在这项工作中,我们计算了几个具有代表性的FinFET/MuGFET器件的器件开关能量CgVg2,并探讨了该数量作为基本物理缩放限制的作用,我们预测这将在2030年左右发生。在此过程中,参考了ITRS降尺度投影数据[6]。当FET栅极长度缩放到6nm及以下时,mufet开关能量以100kBT (T=300K)为单位绘制为图1中的蓝色曲线。图1的插入部分表示我们对ITRS数据的外推。这种绘制开关能的新方法表明,当栅极长度缩小到约5nm以下时,开关能接近热波动的开关能。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
How much time does FET scaling have left?
The ultimate end of CMOS scaling was predicted almost immediately after the now ubiquitous technology was invented by Frank Wanlass in 1963 [1]. Indeed, many possible limitations to downscaling were discussed in the 1970s, 80s, and 90s [2]. In 2003, Zhirnov et al. [3] estimated the minimal feature size of a “binary logic switch” to be around 1.5nm, based on the Heisenberg uncertainty and Landauer principles. Since then, there have been many papers [2,4,5] discussing the likely end of CMOS scaling due to lithographical, power-thermal, material, and other technological, as opposed to fundamental physical, limitations. In this work, we compute the device switching energy, CgVg2, for several representative FinFET/MuGFET devices, and explore the role of this quantity as a fundamental physical scaling limitation, which we predict will occur around 2030. In doing so, ITRS downscaling projection data [6] is utilized for reference. MuGFET switching energies are plotted as the blue curve in Fig. 1, in units of 100kBT (T=300K), as FET gate lengths are scaled to 6-nm and below. The inset of Fig. 1 represents our extrapolation of ITRS data. This new way of plotting switching energy reveals that as gate lengths arescaled below about 5nm, the switching energy approaches that of thermal fluctuations.
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