Abstract

Nanosheet (NS) and nanowire (NW) FET architectures scaled to a gate length ( $L_{\textbf {G}}$ ) of 16 nm and below are benchmarked against equivalent FinFETs. The device performance is predicted using a 3D finite element drift-diffusion/Monte Carlo simulation toolbox with integrated 2D Schrodinger equation based quantum corrections. The NS FET is a viable replacement for the FinFET in high performance (HP) applications when scaled down to $L_{\textbf {G}}$ of 16 nm offering a larger on-current ( $I_{\textbf {ON}}$ ) and slightly better sub-threshold characteristics. Below $\text{L}_{\textbf {G}}$ of 16 nm, the NW FET becomes the most promising architecture offering an almost ideal sub-threshold swing, the smallest off-current ( $I_{\textbf {OFF}}$ ), and the largest $I_{\textbf {ON}}/I_{\textbf {OFF}}$ ratio out of the three architectures. However, the NW FET suffers from early $I_{\textrm {ON}}$ saturation with the increasing gate bias that can be tackled by minimizing interface roughness and/or by optimisation of a doping profile in the device body.

Highlights

  • Fin field effect transistor (FinFET) technology is the leading architecture for high performance (HP) applications

  • The overall performance enhancement is compared through the ION/IOFF ratio and we found that it decreases by −32%, −68% and −76% for the NW FET, NS FET and FinFET, respectively, as we increased the NS/D from 5 × 1019 cm−3 to 1.5 × 1020 cm−3

  • The NS FET can be an excellent alternative to the FinFET for various digital applications because it offers a higher ION and slightly better sub-threshold region characteristics while reusing a similar fabrication process

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Summary

INTRODUCTION

Fin field effect transistor (FinFET) technology is the leading architecture for high performance (HP) applications. Three parameters were adjusted: (i) the maximum source/drain doping (NS/D), (ii) the position (Xmax) where the doping starts to decay from NS/D, and (iii) the Gaussian lateral straggle (σmax) This process is repeated until a good agreement is achieved in ID-VG characteristics between the experimental and the simulated data in the sub-threshold region obtained from the 3D SCH-DD. The characteristics are directly obtained by time consuming SCH-MC simulations of electron transport in the transistor domain including electrons in the heavily doped source/drain that provides a correct electron distribution for their injection into device channel [17], [33], [36]. An increase in NS/D affects the performance of the FinFET the most, leading to the worst sub-threshold characteristics and the lowest ION

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