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高性能P型和N型硅锗/硅应变超晶格鳍式场效应晶体管及CMOS反相器:硅和硅锗鳍式场效应晶体管的比较

High-Performance P- and N-Type SiGe/Si Strained Super-Lattice FinFET and CMOS Inverter: Comparison of Si and SiGe FinFET.

作者信息

Yao Yi-Ju, Yang Ching-Ru, Tseng Ting-Yu, Chang Heng-Jia, Lin Tsai-Jung, Luo Guang-Li, Hou Fu-Ju, Wu Yung-Chun, Chang-Liao Kuei-Shu

机构信息

College of Semiconductor Research, National Tsing Hua University, Hsinchu 30013, Taiwan.

Department of Engineering and System Science, National Tsing Hua University, Hsinchu 30013, Taiwan.

出版信息

Nanomaterials (Basel). 2023 Apr 8;13(8):1310. doi: 10.3390/nano13081310.

DOI:10.3390/nano13081310
PMID:37110895
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10145376/
Abstract

This research presents the optimization and proposal of P- and N-type 3-stacked SiGe/Si strained super-lattice FinFETs (SL FinFET) using Low-Pressure Chemical Vapor Deposition (LPCVD) epitaxy. Three device structures, Si FinFET, SiGe FinFET, and SiGe/Si SL FinFET, were comprehensively compared with HfO = 4 nm/TiN = 80 nm. The strained effect was analyzed using Raman spectrum and X-ray diffraction reciprocal space mapping (RSM). The results show that SiGe/Si SL FinFET exhibited the lowest average subthreshold slope (SS) of 88 mV/dec, the highest maximum transconductance (G) of 375.2 μS/μm, and the highest ON-OFF current ratio (I/I), approximately 10 at V = 0.5 V due to the strained effect. Furthermore, with the super-lattice FinFETs as complementary metal-oxide-semiconductor (CMOS) inverters, a maximum gain of 91 was achieved by varying the supply voltage from 0.6 V to 1.2 V. The simulation of a SiGe/Si super-lattice FinFET with the state of the art was also investigated. The proposed SiGe/Si strained SL FinFET is fully compatible with the CMOS technology platform, showing promising flexibility for extending CMOS scaling.

摘要

本研究介绍了采用低压化学气相沉积(LPCVD)外延技术对P型和N型三层SiGe/Si应变超晶格鳍式场效应晶体管(SL FinFET)进行的优化及方案。将三种器件结构,即硅鳍式场效应晶体管(Si FinFET)、硅锗鳍式场效应晶体管(SiGe FinFET)和SiGe/Si SL FinFET,与HfO = 4 nm/TiN = 80 nm进行了全面比较。利用拉曼光谱和X射线衍射倒易空间映射(RSM)分析了应变效应。结果表明,由于应变效应,SiGe/Si SL FinFET表现出最低的平均亚阈值斜率(SS),为88 mV/dec,最高的最大跨导(G),为375.2 μS/μm,以及最高的开/关电流比(I/I),在V = 0.5 V时约为10。此外,将超晶格鳍式场效应晶体管用作互补金属氧化物半导体(CMOS)反相器时,通过将电源电压从0.6 V变化到1.2 V,实现了91的最大增益。还研究了与现有技术水平的SiGe/Si超晶格鳍式场效应晶体管的模拟。所提出的SiGe/Si应变SL FinFET与CMOS技术平台完全兼容,显示出在扩展CMOS缩放方面具有良好的灵活性。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/9ed464b49600/nanomaterials-13-01310-g012.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/8594c6b8d2dd/nanomaterials-13-01310-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/9ed464b49600/nanomaterials-13-01310-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/6167a055bd26/nanomaterials-13-01310-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/4fdc5869a09a/nanomaterials-13-01310-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/1ab3bf09c9cd/nanomaterials-13-01310-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/8166ec205671/nanomaterials-13-01310-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/32ff252e62aa/nanomaterials-13-01310-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/666e9b40e600/nanomaterials-13-01310-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/94d334184e22/nanomaterials-13-01310-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/790626466d29/nanomaterials-13-01310-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/c0711408d6e0/nanomaterials-13-01310-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/b68642374bf5/nanomaterials-13-01310-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/8594c6b8d2dd/nanomaterials-13-01310-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9527/10145376/9ed464b49600/nanomaterials-13-01310-g012.jpg

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