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5纳米以下节点硅纳米片场效应晶体管中SiGe和SiC引起的阈值电压变化

Threshold Voltage Variations Induced by SiGe and SiC of Sub 5-nm Node Silicon Nanosheet Field-Effect Transistors.

作者信息

Jeong Jinsu, Yoon Jun-Sik, Lee Seunghwan, Baek Rock-Hyun

机构信息

Department of Electrical Engineering, Pohang University of Science and Technology (POSTECH), Pohang 37673, Republic of Korea.

出版信息

J Nanosci Nanotechnol. 2020 Aug 1;20(8):4684-4689. doi: 10.1166/jnn.2020.17799.

DOI:10.1166/jnn.2020.17799
PMID:32126641
Abstract

In this paper, we investigated the threshold voltage () variations in sub 5-nm node silicon nanosheet FETs (NSFETs) caused by Ge and C diffusion into NS channels using fully-calibrated 3-D TCAD simulation. Ge (C) atoms of SiGe (SiC) source/drain (S/D) diffuse toward the NS channels in lateral direction in -type (-type) FETs, and Ge atoms of SiGe stacks diffuse toward the NS channels in vertical direction. Increasing Ge mole fraction of the SiGe S/D in the -type FETs (PFETs) causing increasing compressive channel stress retards boron dopants diffusing from the SiGe S/D into the NS channels, thus increasing the of PFETs (). However, the decreases as the Ge mole fraction of the SiGe S/D becomes greater than 0.5 due to the higher valence band energy () of the NS channels. On the other hand, the of -type FETs (NFETs) () consistently increases as the C mole fraction of the SiC S/D increases due to monotonously retarded phosphorus dopants diffusing from the SiC S/D into the NS channels. On the other hand, the and consistently decreases and increases, respectively, as Si/SiGe intermixing becomes severer because both and conduction band energies () of the NS channels become higher. In addition, the variations are more sensitive to the Si/SiGe intermixing than the variations because the Ge mole fraction in NS channels affects the remarkably rather than the . As a result, the Ge atoms diffusing toward the NS channels should be carefully considered more than the C diffusion toward the NS channels for fine variation optimization in sub 5-nm node NSFETs.

摘要

在本文中,我们使用完全校准的三维工艺计算机辅助设计(TCAD)模拟,研究了锗(Ge)和碳(C)扩散到硅纳米片场效应晶体管(NSFET)的纳米片中,导致低于5纳米节点的NSFET阈值电压( )变化的情况。在p型(n型)FET中,SiGe(SiC)源极/漏极(S/D)中的Ge(C)原子沿横向向NS沟道扩散,而SiGe叠层中的Ge原子沿垂直方向向NS沟道扩散。在p型FET(PFET)中增加SiGe S/D的Ge摩尔分数会导致压缩沟道应力增加,从而阻碍硼掺杂剂从SiGe S/D扩散到NS沟道中,进而增加PFET的 ( )。然而,由于NS沟道的价带能量( )较高,当SiGe S/D的Ge摩尔分数大于0.5时, 会降低。另一方面,随着SiC S/D的C摩尔分数增加,n型FET(NFET)的 ( )持续增加,这是因为从SiC S/D扩散到NS沟道中的磷掺杂剂受到持续阻碍。另一方面,随着Si/SiGe混合变得更严重, 和 分别持续降低和增加,因为NS沟道的 和导带能量( )都变得更高。此外, 变化对Si/SiGe混合比 变化更敏感,因为NS沟道中的Ge摩尔分数对 的影响显著大于对 的影响。因此,对于低于5纳米节点的NSFET中精细的 变化优化,向NS沟道扩散的Ge原子比向NS沟道扩散的C更应仔细考虑。

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