超低比接触电阻率金属/ p型GeSn触点

X. Gong, Ying Wu, Haiwen Xu, Kaizhen Han, L. Chua, W. Zou, T. Henry
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引用次数: 0

摘要

近几十年来,场效应晶体管(fet)的源极/漏极(S/D)区域的接触电阻rc随着器件尺寸的缩小而显著增加[1]。对于最先进的晶体管技术,接触面积约为10×10 nm 2[2]。rc与有效接触面积成反比,是限制器件导通电流和开关速度的主要寄生电阻。为了减轻rc的影响,需要小于10−9 Ω-cm 2的超低比接触电阻率ρ c[3]。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Metal/P-type GeSn Contacts with Ultra-low Specific Contact Resistivity
Contact resistance R c in the source/drain (S/D) regions of field-effect transistors (FETs) has increased significantly due to the shrinkage of contact area accompanied with the scaling of device dimensions in the past decades [1] . For the state-of-art transistor technology, the contact area is around 10×10 nm 2 [2] . R c , inversely proportional to the effective contact area, is the main parasitic resistance that limits the on-state current and switching speed of the device in the leading technology. To alleviate the impact of R c , an ultralow specific contact resistivity ρ c of less than 10 −9 Ω-cm 2 is required [3] .
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