Jenny Hu, X. Guan, D. Choi, J. Harris, K. Saraswat, H. Wong
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引用次数: 4
摘要
高迁移率III-V化合物是将高性能逻辑扩展到22纳米技术节点以外的有力竞争者[1-3]。然而,尽管栅极长度为纳米级,但优异的III-V性能的演示需要微米级的器件封装,以避免接触合金过程中的源极/漏极短路。通常用于欧姆接触的多层合金结构的横向扩散大得令人无法接受,这严重限制了III-V型场效应管的缩放[4]。在我们最近的工作中,我们通过使用Al作为非固定费米能级上的低工作功能金属,引入了一种新型的非合金,高度可扩展的接触结构[5]。我们使用砷化镓作为基准III-V材料,其中开发的接触技术可以扩展到InGaAs和InSb,这些材料在技术上更重要[6]。在这项工作中,我们详细解释了解钉机制和材料选择的基本原理。我们证明了相同的方法可以应用于各种金属,Y, Er, Al, Ti, W和Pt,为III-V HEMTs/ mosfet和肖特基势垒fet的理想源极/漏极触点设计提供了很大的灵活性。
Fermi level depinning for the design of III–V FET source/drain contacts
High mobility III–V compounds is a strong contender for extending high performance logic beyond the 22 nm technology node [1–3]. However, demonstrations of exceptional III–V performance required device footprints on the µm-scale despite nm-scale gate lengths, in order to avoid source/drain shorting during contact alloying. The scaling of III–V FETs is severely limited by the unacceptably large lateral diffusion of the multilayer alloyed structures typically used for ohmic contacts [4]. In our recent work, we introduced a novel non-alloyed, highly scalable contact structure through the use of Al as a low workfunction metal on an unpinned Fermi level [5]. We use GaAs as a baseline III–V material, where the developed contact techniques can be extended to InGaAs and InSb, materials which are more technologically important [6]. In this work, we explain in detail the unpinning mechanisms and the rationale for the material selection. We demonstrate the same method can be applied to a variety of metals, Y, Er, Al, Ti, W, and Pt, providing much flexibility in the design of an ideal source/drain contact for III–V HEMTs/MOSFETs and Schottky Barrier FETs.