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通过磁控溅射和闪光灯退火制备薄镍锗薄膜

Formation of Thin NiGe Films by Magnetron Sputtering and Flash Lamp Annealing.

作者信息

Begeza Viktor, Mehner Erik, Stöcker Hartmut, Xie Yufang, García Alejandro, Hübner Rene, Erb Denise, Zhou Shengqiang, Rebohle Lars

机构信息

Helmholtz-Zentrum Dresden-Rossendorf, Institute of Ion Beam Physics and Materials Research, Bautzner Landstrasse 400, 01328 Dresden, Germany.

TU Dresden, faculty of physics, 01062 Dresden, Germany.

出版信息

Nanomaterials (Basel). 2020 Mar 31;10(4):648. doi: 10.3390/nano10040648.

DOI:10.3390/nano10040648
PMID:32244356
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7221967/
Abstract

The nickel monogermanide (NiGe) phase is known for its electrical properties such as low ohmic and low contact resistance in group-IV-based electronics. In this work, thin films of nickel germanides (Ni-Ge) were formed by magnetron sputtering followed by flash lamp annealing (FLA). The formation of NiGe was investigated on three types of substrates: on amorphous (a-Ge) as well as polycrystalline Ge (poly-Ge) and on monocrystalline (100)-Ge (c-Ge) wafers. Substrate and NiGe structure characterization was performed by Raman, TEM, and XRD analyses. Hall Effect and four-point-probe measurements were used to characterize the films electrically. NiGe layers were successfully formed on different Ge substrates using 3-ms FLA. Electrical as well as XRD and TEM measurements are revealing the formation of Ni-rich hexagonal and cubic phases at lower temperatures accompanied by the formation of the low-resistivity orthorhombic NiGe phase. At higher annealing temperatures, Ni-rich phases are transforming into NiGe, as long as the supply of Ge is ensured. NiGe layer formation on a-Ge is accompanied by metal-induced crystallization and its elevated electrical resistivity compared with that of poly-Ge and c-Ge substrates. Specific resistivities for 30 nm Ni on Ge were determined to be 13.5 μΩ·cm for poly-Ge, 14.6 μΩ·cm for c-Ge, and 20.1 μΩ·cm for a-Ge.

摘要

一锗化镍(NiGe)相因其电学性质而闻名,比如在基于IV族的电子器件中具有低欧姆电阻和低接触电阻。在本工作中,通过磁控溅射然后进行闪光灯退火(FLA)形成了锗化镍(Ni-Ge)薄膜。在三种类型的衬底上研究了NiGe的形成:非晶锗(a-Ge)、多晶锗(poly-Ge)以及单晶(100)-锗(c-Ge)晶圆。通过拉曼光谱、透射电子显微镜(TEM)和X射线衍射(XRD)分析对衬底和NiGe结构进行了表征。利用霍尔效应和四点探针测量对薄膜进行电学表征。使用3毫秒的闪光灯退火在不同的锗衬底上成功形成了NiGe层。电学以及XRD和TEM测量结果表明,在较低温度下形成了富镍的六方相和立方相,同时形成了低电阻率的正交晶系NiGe相。在较高的退火温度下,只要确保锗的供应,富镍相就会转变成NiGe。在a-Ge上形成NiGe层伴随着金属诱导结晶,并且与poly-Ge和c-Ge衬底相比其电阻率升高。对于在锗上的30纳米镍,poly-Ge的比电阻率测定为13.5μΩ·cm,c-Ge为14.6μΩ·cm,a-Ge为20.1μΩ·cm。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a58/7221967/7585323ef4e7/nanomaterials-10-00648-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a58/7221967/a09ba1cdec96/nanomaterials-10-00648-g0A1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a58/7221967/c11f8a4aa2f8/nanomaterials-10-00648-g0A2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a58/7221967/c8983beda8a0/nanomaterials-10-00648-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a58/7221967/38a70860e24e/nanomaterials-10-00648-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a58/7221967/749b233d674f/nanomaterials-10-00648-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a58/7221967/7585323ef4e7/nanomaterials-10-00648-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a58/7221967/a09ba1cdec96/nanomaterials-10-00648-g0A1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a58/7221967/c11f8a4aa2f8/nanomaterials-10-00648-g0A2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a58/7221967/c8983beda8a0/nanomaterials-10-00648-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a58/7221967/38a70860e24e/nanomaterials-10-00648-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a58/7221967/749b233d674f/nanomaterials-10-00648-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1a58/7221967/7585323ef4e7/nanomaterials-10-00648-g004.jpg

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本文引用的文献

1
Germanium Based Field-Effect Transistors: Challenges and Opportunities.基于锗的场效应晶体管:挑战与机遇。
Materials (Basel). 2014 Mar 19;7(3):2301-2339. doi: 10.3390/ma7032301.
2
Oxide-confined formation of germanium nanowire heterostructures for high-performance transistors.氧化物限域形成用于高性能晶体管的锗纳米线异质结构。
ACS Nano. 2011 Jul 26;5(7):6008-15. doi: 10.1021/nn2017777. Epub 2011 Jul 1.