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金属锗的自下而上组装。

Bottom-up assembly of metallic germanium.

作者信息

Scappucci Giordano, Klesse Wolfgang M, Yeoh LaReine A, Carter Damien J, Warschkow Oliver, Marks Nigel A, Jaeger David L, Capellini Giovanni, Simmons Michelle Y, Hamilton Alexander R

机构信息

School of Physics, University of New South Wales, Sydney, 2052, Australia.

1] Department of Chemistry, Curtin University, Perth WA 6845, Australia. [2] Nanochemistry Research Institute, Curtin University, Perth WA 6845, Australia.

出版信息

Sci Rep. 2015 Aug 10;5:12948. doi: 10.1038/srep12948.

DOI:10.1038/srep12948
PMID:26256239
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC4530340/
Abstract

Extending chip performance beyond current limits of miniaturisation requires new materials and functionalities that integrate well with the silicon platform. Germanium fits these requirements and has been proposed as a high-mobility channel material, a light emitting medium in silicon-integrated lasers, and a plasmonic conductor for bio-sensing. Common to these diverse applications is the need for homogeneous, high electron densities in three-dimensions (3D). Here we use a bottom-up approach to demonstrate the 3D assembly of atomically sharp doping profiles in germanium by a repeated stacking of two-dimensional (2D) high-density phosphorus layers. This produces high-density (10(19) to 10(20) cm(-3)) low-resistivity (10(-4)Ω · cm) metallic germanium of precisely defined thickness, beyond the capabilities of diffusion-based doping technologies. We demonstrate that free electrons from distinct 2D dopant layers coalesce into a homogeneous 3D conductor using anisotropic quantum interference measurements, atom probe tomography, and density functional theory.

摘要

要将芯片性能提升至当前小型化极限之外,需要能与硅平台良好集成的新材料和新功能。锗符合这些要求,已被提议用作高迁移率沟道材料、硅基集成激光器中的发光介质以及用于生物传感的等离子体导体。这些不同应用的共同之处在于需要在三维空间(3D)中实现均匀的高电子密度。在此,我们采用自下而上的方法,通过重复堆叠二维(2D)高密度磷层来展示锗中原子级尖锐掺杂分布的三维组装。这产生了具有精确界定厚度的高密度(10¹⁹至10²⁰ cm⁻³)、低电阻率(10⁻⁴Ω·cm)的金属锗,这是基于扩散的掺杂技术所无法实现的。我们使用各向异性量子干涉测量、原子探针断层扫描和密度泛函理论证明,来自不同二维掺杂层的自由电子聚合成了均匀的三维导体。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a14a/4530340/f2fd1993d9f1/srep12948-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a14a/4530340/3bf7615674ad/srep12948-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a14a/4530340/2609a4e9dd3c/srep12948-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a14a/4530340/f2fd1993d9f1/srep12948-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a14a/4530340/3bf7615674ad/srep12948-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a14a/4530340/2609a4e9dd3c/srep12948-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a14a/4530340/f2fd1993d9f1/srep12948-f3.jpg

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本文引用的文献

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Bottom-up superconducting and Josephson junction devices inside a group-IV semiconductor.在 IV 族半导体中实现的自下而上的超导和约瑟夫森结器件。
Nat Commun. 2014 Jul 2;5:4225. doi: 10.1038/ncomms5225.
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Spontaneous breaking of time-reversal symmetry in strongly interacting two-dimensional electron layers in silicon and germanium.硅和锗中强相互作用二维电子层中时间反演对称性的自发破缺。
Phys Rev Lett. 2014 Jun 13;112(23):236602. doi: 10.1103/PhysRevLett.112.236602.
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Phosphorus molecules on Ge(001): a playground for controlled n-doping of germanium at high densities.
锗(001)表面的磷分子:在高密度下对锗进行可控 n 型掺杂的理想场所。
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Opt Express. 2012 May 7;20(10):11316-20. doi: 10.1364/OE.20.011316.
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Science. 2012 Jan 6;335(6064):64-7. doi: 10.1126/science.1214319.
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Academic and industry research progress in germanium nanodevices.锗纳米器件的学术和工业研究进展。
Nature. 2011 Nov 16;479(7373):324-8. doi: 10.1038/nature10678.
9
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