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带电粒子单纳米制造。

Charged particle single nanometre manufacturing.

作者信息

Prewett Philip D, Hagen Cornelis W, Lenk Claudia, Lenk Steve, Kaestner Marcus, Ivanov Tzvetan, Ahmad Ahmad, Rangelow Ivo W, Shi Xiaoqing, Boden Stuart A, Robinson Alex P G, Yang Dongxu, Hari Sangeetha, Scotuzzi Marijke, Huq Ejaz

机构信息

Oxford Scientific Consultants Ltd, 67 High Street, Dorchester-on-Thames, OX10 7HN, UK.

Department of Imaging Physics, Delft University of Technology, Lorentzweg 1, 2628 CJ Delft, Netherlands.

出版信息

Beilstein J Nanotechnol. 2018 Nov 14;9:2855-2882. doi: 10.3762/bjnano.9.266. eCollection 2018.

DOI:10.3762/bjnano.9.266
PMID:30498657
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6244241/
Abstract

Following a brief historical summary of the way in which electron beam lithography developed out of the scanning electron microscope, three state-of-the-art charged-particle beam nanopatterning technologies are considered. All three have been the subject of a recently completed European Union Project entitled "Single Nanometre Manufacturing: Beyond CMOS". Scanning helium ion beam lithography has the advantages of virtually zero proximity effect, nanoscale patterning capability and high sensitivity in combination with a novel fullerene resist based on the sub-nanometre C molecule. The shot noise-limited minimum linewidth achieved to date is 6 nm. The second technology, focused electron induced processing (FEBIP), uses a nozzle-dispensed precursor gas either to etch or to deposit patterns on the nanometre scale without the need for resist. The process has potential for high throughput enhancement using multiple electron beams and a system employing up to 196 beams is under development based on a commercial SEM platform. Among its potential applications is the manufacture of templates for nanoimprint lithography, NIL. This is also a target application for the third and final charged particle technology, viz. field emission electron scanning probe lithography, FE-eSPL. This has been developed out of scanning tunneling microscopy using lower-energy electrons (tens of electronvolts rather than the tens of kiloelectronvolts of the other techniques). It has the considerable advantage of being employed without the need for a vacuum system, in ambient air and is capable of sub-10 nm patterning using either developable resists or a self-developing mode applicable for many polymeric resists, which is preferred. Like FEBIP it is potentially capable of massive parallelization for applications requiring high throughput.

摘要

在简要回顾电子束光刻技术如何从扫描电子显微镜发展而来的历史之后,我们将探讨三种最先进的带电粒子束纳米图案化技术。这三种技术均是最近完成的一个名为“单纳米制造:超越CMOS”的欧盟项目的研究对象。扫描氦离子束光刻技术具有几乎零邻近效应、纳米级图案化能力和高灵敏度等优点,同时还结合了一种基于亚纳米级C分子的新型富勒烯抗蚀剂。目前实现的散粒噪声限制最小线宽为6纳米。第二种技术是聚焦电子诱导加工(FEBIP),它使用喷嘴喷射的前驱体气体在纳米尺度上进行蚀刻或沉积图案,无需抗蚀剂。该工艺利用多电子束有提高通量的潜力,并且基于商业扫描电子显微镜平台正在开发一种采用多达196束电子束的系统。其潜在应用包括制造纳米压印光刻(NIL)的模板。这也是第三种也是最后一种带电粒子技术,即场发射电子扫描探针光刻(FE-eSPL)的目标应用。它是从扫描隧道显微镜发展而来的,使用的是较低能量的电子(几十电子伏特,而不是其他技术的几十千电子伏特)。它具有相当大的优势,即在环境空气中无需真空系统即可使用,并且能够使用可显影抗蚀剂或适用于许多聚合物抗蚀剂的自显影模式进行亚10纳米图案化,后者更为可取。与FEBIP一样,它在需要高通量的应用中也具有大规模并行化的潜力。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/30442f463550/Beilstein_J_Nanotechnol-09-2855-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/f6b7524558ad/Beilstein_J_Nanotechnol-09-2855-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/5edb2decd8a1/Beilstein_J_Nanotechnol-09-2855-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/3715674658d0/Beilstein_J_Nanotechnol-09-2855-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/104adc780634/Beilstein_J_Nanotechnol-09-2855-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/2ea944cd0428/Beilstein_J_Nanotechnol-09-2855-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/a6841037aaac/Beilstein_J_Nanotechnol-09-2855-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/940a3896dcc3/Beilstein_J_Nanotechnol-09-2855-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/bec08d5660ea/Beilstein_J_Nanotechnol-09-2855-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/30442f463550/Beilstein_J_Nanotechnol-09-2855-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/f6b7524558ad/Beilstein_J_Nanotechnol-09-2855-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/5edb2decd8a1/Beilstein_J_Nanotechnol-09-2855-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/3715674658d0/Beilstein_J_Nanotechnol-09-2855-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/104adc780634/Beilstein_J_Nanotechnol-09-2855-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/2ea944cd0428/Beilstein_J_Nanotechnol-09-2855-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/a6841037aaac/Beilstein_J_Nanotechnol-09-2855-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/940a3896dcc3/Beilstein_J_Nanotechnol-09-2855-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/bec08d5660ea/Beilstein_J_Nanotechnol-09-2855-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/6244241/30442f463550/Beilstein_J_Nanotechnol-09-2855-g012.jpg

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