硬x射线光刻中衬底光电子的蒙特卡罗模拟及缓冲层的影响

In-Beom Park, O. Kim
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引用次数: 0

摘要

由于硬x射线光刻比软x射线波长更短,分辨率更高,因此硬x射线光刻技术被引入到50纳米及以上一代(Khan等人,1999年)。在硬x射线光刻中,光电子模糊增加是因为在电阻-衬底界面产生更多的光电子和俄歇电子,并且随着光子能量从软x射线到硬x射线的增加,抗蚀剂的光吸收减少。这种模糊,由于二次电子在线的边缘,被认为是造成图案退化。本文基于Murata的模型(Murata et al, IEEE Trans)对平均能量为2.36 keV的硬谱进行了光电子和俄格电子的蒙特卡罗模拟。电子发展vol. ED-32, p. 1694, 1985)和徐等人的工作(J. Vac。科学。抛光工艺。B卷,第18卷,no。6,第3349页,2000年)。计算并绘制了在W和Si衬底上无缓冲层和在W衬底上有不同厚度(Si/sub 3/N/sub 4/和SiO/sub 2/)缓冲层的200 nm厚tdurn - n908抗蚀剂和衬底之间200,000光子的能量损失密度和电子轨迹。缓冲层为10 nm缓冲层(10 nm Si/sub 3/N/sub 4/), 30 nm缓冲层(10 nm Si/sub 3/N/sub 4/+20 nm SiO/sub 2/)和70nm缓冲层(10 nm Si/sub 3/N/sub 4/+60 nm SiO/sub 2/)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Monte Carlo simulation of substrate photoelectrons in hard X-ray lithography and the effect of buffer layer
Hard X-ray lithography was introduced for 50 nm generation and beyond due to its shorter wavelength and higher resolution than the soft X-ray (Khan et al, 1999). Photoelectron blur increases in hard X-ray lithography because more photo and Auger electrons are generated at the resist-substrate interface and the resist photoabsorption decreases as photon energy increases from soft X-ray to hard X-ray. This blur, due to secondary electrons at the line edge, is considered to cause pattern degradation. In this paper, Monte Carlo simulation of photo and Auger electrons for this harder spectrum of 2.36 keV average energy was carried out based on Murata's model (Murata et al, IEEE Trans. Electron Dev. vol. ED-32, p. 1694, 1985) and the work of Seo et al (J. Vac. Sci. Technol. B vol. 18, no. 6, p. 3349, 2000). Energy loss density and electron trajectories for 200,000 photons were calculated and plotted in a 200 nm thick TDUR-N908 resist on a W and Si substrate without a buffer layer and with buffer layers of various thickness (Si/sub 3/N/sub 4/ and SiO/sub 2/) on a W substrate between resist and substrate. The buffer layers are 10 nm buffer (10 nm Si/sub 3/N/sub 4/), 30 nm buffer (10 nm Si/sub 3/N/sub 4/+20 nm SiO/sub 2/) and 70nm buffer (10 nm Si/sub 3/N/sub 4/+60 nm SiO/sub 2/).
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