Effect of ion beam figuring and subsequent antireflective coating deposition on the surface absorption of CaF_2 at 193  nm

2016 ◽  
Vol 56 (4) ◽  
pp. C91 ◽  
Author(s):  
Christian Mühlig ◽  
Simon Bublitz ◽  
Roman Feldkamp ◽  
Helmut Bernitzki
2021 ◽  
Author(s):  
Gyo Wun Kim ◽  
Won Jun Chang ◽  
Ji Eun Kang ◽  
Hee Ju Kim ◽  
Geun Young Yeom

Abstract Even though EUV lithography has the advantage of implenting a finer pattern compared to ArF immersion lithography due to the use of 13.5 nm instead of 193 nm as the wavelengh of the light source, due to the low energy of EUV light source, EUV resist has a thinner thickness than conventional ArF resist. EUV resist having such a thin thickness is more vulnerable to radiation damage received during the etching because of its low etch resistance and also tends to have a problem of low etch selectivity. In this study, the radiation damage to EUV resist during etching of hardmask materials such as Si3N4, SiO2, etc. using CF4 gas was compared between neutral beam etching (NBE) and ion beam etching (IBE). When NBE was used, after the etching of 20 nm thick EUV resist, the line edge roughness (LER) increase and the critical dimension (CD) change of EUV resist were reduced by ~ 1/3 and ~ 1/2, respectively, compared to those by IBE. Also, at that EUV etch depth, the RMS(root mean square) surface roughness value of EUV resist etched by NBE was ~2/3 compared to that by IBE on the average. It was also confirmed that the etching selectivity between SiO2, Si3N4, etc. and EUV resist was higher for NBE compared to IBE. The less damage to the EUV resist and the higher etch selectivity of materials such as Si3N4 and SiO2 over EUV resist for NBE compared to IBE are believed to be related to the no potential energy released by the neutralization of the ions during the etching for NBE.


2012 ◽  
Author(s):  
Weiyuan Guo ◽  
Bin Liang ◽  
Xiankai Cheng ◽  
Yi Zheng
Keyword(s):  
Ion Beam ◽  

2009 ◽  
Author(s):  
M. Ghigo ◽  
S. Cornelli ◽  
R. Canestrari ◽  
D. Garegnani
Keyword(s):  
Ion Beam ◽  

2013 ◽  
Vol 552 ◽  
pp. 142-146
Author(s):  
Yong Qiang Gu

Ion Beam Figure (IBF) is believed to be one of the most effective technics that can fabricate lens with nano or even sub-nano accuracy. For different sizes of IBF removal functions, the correct effects in different spatial frequency range are different. Power Spectral Density (PSD) curve can describe surface errors in full spatial frequency range, so it is a very convenient way to evaluate the quality of lens’ surface. In this paper, firstly, the principles of IBF and PSD are introduced briefly; Secondly, IBF removal functions with sizes from 2 mm to 15 mm are generated. A lens with surface error more than PV value 400nm is simulated with different sizes of IBF removal functions by Lucy-Richardson algorithm. Finally, experiments are done by IBF plant. A lens is fabricated by different sizes of removal functions and the fabricate results are tested by interferometer precisely and calculated to PSD curves. By the comparison of these curves, the IBF fabricate effects with different removal sizes are analyzed, which show that the smaller the removal size, the better the removal effect in higher spatial frequency range, but in the meantime, it will take a much longer time. Also the reasons of the difference between theory simulation and actual fabrication result are taken into account, and several influence factors are analyzed.


Author(s):  
Lin Zhou ◽  
Yi Fan Dai ◽  
Xu Hui Xie ◽  
Chang Jun Jiao ◽  
Sheng Yi Li
Keyword(s):  
Ion Beam ◽  

2020 ◽  
Vol 40 (12) ◽  
pp. 1222001
Author(s):  
宋辞 Song Ci ◽  
田野 Tian Ye ◽  
石峰 Shi Feng ◽  
张坤 Zhang Kun ◽  
沈永祥 Shen Yongxiang

2016 ◽  
Vol 24 (12) ◽  
pp. 2975-2982
Author(s):  
徐明进 XU Ming-jin ◽  
戴一帆 DAI Yi-fan ◽  
解旭辉 XIE Xu-hui ◽  
周 林 ZHOU Lin

1999 ◽  
Author(s):  
Raymond Mercier ◽  
Michel Mullot ◽  
Michel Lamare ◽  
Gerard Tissot

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