Charge-induced pattern displacement in E-beam lithography

被引:14
作者
Arat, Kerim T. [1 ]
Klimpel, Thomas [2 ]
Zonnevylle, Aernout C. [3 ]
Ketelaars, Wilhelmus S. M. M. [3 ]
Heerkens, Carel Th. H. [1 ]
Hagen, Cornelis W. [1 ]
机构
[1] Delft Univ Technol, Fac Appl Sci, Lorentzweg 1, NL-2628 CJ Delft, Netherlands
[2] GenISys GmbH, Eschenstr 66, D-820249 Taufkirchen, Germany
[3] Raith BV, Dintel 27a, NL-5684 PS Best, Netherlands
来源
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B | 2019年 / 37卷 / 05期
关键词
RESOLUTION LIMITS; RADIATION-DAMAGE; ELECTRON; POLYMETHYLMETHACRYLATE;
D O I
10.1116/1.5120631
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
Electron beam lithography (EBL) requires conducting substrates to ensure pattern fidelity. However, there is an increasing interest in performing EBL on less well-conducting surfaces or even insulators, usually resulting in seriously distorted pattern formation. To understand the underlying charging phenomena, the authors use Monte Carlo simulations that include models for substrate charging, electron beam-induced current, and electric breakdown. Simulations of electron beam exposure of glass wafers are presented, exposing regular patterns which become distorted due to charge-induced beam deflection. The resulting displacements within the patterns are mapped and compared to experimental displacement maps obtained from patterns in PMMA resist on glass substrates. Displacements up to several hundreds of nanometers were observed at a primary beam energy of 50 keV. Also, various scan strategies were used to write the patterns, in the simulations as well as the experiments, revealing their strong effect on pattern distortion, in shape and in magnitude. A qualitative, in some cases even quantitative, good agreement was found between the simulations and the experiments, providing enough confidence in Monte Carlo simulations to predict charge-induced pattern displacement and shape distortion and to find smart scan strategies to minimize the effects of charging. Published by the AVS.
引用
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页数:10
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