Home Development and performance of EUV pellicles
Article
Licensed
Unlicensed Requires Authentication

Development and performance of EUV pellicles

  • Derk Brouns EMAIL logo
Published/Copyright: June 8, 2017
Become an author with De Gruyter Brill

Abstract

In a lithography process, an image on a mask (reticle) is projected onto a wafer. Continuous decrease in feature sizes also led to a reduction in the wavelength used for exposing. The next step is the move from 193-nm light to extreme ultra-violet (EUV) at 13.5 nm. This poses a lot of challenges that have been overcome in the past years. One of these challenges is the protection of the reticle from front side defects. This protection can be achieved by the use of an EUV pellicle. This is a thin membrane that protects particles from landing on the reticle surface, as will be explained in more detail later. With multiple semiconductor manufacturers preparing for volume EUV manufacturing, the need for a volume production-ready pellicle solution is here today. This article gives an overview of the performance of the current EUV pellicle solution and the status of the development of future EUV pellicles.

References

[1] A. Pirati, Proc. SPIE 9776-10 (2016).Search in Google Scholar

[2] B. Turkott, EUVL Readiness for High Volume Manufacturing, (keynote speech, EUVL Hiroshima, 2016).Search in Google Scholar

[3] D. Brouns, Proc. SPIE 9776-71 (2016).Search in Google Scholar

[4] D. Brouns, Proc. SPIE 9985-9 (2016).10.1117/12.2239882Search in Google Scholar

[5] Y. Ono, Proc. SPIE 9985-10 (2016).10.1117/12.2241393Search in Google Scholar

[6] B. Turkott, Proc. SPIE, 9776-1 (2016).Search in Google Scholar

[7] L. Scaccabarozzi, Proc. SPIE 8679, 867904 (2013).10.1117/12.2015833Search in Google Scholar

[8] C. Zoldesi, in Proc. SPIE 9048 90481N (April 17, 2014). doi: 10.1117/12.2049276.10.1117/12.2049276Search in Google Scholar

[9] M. van de Kerkhof, Proc. SPIE 10143, Extreme Ultraviolet (EUV) Lithography VIII, 101430D (24 March 2017); doi: 10.1117/12.2258025.10.1117/12.2258025Search in Google Scholar

[10] Y. A. Shroff, Proc. SPIE 6151, 615104 (2006).10.1117/12.656551Search in Google Scholar

[11] Y. A. Shroff, M. Leeson, P.-Y. Yan, E. Gullikson and F. Salmassi, J. Vac. Sci. Technol. B 28(4), C6E36–41 (2010).10.1116/1.3505126Search in Google Scholar

[12] S. Akiyama and Y. Kubota, in Int. EUVL Symposium Proceedings Vol. 1, p. 1435, (Prague, 2009).Search in Google Scholar

[13] F. Dhalluin, Proc. SPIE 9658, 96580J (2015). doi: 10.1117/12.2197454.10.1117/12.2197454Search in Google Scholar

[14] L. Sjmaenok, in 2012 International Workshop on EUV and Soft X-Ray Sources, October 8–11, 2012, Dublin, Ireland.Search in Google Scholar

[15] C. Zoldesi, EUV Pellicle complete solution, (EMLC, 2015).Search in Google Scholar

[16] M. Nasalevich, in Proc. SPIE 10032, 32nd European Mask and Lithography Conference, 100320L (October 20, 2016).10.1117/12.2255040Search in Google Scholar

[17] I. Pollentier, Proc. SPIE 9776-72 (2016).10.1117/12.2220031Search in Google Scholar

[18] D. Goldfarb, Proc. SPIE 9776-74 (2016).Search in Google Scholar

[19] D. Goldfarb, Proc. SPIE 9635-9 (2015).10.1117/12.2196901Search in Google Scholar

[20] D. Goldfarb, Proc. SPIE, 9776–54 (2016).10.1117/12.2218453Search in Google Scholar

[21] P.-J. van Zwol, J. Appl. Phys. 118 213107 (2015), doi: 10.1063/1.4936851.10.1063/1.4936851Search in Google Scholar

Received: 2017-3-24
Accepted: 2017-4-21
Published Online: 2017-6-8
Published in Print: 2017-6-27

©2017 THOSS Media & De Gruyter, Berlin/Boston

Downloaded on 2.10.2025 from https://www.degruyterbrill.com/document/doi/10.1515/aot-2017-0023/html
Scroll to top button