Hostname: page-component-cd9895bd7-q99xh Total loading time: 0 Render date: 2024-12-27T01:48:09.470Z Has data issue: false hasContentIssue false

The Applicability of Fluorinated Silicon Nitride Film As Bottom Antireflective Layer In Deep Ultraviolet Lithography

Published online by Cambridge University Press:  10 February 2011

Jun Byung-Hyuk
Affiliation:
Department of Materials Science & Engineering, Korea Advanced Institute of Science and Technology, Taejon, 305-701, Korea
Han Sang-Soo
Affiliation:
Department of Materials Science & Engineering, Korea Advanced Institute of Science and Technology, Taejon, 305-701, Korea
Kim Dong-Wan
Affiliation:
Semiconductor R/D center, Samsung Electronics Co. Ltd., Yongin, 449-900, Korea
Kang Ho-Young
Affiliation:
Semiconductor R/D center, Samsung Electronics Co. Ltd., Yongin, 449-900, Korea
Koh Young-Bum
Affiliation:
Semiconductor R/D center, Samsung Electronics Co. Ltd., Yongin, 449-900, Korea
Bae Byeong-Soo
Affiliation:
Semiconductor R/D center, Samsung Electronics Co. Ltd., Yongin, 449-900, Korea
No Kwangsoo
Affiliation:
Department of Materials Science & Engineering, Korea Advanced Institute of Science and Technology, Taejon, 305-701, Korea
Get access

Abstract

This study describes the use of fluorinated silicon nitride film as a bottom antireflective layer (BARL) material suitable for line-patterning in quarter-micron KrF excimer laser lithography. For the structures of photoresist/BARL (300Å)/c-Si and photoresist/BARL (300 Å )/W-Si at a wavelength of 248nm, 0% reflectance could be achieved when the refractive index (n) and extinction coefficient (k) values of the film are 2.11 and 0.68 or 2.05 and 0.59, respectively. The fluorinated silicon nitride thin films on p-type (100) Si substrates obtained by inductively coupled plasma enhanced CVD have been evaluated with the variations of NF3 flow rates under the two conditions of SiH4:N2=2:15 and 3:20 (seem). The films optical constants and reflectance were investigated by spectroscopic ellipsometry combined with a reflectance simulation program. The film n and k values at 248nm vary in the ranges of 1.67~2.35 and 0.01~0.69, respectively, depending on gas flow ratio of SiH4:N2:NF3. Low reflectance of below 5% can be obtained from reflectance simulation for two deposition conditions with a BARL thickness of 300Å. In addition, the reflectance could be reduced to almost 0% by controlling film thickness. Finally, the antireflective layer performance was investigated using KrF excimer laser lithography.

Type
Research Article
Copyright
Copyright © Materials Research Society 1997

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

1 Jain, K., Excimer Laser Lithography. (SPIE Optical Engineering Press, Bellingham, 1990).Google Scholar
2 Fahey, J., Moreau, W., Welsh, K., Miura, S., Eib, N., Spinillo, G. and Sturtevant, J. in Advances in Resist Technology and Processing XI. edited by Nalamasu, O. (SPIE Proc, 2195, San Jose, California, 1994) p. 422.Google Scholar
3 Suda, Y., Motoyama, T., Harada, H. and Kanazawa, M. in Optical/Laser Microlithography V. edited by Cothbert, John D. (SPIE Proc. 1674, San Jose, California, 1992) p. 350.Google Scholar
4 Ogawa, T., Kimura, M., Gotyo, T., Tomo, Y. and Tsumori, T. in Optical/Laser Microlithography. edited by Cothbert, John D. (SPIE Proc. 1927, San Jose, California, 1993) p. 263.Google Scholar
5 Jun, B-H. et al. , Appl. Opt. (1996, accepted).Google Scholar
6 Lieberman, M. A. and Lichtenberg, A. J., Principles of Plasma Discharges and Materials Processing. (John Wiley & Sons, Inc., New York, 1994), p. 387.Google Scholar
7 Macleod, H. A., Thin-Film Optical Filters. 2nd ed. (Macmillan Publishing Company, New York, 1986), p.11.Google Scholar
8 Jun, B-H. et al. , Thin Solid Films (1996, submitted).Google Scholar