Hostname: page-component-8448b6f56d-42gr6 Total loading time: 0 Render date: 2024-04-19T03:03:03.548Z Has data issue: false hasContentIssue false

The Structural Evolution of A-SI:H Films Prepared by Pulse Rf Power Modulation with Hydrogen and Helium Dilution

Published online by Cambridge University Press:  10 February 2011

Yeu-Long Jiang
Affiliation:
Department of Electrical Engineering, National Chung Hsing University, Taichung 40227, Taiwan
Min-Chang Lee
Affiliation:
Department of Electrical Engineering, National Chung Hsing University, Taichung 40227, Taiwan
Shieng-Huai Chen
Affiliation:
Department of Electrical Engineering, National Chung Hsing University, Taichung 40227, Taiwan
Get access

Abstract

A-Si:H films were deposited in a PECVD system using 5k to 5 Hz and 25 to 75% duty cycle square-wave pulse modulation RF power and with 80% hydrogen or 80% helium dilution. The transmission and the microstructure of the hydrogen bonding configuration were measured using NIR-VIS-UV and FTIR spectrometers. The powder formation in the reactor chamber was low for a deposition rate less than 5.87 nm/min and was completely suppressed by the 500 Hz pulse RF power with a duty cycle less than 33.3%. The low microstructure R ratio is the result of the reduction of the polymization reaction in the plasma for a low deposition process. A R ratio less than 14% could be obtained using 500 Hz with a duty cycle less than 33.3% for helium dilution or using 5k to 50 Hz with a duty cycle less than 50% for hydrogen dilution. The refractive index of the films is high for the films with low R ratio. The more compact and higher quality films exhibit greater SiH bonding configurations in the a-Si:H films.

Type
Research Article
Copyright
Copyright © Materials Research Society 1998

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

REFERENCES

[1] Shirai, H., Das, D., Hanna, J.I. and Shimizu, I., Appl. Phys. Lett., ’59(9), (1991) p. 1096 Google Scholar
[2] Hsu, K.C., Chang, H., Hong, C.S., and Hwang, H.L., Mat. Res. Soc. Symp. Proc. Vol. 258, (1992), pp. 6974.Google Scholar
[3] Howling, A.A., Hollenstein, Ch., and Paris, P.-J., Appl. Phys. Lett. 59(12)(1991), pp. 14091411.Google Scholar
[4] Overzet, L.J and Verdeyen, J.T., Appl. Phys. Lett. 48(11)(1986), pp. 695697.Google Scholar
[5] Watanabe, Y. et al., Appl. Phys. Lett. 53(14)(1988), pp. 12631265.Google Scholar
[6] Lloret, A. et al., J. Appl. Phys. 69(2) (1991), pp. 632638.Google Scholar
[7] Yoshida, T. et al., Mat. Res. Soc. Symp. Proc. Vol. 219, (1991), pp. 655665.Google Scholar
[8] Howling, A.A., Sansonnens, L., Dorier, J.-L., and Hollenstein, Ch., J. Appl. Phys. Vol. 75(3)(1994) pp. 13401353.Google Scholar
[9] Macarico, A. et al., J. Non-Cryst. Solids 198–200(1996), pp. 12071211.Google Scholar
[10] Cody, G.D. et al., Solar Cells, 2, (1980), p. 231.Google Scholar
[11] Ley, L. in “The Physics of Hydrogenated Amorphous Silicon II,” Joannopoulos, J.D. and Lucovsky, G. eds., Springer-Verlag, Berlin, (1984), p. 231.Google Scholar
[12] Bernsten, A.J.M. et al., Mat. Res. Soc. Symp. Proc. Vol. 258, (1992), pp. 275280.Google Scholar