Hostname: page-component-586b7cd67f-t8hqh Total loading time: 0 Render date: 2024-11-29T07:22:25.682Z Has data issue: false hasContentIssue false

Properties and Application of Undoped Hydrogenated Microcrystalline Silicon Thin Films

Published online by Cambridge University Press:  25 February 2011

J. Kanicki
Affiliation:
IBM Research Division, Thomas J. Watson Research Center, Yorktown Heights, N.Y, 10598;
E. Hasan
Affiliation:
Department of Materials Science and Engineering, MIT, Cambridge, MA 02139
D. F. Kotecki
Affiliation:
IBM General Technology Division, Hopewell Junction, N.Y, 12533
T. Takamori
Affiliation:
IBM Research Division, Thomas J. Watson Research Center, Yorktown Heights, N.Y, 10598;
J. H. Griffith
Affiliation:
IBM Research Division, Thomas J. Watson Research Center, Yorktown Heights, N.Y, 10598;
Get access

Abstract

Device quality undoped hydrogenated microcrystalline silicon has been prepared by plasma enhanced chemical vapor deposition under different conditions. The dependence of physical, chemical, structural, and electrical properties on the deposition conditions has been investigated. Conductive (conductivity above 10−3Ω−1 cm−1) and resistive (conductivity around 10−9Ω−1cm−1) layers having approximately the same grain size, at a given substrate temperature, have been deposited between 200 and 500°C at two different hydrogen dilutions. Independently of the hydrogen dilution, the average grain sized is dependent on the deposition temperature and the film thickness; and a maximum average grain size of about 40 nm has been achieved for a thick film deposited at 500°C. The density of paramagnetic defects also increases with increasing deposition temperature, which indicates that more dangling bond defects are introduced as the total area of the grain boundaries increases. The etch rate decreases with increasing deposition temperature, and for the films deposited at 250 and 500°C the etch rate has been measured to be 6.6 and 2.7 nm/min, respectively. Thin film transistors incorporating a microcrystalline channel have been fabricated and evaluated. The best device had the following properties: field effect mobility, threshold voltage, and on/off current ratio of about 0.8 cm2/V sec, below 5 V, and around 106, respectively.

Type
Research Article
Copyright
Copyright © Materials Research Society 1989

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. Matsuda, A., J. Non Cryst. Solids, 59&60, 767 (1983).Google Scholar
2. Veprek, S., Iqbal, Z., Kuhne, R.O., Capezzuto, P., Sarott, F.A. and Gimzewski, J.K., J. Phys. C: Solid State Phys., 16, 6241 (1983).Google Scholar
3. Mishima, Y., Miyazaki, S., Hirose, M. and Osaka, Y., Philos. Mag. B, 46, 1 (1982).Google Scholar
4. Moustakas, T.D., Weitz, D.A., Prestridge, E.B. and Friedman, R., Mat. Res. Soc. Symp. Proc., 38, 401 (1985).Google Scholar
5. Spear, W.E., Willeke, G. and LeComber, P.G., Physica, 117B & 118B, 908 (1983).Google Scholar
6. Shibata, N., Fukuda, K., Ohtoshi, H., Hanna, J., Oda, S. and Shimizu, I., Jpn. J. Appl. Phys., 26, L10 (1987).Google Scholar
7. Iqbal, Z. and Veprek, S., J. Phys. C: Solid State Phys., 15, 377 (1982).Google Scholar
8. Kanicki, J., Hasan, E., Griffith, J., Takamori, T. and Tsang, J.C. (this volume).Google Scholar
9. Lustig, N. and Kanicki, J., J. Appl. Phys., 65, 3951 (1989).CrossRefGoogle Scholar
10. The ESR measurements were done by Jousse, Dr. D. (personal communication of the unpublished data).Google Scholar
11. Miyazaki, S., Osaka, Y. and Hirose, M., Solar Energy Mat., 11, 85 (1984).Google Scholar