Hostname: page-component-586b7cd67f-t8hqh Total loading time: 0 Render date: 2024-11-29T07:51:31.730Z Has data issue: false hasContentIssue false

Hydrogen Diffusion in Undoped and B-Doped a-Si1-xCx:H

Published online by Cambridge University Press:  16 February 2011

R. Shinar
Affiliation:
Microelectronics Research Center, Iowa State University, AMes, Iowa 50011
J. Shinar
Affiliation:
Ames Laboratory - USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011
G. Subramania
Affiliation:
Ames Laboratory - USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011
H. Jia
Affiliation:
Ames Laboratory - USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011
S. Sankaranarayanan
Affiliation:
Ames Laboratory - USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011
M. Leonard
Affiliation:
Microelectronics Research Center, Iowa State University, AMes, Iowa 50011
V. L. Dalai
Affiliation:
Microelectronics Research Center, Iowa State University, AMes, Iowa 50011 Department of Electrical and Computer Engineering, Iowa State University, Ames, IA 50011
Get access

Abstract

A deuterium secondary ion mass spectrometry (SIMS) study of hydrogen diffusion in undoped and boron-doped a-Si0.86C0.4:H deposited by an electron cyclotron resonance plasma is described. The undoped films deposited at 250°C clearly indicated deuterium-hydrogen interdiffusion at T ≥ 350°C. The dispersion parameter a of the power-law time dependent diffusion constant D = D00t)−α decreased from ∼0.3 at T = 350 and 400°C to ∼0.1 at 450°C, and the activation energy for a diffusion length of 1000 Å was ∼1.0 eV. These results are discussed in relation to previous studies of a-Si:H. The diffusion in ∼0.2 and ∼0.6 at.% B-doped a-Si0.86C0.14:H sharply differs from that in B-doped a-Si:H, where an enhancement of up to ∼103 was previously observed. In doped a-Si0.86C0.14:H, the diffusion of most of the H atoms is strongly suppressed, but a small fraction undergoes fast diffusion. IR Measurements indicate that the B-doping reduces the bulk-like Si-H stretch vibration at ∼2000 cm1. Upon annealing, the Si-CHn and C-H wag modes at ∼780 and ∼1000 cm−1, resp., increase, while the 640 and ∼2000 cm1 Si-H wag and stretch modes, resp., weaken, indicating transfer of hydrogen from Si- to C-bonds, in which the H atoms are apparently deeply trapped. As in a-Si:H, the fast diffusion component is apparently due to carrier recombination-enhanced weak Si-Si bond breaking. The results suggest that B-doping also induces microvoids and enhances the rate of breaking of weak Si-C bonds, leading to enhanced trapping of H.

Type
Research Article
Copyright
Copyright © Materials Research Society 1994

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. Li, Y.-M., in Amorphous Silicon Technology - 1993, edited by Schiff, E., Thompson, M. J., Madan, A., Tanaka, K., and LeComber, P. G. (Mat. Res. Soc. Proc. 297, Pittsburgh, PA, 1993), p. 803 and references therein.Google Scholar
2. Eberhardt, K., Lotter, E., Heintze, M., and Bauer, G. H., in Amorphous Silicon Technology - 1992, edited by Thompson, M. J., Hamakawa, Y., LeComber, P. G., Madan, A., and Schiff, E. (Mat. Res. Soc. Proc. 258, Pittsburgh, PA, 1992), p. 673.Google Scholar
3. Street, R. A., Tsai, C. C., Kakalios, J., and Jackson, W. B., Phil. Mag. B 56, 305 (1987).Google Scholar
4. Jackson, W. B. and Kakalios, J., in Amorphous Silicon and Related Materials, edited by Fritzsche, H., p. 247 (World Scientific, NY, 1988), and references therein.Google Scholar
5. Kakalios, J., Street, R.A., and Jackson, W.B., Phys. Rev. Lett. 59, 1037 (1987).Google Scholar
6. Jackson, W.B., Phys. Rev. B 38, 3595 (1988).CrossRefGoogle Scholar
7. Shinar, J., Shinar, R., Mitra, S., and Kim, J.Y., Phys. Rev. Lett. 62, 2001 (1989).Google Scholar
8. Mitra, S., Shinar, R., and Shinar, J., Phys. Rev. B 42, 6746 (1990).Google Scholar
9. Tang, X.-M., Weber, J., Baer, Y., and Finger, F., Phys. Rev. B 42, 7277 (1990).Google Scholar
10. Shinar, J., Shinar, R., Wu, X.-L., Mitra, S., and Girvan, R. F., Phys. Rev. B 43, 1631 (1991).Google Scholar
11. Shinar, R., Shinar, J., Jia, H., and Wu, X.-L., Phys. Rev. B 47, 9361 (1993).CrossRefGoogle Scholar
12. Beyer, W., Herion, J., Wagner, H., and Zastrow, U., in Amorphous Silicon Technology -1991, edited by Madan, A., Hamakawa, Y., Thompson, M. J., Taylor, P. C., and LeComber, P. G. (Mat. Res. Soc. Proc. 219, Pittsburgh, PA, 1991), p. 81.Google Scholar
13. Knox, R. D., Dalai, V. L., Moradi, B., and Chumanov, G., J. Vac. Sci. Tech. A 11, 1896 (1993).Google Scholar
14. Branz, H. M., Asher, S. E., and Nelson, B. P., Phys. Rev. B 47, 7061 (1993).CrossRefGoogle Scholar
15. Santos, P. V., Johnson, N. M., Street, R. A., Hack, M., Thompson, R., and Tsai, C. C., Phys. Rev. B 47, 10244 (1993).CrossRefGoogle Scholar
16. Shinar, R. et al., unpublished results.Google Scholar
17. Fritzsche, H. and Deng, X.-M., Bull. Am. Phys. Soc. 35, 349 (1990)Google Scholar