Hostname: page-component-586b7cd67f-2brh9 Total loading time: 0 Render date: 2024-12-01T07:19:58.253Z Has data issue: false hasContentIssue false

ESR Study of Crystallization of Hydrogenated Amorphous Silicon Thin Films

Published online by Cambridge University Press:  01 February 2011

Tining Su
Affiliation:
[email protected], Colorado School of Mines, Physics, 1523 Illinois Street, Golden, CO, 80401, United States
Tong Ju
Affiliation:
[email protected], University of Utah, Department of Physics, Salt Lake City, UT, 84112, United States
P. Craig Taylor
Affiliation:
[email protected], Colorado School of Mines, Department of Physics, Golden, CO, 80401, United States
Pauls Stradins
Affiliation:
[email protected], National Renewable Energy Laboratory, Golden, CO, 80401, United States
Yueqin Xu
Affiliation:
[email protected], National Renewable Energy Laboratory, Golden, CO, 80401, United States
Falah Hasoon
Affiliation:
[email protected], National Renewable Energy Laboratory, Golden, CO, 80401, United States
Qi Wang
Affiliation:
[email protected], National Renewable Energy Laboratory, Golden, CO, 80401, United States
Walter A. Harrison
Affiliation:
[email protected], Stanford University, Department of Applied Physics, Stanford, CA, 94305, United States
Get access

Abstract

Solid-phase crystallization and the subsequent re-hydrogenation of the amorphous silicon thin films provides a low cost approach for thin-film crystalline Si:H-based photovoltaic devices. During the hydrogen effusion, significant lattice reconstruction occurs, as hydrogen is driven out of the film, accompanied by creation and migration of a large number of dangling bonds. We used electron-spin-resonance (ESR) to study evolution of the local order surrounding these dangling bonds during crystallization. When samples made by both plasma enhanced chemical vapor deposition (PECVD) and the and hot wire CVD (HWCVD) are heated to 560°C, hydrogen effuses within 30 min, giving rise to H-effused defect densities of about 5x1018 cm-3. Further heating at 560°C results in crystallizati°n in the HWCVD sample after about 200 min. On the other hand, PECVD samples crystallize only when heated up to 580°C, and then only after much longer times (Dt ~ 1300 min) [1,2]. ESR defects in both samples persist at the 5x1018 cm-3 level as long as the sample remains amorphous during the grain nucleation period. As the crystallites appear, the defect densities gradually decrease and saturate at about 3x1017 cm-3 as the crystallization is completed, both in HWCVD and PECVD samples.

In the H-effused states before crystallization, the ESR signals for both the HWCVD and PECVD samples show significant exchange-narrowing, suggesting that the defects are probably clustered. As the sample crystallizes, the defect clustering largely disappears, yet the line-widths in fully crystallized films are somewhat narrower than those in typical micro-crystalline silicon thin films as reported earlier [3]. This difference is probably due the specific structures of the grain boundaries in the present study. The effect of re-hydrogenation on both the H-effused amorphous and crystallized states will be discussed.

Type
Research Article
Copyright
Copyright © Materials Research Society 2007

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 Stradins, P., Young, D., , Y, , Yan, Iwaniczko, E., Xu, Y., Reedy, R., Branz, H. M., and Wang, Q.; Appl. Phys. Lett. 89, 121921, (2006).Google Scholar
2 Young, D. L., Stradins, P., Xu, Y., Gedvilas, L., Reedy, R., Mahan, A. H., Branz, H. M., Wang, Q., and Williamson, D. L., Appl. Phys. Lett, 89, 161910 (2006).Google Scholar
3 Lima, M. M. de Jr Taylor, P. C., Morrison, S., LeGeune, A., and Marques, F. C., Phys. Rev. B 65, 235324–1 (2002). (And references therein)Google Scholar
4 Brodsky, M. H., Title, R. S., Weiser, K., and Pettit, G. D., Phys. Rev. B 1, 2632 (1970).Google Scholar
5 Whitaker, J., Viner, J., Zukotynski, S., Johnson, E., Taylor, P. C., Stradins, P., Tritium Induced Defects in Amorphous Silicon, in Amorphous and Nanocrystalline Silicon Science and Technology—2004, edited by Ganguly, Gautam, Kondo, Michio, Schiff, Eric A., Carius, Reinhard, and Biswas, Rana (Mater. Res. Soc. Symp. Proc. 808, Warrendale, PA, 2004), A2.3.Google Scholar
6 Ju, T., Whitacker, J., Zukotynski, S., Kherani, N., Taylor, P. C., Stradins, P. (To be published).Google Scholar
7For example see, Vleck, J. H. Van, Phys. Rev. 74, 1168 (1948); P. W. Anderson and P. R. Weiss, Rev. Mod. Phys. 25, 269 (1953).Google Scholar
8Elementary Electronic Structures”, Harrison, W. A., (World Scientific Publishing Con. Singapore, Singapore, 2004).Google Scholar