Hostname: page-component-848d4c4894-8bljj Total loading time: 0 Render date: 2024-06-14T15:45:16.572Z Has data issue: false hasContentIssue false

Lattice Disorder Effects on The Vacancy-Oxygen Centre in Ion-Irradiated Silicon

Published online by Cambridge University Press:  15 February 2011

N. Keskitalo
Affiliation:
Uppsala University, Department of Material Science, Electronics, P.O. Box 534, S-751 21 Uppsala, Sweden, niclas.keskitalo@material.uu.se
A. Hallén
Affiliation:
Royal Institute of Technology, Solid State Electronics, P.O. Box E229, S-164 40 Kista-Stockholm
J. Lalita
Affiliation:
Royal Institute of Technology, Solid State Electronics, P.O. Box E229, S-164 40 Kista-Stockholm
B. G. Svensson
Affiliation:
Royal Institute of Technology, Solid State Electronics, P.O. Box E229, S-164 40 Kista-Stockholm
Get access

Abstract

The Vacancy-Oxygen (VO) centre is one of the most prominent defects appearing in silicon after irradiation with energetic particles and gamma rays. It is formed when migrating vacancies are trapped by interstitial oxygen atoms. It gives rise to a deep level in the upper part of the silicon bandgap at 0.164 eV below the conduction band edge that can be conveniently studied by deep level transient spectroscopy (DLTS). It is furthermore a very important defect from a technological point of view since it normally controls the charge carrier lifetimes in silicon power devices at high injection levels.

Various doped n-type float zone Si samples have been irradiated with MeV ions at low doses. DLTS measurements of the charge carrier capture kinetics reveal lower capture rates if heavier ions, i.e. larger collision cascades, have been used to generate the defects. This effect can be interpreted as a local lowering of the Fermi level following lattice disorder in regions with a high elastic energy deposition. It will be shown that the VO is also very sensitive to lattice disorder in a similar way as previously reported for the divacancy centre.

In the DLTS spectra another defect, originating from an interstitial-carbon—substitutional-carbon pair (Cj-Cs), overlaps with the VO-peak. The Ci-Cs pair has been observed to posses bistable properties and in this paper we will further elucidate the various contributions from the two defects to the Ec-0.164 eV peak. In particular, the temperature dependence of the electron capture cross section of the Cj-Cs level will be discussed.

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

REFERENCES

[1] Watkins, G. D. and Corbett, J. W., Phys. Rev. 121, pp. 10011014 (1961).Google Scholar
[2] Hallén, A., Keskitalo, N., Masszi, F., and Nágl, V., J. Appl. Phys. 79, pp. 39063914 (1996).Google Scholar
[3] Bleichner, H., Jonsson, P., Keskitalo, N., and Nordlander, E., J. Appl. Phys. 79, pp. 91429148 (1996).Google Scholar
[4] Keskitalo, N., Jonsson, P., Nordgren, K., Bleichner, H., and Nordlander, E., Submitted to J. Appl. Phys., pp.Google Scholar
[5] Cheng, L. J., Corelli, J. C., Corbett, J. W., and Watkins, G. D., Phys. Rev. 152, pp. 761774 (1966).Google Scholar
[6] Keskitalo, N., Hallén, A., Josyula, L., and Svensson, B. G., Nucl. Instr. Meth. B, in press.Google Scholar
[7] Svensson, B. G., Mohadjeri, B., Hallén, A., Svensson, J. H., and Corbett, J. W., Phys. Rev. B 43, pp. 22922298 (1991).Google Scholar
[8] Brotherton, S. D. and Bradley, P., J. Appl. Phys. 53, pp. 57205732 (1982).Google Scholar
[9] Song, L. W., Zhan, X. D., Benson, B. W., and Watkins, G. D., Phys. Rev. B 42, pp. 57655783 (1990).Google Scholar
[10] Song, L. W., Benson, B. W., and Watkins, G. D., Appl. Phys. Lett. 51, pp. 11551157 (1987).Google Scholar
[11] Jellison, J. G. E., J. Appl. Phys. 53, pp. 57155719 (1982).Google Scholar
[12] Keskitalo, N., Hallén, A., Masszi, F., and Olsson, J., Solid-St. Electron. 39, pp. 10871092 (1996).Google Scholar
[13] Hallén, A., Ingemarsson, P. A., Håkansson, P., Sundqvist, B. U. R., and Possnert, G., Nucl. Instr. and Meth. B36, pp. 345349 (1989).Google Scholar
[14] Ferenczi, G., Krispin, P., and Somogyi, M., J. Appl. Phys. 54, pp. 39023912 (1983).Google Scholar
[15] Kimerling, L. C., Institute of Physics Conference series, (1976) p. 221230.Google Scholar
[16] Pons, D., J. Appl. Phys. 55, pp. 36443657 (1984).Google Scholar
[17] Laiita, J., Svensson, B. G., Jagadish, C., and Hallén, A., Nucl. Instr. Meth. B, in press.Google Scholar
[18] Davies, L. W., Proceedings of the IEEE, (1963) p. 16371642.Google Scholar