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Silicon Delta Doping in GaAs: An Ongoing Enigma

Published online by Cambridge University Press:  26 February 2011

R. C. Newman
Affiliation:
IRC Semiconductor Materials, The Blackett Laboratory, Imperial College of Science, Technology and Medicine, Prince Consort Road, London SW7 2BZ, United Kingdom
M. J. Ashwin
Affiliation:
IRC Semiconductor Materials, The Blackett Laboratory, Imperial College of Science, Technology and Medicine, Prince Consort Road, London SW7 2BZ, United Kingdom
J. Wagner
Affiliation:
Fraunhofer Institut für Angewandte Festkörperphysik, Tullastrasse 72, D-79108 Freiburg, Germany
M. R. Fahy
Affiliation:
IRC Semiconductor Materials, The Blackett Laboratory, Imperial College of Science, Technology and Medicine, Prince Consort Road, London SW7 2BZ, United Kingdom
L. Hart
Affiliation:
IRC Semiconductor Materials, The Blackett Laboratory, Imperial College of Science, Technology and Medicine, Prince Consort Road, London SW7 2BZ, United Kingdom
S. N. Holmes
Affiliation:
IRC Semiconductor Materials, The Blackett Laboratory, Imperial College of Science, Technology and Medicine, Prince Consort Road, London SW7 2BZ, United Kingdom
C. Roberts
Affiliation:
IRC Semiconductor Materials, The Blackett Laboratory, Imperial College of Science, Technology and Medicine, Prince Consort Road, London SW7 2BZ, United Kingdom
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Abstract

Infrared (IR) absorption and Raman scattering are reported from the localized vibrational modes (LVM) of Al and Si δ-layer superlattices in MBE (100) GaAs grown at 400°C as a function of the total areal concentrations, [A1]A and [Si]A respectively. The Al superlattices show the expected behavior on passing from sub-monolayer (ML) to thicker layers (thin AlAs) since the impurities still occupy only Ga-sites. The behavior is very different from that found for Si δ-layers. In addition to SiGa reported previously, we now show that SiAs, SiGa-SiAs pairs and the electron trap Si-X are also present in Si δ-layers and superlattices for 0.05 ≤ [Si]A≤ 0.5 ML. The conductivity of these structures and the concentrations of substitutional Si in GaAs at all sites fall to zero for [Si]A> 0.5 ML but a Raman feature at 470–490 cm−1, attributed to the vibrations of covalent Si-Si bonds is then detected. This feature is not observed in structures containing very closely spaced dilute (0.01 ML) Si δ-planes. It is inferred that long-range Si diffusion does not occur in the bulk crystal, although there could be surface diffusion during Si deposition. The maximum measured carrier concentrations are always less than 2 × 1019 cm−3, the DX limit. The redistribution of Si amongst the various lattice sites is discussed in terms of SiGa DX-like displacements occurring during growth, followed by local thermally activated diffusion jumps. It is speculated that AsGa antisite defects and Ga-vacancies are produced by this process. The reason why the Si δ-layer is non-conducting remains unclear.

Type
Research Article
Copyright
Copyright © Materials Research Society 1995

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References

[1] Köhler, K., Ganser, P. and Maier, M., J. Cryst. Growth 127, 720 (1993).Google Scholar
[2] Maguire, J., Murray, R., Newman, R. C., Beall, R. B. and Harris, J. J., Appl. Phys. Lett 50, 516 (1987).Google Scholar
[3] Murray, R., Newman, R. C., Sangster, M. J. L., Beall, R. B., Harris, J. J., Wright, P. J., Wagner, J. and Ramsteiner, M., J. Appl. Phys. 66, 2589 (1989).Google Scholar
[4] Maude, D. K., Portal, J.C., Murray, R., Foster, T.J., Dmowski, L., Eaves, L., Newman, R.C., Basmaji, P., Gibart, P., Harris, J.J. and Beall, R.B., in Physics of DX-centers in GaAs alloys (Solid State Phenomena 10) ed. J. C. Bourgoin (Liechtenstein Sci.-Tech) p121.Google Scholar
[5] Ogawa, M. and Baba, T., Jpn. J. Appl. Phys. 24, L572 (1985).Google Scholar
[6] Briones, F., Gonzalez, L. and Ruiz, A., Appl. Phys. A49, 729 (1989).Google Scholar
[7] Ramsteiner, M., Wagner, J., Hiesinger, P., Köhler, K. and Rössler, U., J. Appl. Phys. 73, 5023 (1993).Google Scholar
[8] McQuaid, S. M., Newman, R. C., Missous, M. and O’Hagan, S., Appl. Phys. Lett., 61, 3008 (1992); J. Cryst. Growth 127, 515 (1993).Google Scholar
[9] Ploog, K., Hauser, M. and Fischer, A., Appl. Phys. A45, 233 (1988).Google Scholar
[10] Schubert, E. F., J. Vac. Sci. Technol., 8, 2980 (1990).Google Scholar
[11] Harris, J. J., J. Mat.Sci: Materials in Electronics, 4, 93 (1993).Google Scholar
[12] Zrenner, A. and Koch, F., in Properties of Impurity States in Superlattice Semiconductors, ed. Fong, C. Y., Batra, I. P. and Ciraci, S., NATO ASI Series B (1988) Plenum NY) p1.Google Scholar
[13] Ashwin, M. J., Fahy, M. R., Harris, J. J., Newman, R. C., Sansom, D. A., Addinall, R., McPhail, D. S. and Sharma, V. K. M., J. Appl. Phys. 73, 633 (1993).Google Scholar
[14] Clegg, J. B. and Beall, R. B., Suf. Int. Anal. 14, 307 (1989).Google Scholar
[15] Hart, L., Fahy, M. R., Newman, R. C. and Fewster, P. F. Appl. Phys. Lett. 18, 2218 (1993).Google Scholar
[16] Hart, L., Ashwin, M. J., Fewster, P. F., Zhang, X., Fahy, M. R. and Newman, R. C., Semicond. Sci. Technol 10, 32 (1994).Google Scholar
[17] Wagner, J., Newman, R. C. and Roberts, C., unpublished work (1995).Google Scholar
[18] Brandt, O., Crook, G. E., Ploog, K., Wagner, J. and Maier, M., Appl. Phys. Lett. 59, 2730 (1991).Google Scholar
[19] Newman, R. C., Semicond. Sci. Technol. 9, 1749 (1994).Google Scholar
[20] Ashwin, M. J., Fahy, M. R., Hart, L., Newman, R. C. and Wagner, J., J. Appl. Phys. 76, 7627 (1994).Google Scholar
[21] Dewdney, A. J., Holmes, S., Yu, H., Fahy, M. R. and Murray, R., Superlattices and Microstructures 14, 205 (1993).Google Scholar
[22] Tanino, H., Kawanami, H., Matsuhata, H., Appl. Phys. Lett. 60, 1978 (1992).Google Scholar
[23] Jones, R. and Öberg, S., unpublished work (1995).Google Scholar
[24] Wagner, J., Mater. Sci. Forum 65–66, 1 (1990).Google Scholar
[25] Avery, A.R., Holmes, D.H., Sudijono, J.L., Jones, T.S., Fahy, M.R. and Joyce, B.A., J.Cryst. Growth, Proc. MBE VIII, in press (1995).Google Scholar
[26] Chadi, D.J. and Chang, K.J., Phys. Rev. Lett. 61 873 (1988).Google Scholar
[27] Warrren, A.C., Woodhall, J.M., Kirchner, P., Yiu, X., Pollak, F., Melloch, M.R., Otsuka, N. and Mahalingam, K., Phys. Rev. B46, 4617 (1992).Google Scholar
[28] Beall, R. B., Clegg, J. B., Castagné, J., Harris, J. J., Murray, R. and Newman, R. C., Semicond. Sci. Technol. 4, 1171 (1989).Google Scholar
[29] Wolk, J.A., Kruger, M.B., Heyman, J.N., Walukiewicz, W., Jeanloz, R. and Haller, E.E., Phys. Rev. Lett. 66, 774(1991).Google Scholar
[30] Sharma, V.K.M., McPhail, D.S. and Fahy, M.R., Surface and Interface Analysis, in press (1995).Google Scholar