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X-ray Topography Studies of Relaxation during the Homo-Epitaxy of 4H-SiC

Published online by Cambridge University Press:  06 February 2015

H. Wang
Affiliation:
Department of Materials Science and Engineering, Stony Brook University, Stony Brook NY 11794-2275, U.S.A.
M. Dudley
Affiliation:
Department of Materials Science and Engineering, Stony Brook University, Stony Brook NY 11794-2275, U.S.A.
J. Zhang
Affiliation:
Dow Corning Compound Semiconductor Solutions, Midland, Michigan, USA 48686
B. Thomas
Affiliation:
Dow Corning Compound Semiconductor Solutions, Midland, Michigan, USA 48686
G. Chung
Affiliation:
Dow Corning Compound Semiconductor Solutions, Midland, Michigan, USA 48686
E. K. Sanchez
Affiliation:
Dow Corning Compound Semiconductor Solutions, Midland, Michigan, USA 48686
D. Hansen
Affiliation:
Dow Corning Compound Semiconductor Solutions, Midland, Michigan, USA 48686
S. G. Mueller
Affiliation:
Dow Corning Compound Semiconductor Solutions, Midland, Michigan, USA 48686
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Abstract

A review is presented of Synchrotron X-ray Topography and KOH etching studies carried out on n type 4H-SiC offcut substrates before and after homo-epitaxial growth to study defect replication and strain relaxation processes and identify the nucleation sources of both interfacial dislocations (IDs) and half-loop arrays (HLAs) which are known to have a deleterious effect on device performance. We show that these types of defects can nucleate during epilayer growth from: (1) short segments of edge oriented basal plane dislocations (BPDs) in the substrate which are drawn by glide into the epilayer; and (2) segments of half loops of BPD that are attached to the substrate surface prior to growth which also glide into the epilayer. It is shown that the initial motion of the short edge oriented BPD segments that are drawn from the substrate into the epilayer is caused by thermal stress resulting from radial temperature gradients experienced by the wafer whilst in the epi-chamber. This same stress also causes the initial glide of the surface half-loop into the epilayer and through the advancing epilayer surface. These mobile BPD segments provide screw oriented segments that pierce the advancing epilayer surface that initially replicate as the crystal grows. Once critical thickness is reached, according to the Mathews-Blakeslee model [1], these screw segments glide sideways under the action of the mismatch stress leaving IDs and HLAs in their wake. The origin of the mismatch stress is shown to be associated with lattice parameter differences at the growth temperature, arising from the differences in doping concentration between substrate and epilayer.

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Articles
Copyright
Copyright © Materials Research Society 2015 

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References

REFERENCES

Matthews, J. and Blakeslee, A., Journal of Crystal Growth 27, 118 (1974).Google Scholar
Jacobson, H., Bergman, J., Hallin, C., Janzén, E., Tuomi, T., and Lendenmann, H., Journal of applied physics 95(3), 1485 (2004).CrossRefGoogle Scholar
Ha, S., Skowronski, M., and Lendenmann, H., Journal of applied physics 96(1), 393 (2004).CrossRefGoogle Scholar
Stahlbush, R., Fatemi, M., Fedison, J., Arthur, S., Rowland, L., and Wang, S., Journal of electronic materials 31(5), 370 (2002).CrossRefGoogle Scholar
Zhang, Z., Moulton, E., and Sudarshan, T.S., Applied Physics Letters 89(8), 081910 (2006).CrossRefGoogle Scholar
Zhang, Z. and Sudarshan, T., Applied Physics Letters 87(15), 151913 (2005).CrossRefGoogle Scholar
VanMil, B.L., Stahlbush, R.E., Myers-Ward, R.L., Lew, K.K., Eddy, C.R., and Gaskill, D.K., Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures 26(4), 1504 (2008).CrossRefGoogle Scholar
Myers-Ward, B.L.V.M. R. L., Stahlbush, R. E., Katz, S. L., McCrate, J. M., Kitt, S. A., Eddy, C. R. Jr., and Gaskill, D. K., Mater. Sci. Forum 105, 615 (2009).Google Scholar
Stahlbush, R.L.M.W. R. E., Vanmill, B. L., Gaskill, D. K., Eddy, C. R. Jr., Mater, . Sci. Forum 271, 645 (2010).Google Scholar
Jacobson, H., Birch, J., Hallin, C., Henry, A., Yakimova, R., Tuomi, T., Janzén, E., and Lindefelt, U., Applied Physics Letters 82(21), 3689 (2003).CrossRefGoogle Scholar
Zhang, X., Ha, S., Hanlumnyang, Y., Chou, C.H., Rodriguez, V., Skowronski, M., Sumakeris, J.J., Paisley, M.J., and O’Loughlin, M.J., Journal of Applied Physics 101(5), 053517 (2007).CrossRefGoogle Scholar
Zhang, N., Chen, Y., Zhang, Y., Dudley, M., and Stahlbush, R.E., Applied Physics Letters 94(12), 122108 (2009).CrossRefGoogle Scholar
Wang, H., Wu, F., Dudley, M., Raghothamachar, B., Chung, G., Zhang, J., Thomas, B., Sanchez, E.K., Mueller, S.G., Hansen, D., and Loboda, M., Materials Science Forum 778780, 328 (2014).CrossRefGoogle Scholar
Sasaki, S., Suda, J., and Kimoto, T., Materials Science Forum 717720, 481 (2012).CrossRefGoogle Scholar
Raghothamachar, B., Dudley, M., and Dhanaraj, G., in Springer Handbook of Crystal Growth (Springer, 2010), pp. 1425.CrossRefGoogle Scholar
Zhang, X., Skowronski, M., Liu, K.X., Stahlbush, R.E., Sumakeris, J.J., Paisley, M.J., and O’Loughlin, M.J., Journal of Applied Physics 102(9), 093520 (2007).CrossRefGoogle Scholar
Zhang, X., Miyazawa, T., and Tsuchida, H., Materials Science Forum 717720, 313 (2012).CrossRefGoogle Scholar
Huang, X.R., Black, D.R., Macrander, A.T., Maj, J., Chen, Y., and Dudley, M., Applied Physics Letters 91(23), 231903 (2007).CrossRefGoogle Scholar
Wang, H.H., Wu, F.Z., Dudley, M., Raghothamachar, B., Chung, G., Zhang, J., Thomas, B., Sanchez, E.K., Mueller, S.G., and Hansen, D.M., presented at the Materials Science Forum, 2014 (unpublished).Google Scholar
Dudley, M., Zhang, N., Zhang, Y., Raghothamachar, B., and Sanchez, E.K., Materials Science Forum 645648, 295 (2010).CrossRefGoogle Scholar