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Structure Of The Defects Responsible For B-Mode Breakdown Of Gate Oxide Grown On The Surface Of Silicon Wafers

Published online by Cambridge University Press:  15 February 2011

T. Mera
Affiliation:
Komatsu Electronic Metals Co. Ltd., 2612 Shinomiya, Hiratsuka, Kanagawa 254, Japan
J. Jablonski
Affiliation:
Komatsu Electronic Metals Co. Ltd., 2612 Shinomiya, Hiratsuka, Kanagawa 254, Japan
M. Danbata
Affiliation:
Komatsu Electronic Metals Co. Ltd., 2612 Shinomiya, Hiratsuka, Kanagawa 254, Japan
K. Nagai
Affiliation:
Komatsu Electronic Metals Co. Ltd., 2612 Shinomiya, Hiratsuka, Kanagawa 254, Japan
M. Watanabe
Affiliation:
Komatsu Electronic Metals Co. Ltd., 2612 Shinomiya, Hiratsuka, Kanagawa 254, Japan
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Abstract

Crystal-originated pits are known as the defects responsible for B-mode Time Zero Dielectric Break-down (TZDB) of the gate oxide grown on the surface of Si wafers. In order to clarify the breakdown mechanism, we have analyzed the structure of those defects formed at the surface of bare and oxidized wafers. In the latter case the analysis has been done both before and after gate oxide breakdown. Electric breakdown has been accomplished by Cu decoration method, recognized as an effective tool for unambiguous detection and positioning of the defects causing B-mode TZDB. As revealed by cross-sectional transmission electron microscopy (XTEM), crystal-originated pits at the bare wafer surface are polyhedral pits having about 5-nm-thick oxide layer on the inner walls. During gate oxidation the thermal oxide is growing faster on the pit walls than on the wafer surface, except for the pit comers where the oxide thinning has been observed. Resulting concave comers of the oxidized pits are suggested to be the weak spots where B-mode TZDB occurs.

Type
Research Article
Copyright
Copyright © Materials Research Society 1997

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References

1. Nakamura, K., Saisyoji, T., and Kubota, T., to be published in J. Cryst. Growth, (1996)Google Scholar
2. Nishimura, M., Yoshino, S., Motoura, H., Shimura, S., Mchedlidze, T., and Hikone, T., J. Electrochem. Soc. 143, p. 243 (1996).Google Scholar
3. Kato, M., Yoshida, T., Ikeda, Y., and Kitagawara, Y., Jpn. J. Appl. Phys 35, p. 5597 (1996).Google Scholar
4. Itsumi, M., Tomita, M., and Yamawaki, M., Microelectronic Engineering 28, p. 39 (1995).Google Scholar
5. Itsumi, M., Akiya, H., Ueki, T., Tomita, M., and Yamanaki, M., J. Appl. Phys. 78, p. 5984 (1995).Google Scholar
6. Miyazaki, M., Miyazaki, S., Yanase, Y., Ochiai, T., and Shigematsu, T., Jpn. J. Appl. Phys. 34, p. 6303 (1995).Google Scholar
7. Shannon, W. J., RCA Review, p. 431, June 1970.Google Scholar
8. Sakina, Y., Ohno, T., and Matsumoto, S., Jpn. J. Appl. Phys. 22, p. L514 (1983).Google Scholar
9. Yamabe, K. and Imai, K., IEEE Trans. Electron Devices ED–34, p. 1681 (1987).Google Scholar