Hostname: page-component-78c5997874-s2hrs Total loading time: 0 Render date: 2024-11-13T01:13:21.976Z Has data issue: false hasContentIssue false

Growth Mechanism of RE-Ba-Cu-O Crystal by Liquid Phase Epitaxy Process

Published online by Cambridge University Press:  18 March 2011

K. Nomura
Affiliation:
Superconductivity Research Laboratory, International Superconductivity Technology Center 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan
S. Hoshi
Affiliation:
Superconductivity Research Laboratory, International Superconductivity Technology Center 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan
X. Yao
Affiliation:
Superconductivity Research Laboratory, International Superconductivity Technology Center 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan
Y. Nakamura
Affiliation:
Superconductivity Research Laboratory, International Superconductivity Technology Center 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan
T. Izumi
Affiliation:
Superconductivity Research Laboratory, International Superconductivity Technology Center 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan
Y. Shiohara
Affiliation:
Superconductivity Research Laboratory, International Superconductivity Technology Center 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan
Get access

Abstract

Growth of YBa2Cu3Oy (YBCO) crystals both on the MgO and the YBCO substrates has been investigated in order to clarify the growth mechanism of the liquid phase epitaxy (LPE) process for the coated conductor. It was found that the slope angle of the growth grain varied with growing in the initial stage of the LPE growth. In the case of the MgO substrate, the slope angle increased with laterally growing the crystal. On the other hand, the slope angle decreased with growing the crystal in the case of the YBCO substrate. This phenomenon with the opposite tendency could be explained by considering the difference in the step-advancing rates between on the MgO and the YBCO surfaces. It was found that the deep and steep valley of the LPE grains due to the slow step-advancing rate on the MgO is the origin of the flux trapping inclusions. It is necessary that the seed films should cover the entire MgO surface without undesired orientation grains and impurity particles in order to obtain the high quality LPE layer.

Type
Research Article
Copyright
Copyright © Materials Research Society 2001

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. Shiohara, Y. and Hobara, N., Advances in Superconductivity XII, ed. by Yamashita, T. and Tanabe, K. (Springer-Verlag, Tokyo, 2000) p.567.Google Scholar
2. Izumi, T., Hobara, N., Kakimoto, K., Izumi, T., Hasegawa, K., Kai, M., Honjo, T., Yao, X., Fuji, H., Nakamura, Y. and Shiohara, Y., submitted to Advances in Superconductivity XIII.Google Scholar
3. Ishida, Y., Kimura, T., Kakimoto, K., Yamada, Y., Nakagawa, Z., Shiohara, Y. and Sawaoka, A. B., Physica C, 292, 264 (1997).Google Scholar
4. Yamada, Y. and Shiohara, Y., Physica C, 217, 182 (1993).Google Scholar
5. Bennema, P., Leeuwen, C. van, Boon, J. and Gilmer, G. H., Kristall und Tecknik, 8, 659 (1973).Google Scholar
6. Izumi, T., Kakimoto, K., Nomura, K. and Shiohara, Y., J. Cryst. Growth, 219, 228 (2000).Google Scholar
7. Nomura, K., Hoshi, S., Yao, X., Kakimoto, K., Izumi, T., Nakamura, Y. and Shiohara, Y., submitted to J. Cryst. Growth.Google Scholar