Hostname: page-component-cd9895bd7-jkksz Total loading time: 0 Render date: 2024-12-28T01:07:41.889Z Has data issue: false hasContentIssue false

Processing characteristics and properties of BiSrCaCuO superconducting glass ceramics prepared by melt-quenching

Published online by Cambridge University Press:  03 March 2011

Y. Massalker
Affiliation:
Materials Engineering Department, Ben-Gurion University of the Negev, Beer-Sheva, Israel
A.N. Sembira
Affiliation:
Chemical Engineering Department, Ben-Gurion University of the Negev, Beer-Sheva, Israel
J. Baram
Affiliation:
Materials Engineering Department, Ben-Gurion University of the Negev, Beer-Sheva, Israel
Get access

Abstract

In the framework of an extensive research program for the production of textured and ductile high Tc BiSrCaCuO (BiSCO) wires and tapes, the influence of processing (by melt-quenching) parameters on the crystallization behavior, the quantitative and qualitative evolution of the crystallized phases, the chemical changes in the bulk, and the superconductive properties of various initial compositions of bulk BiSCO glass ceramics, prepared by melt-quenching, have been studied. The elemental composition of the samples changes drastically during heat treatments, affecting mainly Pb, but Sr and Ca also. The identified crystallographic phases, by XRD, were the low Tc superconducting “2201” (Bi2Sr2CuO6) phase, the high Tc superconducting “2212” and “2223” phases, and the Ca2PbO4, Ca2CuO3, CuO, CaO, Bi2Sr3-xCaxOy, and (Ca, Sr)3Cu5O8 “impurities” compounds. A crystallization sequence from the amorphous state is proposed, involving a reaction at 800 °C between “2223”, CaO, Ca2CuO3, and Bi2SrCaxOy to form “2212” + Ca2PbO4 + CuO and a 2(“2212”) → “2223” + “2201” disproportionation reaction that takes place with the intake of oxygen at a higher temperature. Decomposition of Ca2PbO4, which occurs also at high temperature, causes an increase of “2212”, which favors the increase of “2223” through the disproportionation reaction. The glass transition starts around Tg = 400 °C, and the crystallization reactions from the amorphous state proceed in two steps, at Txl = 465 °C and Tx2 = 504 °C. The Bi2Sr3-xCaxOy “2212” and “2223” phases are among the first to crystallize as early as after a 1 h treatment (in air) at 488 °C. A gain in weight is observed by thermogravimetry, caused by intake of the oxygen necessary for the formation of the high Tc superconducting phases. The oxygen intake starts as early as 600 °C. The Tc onset for the “2223” phase is at 122 K, and at 85.5 °C for the “2212” phase. Coefficients of thermal expansion have been measured and shown to differ according to crystallographic direction of expansion. The resistivity is increased on cooling, indicating semiconducting behavior of the 2223 BiSCO ceramic (semiconductor-to-metal transition temperature: 210–220 K).

Type
Articles
Copyright
Copyright © Materials Research Society 1993

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

1Komatsu, T., Sato, R., Imai, K., Matusita, K., and Yamashita, T., Jpn. J. Appl. Phys. 27, L548 (1988).Google Scholar
2Nasu, H., Ibara, Y., S. Makida, Imura, T., and Osaka, Y., J. Non-Cryst. Solids 105, 185 (1988).CrossRefGoogle Scholar
3Yi, L. Zhi and Persson, M., Supercond. Sci. Tectmol. 1,198 (1988).Google Scholar
4Komatsu, T., Sato, R., Imai, K., Matusita, K., and Yamashita, T., Jpn. J. Appl. Phys. 27, L1839 (1988).CrossRefGoogle Scholar
5Shimomura, S., Takashahi, K., Ohta, M., Watanabe, A., Seido, M., and Hosono, F., Jpn. J. Appl. Phys. 27, L1890 (1988).Google Scholar
6Kamatsu, T., Sato, R., Hirose, C., Matusita, K., and Yamashita, T., Jpn. J. Appl. Phys. 27, L2293 (1988).CrossRefGoogle Scholar
7Varma, K. B. R., Rao, K. J., and Rao, C. N. R., Appl. Phys. Lett. 54, 69 (1989).CrossRefGoogle Scholar
8Yoshimura, M., Sung, T., Ishizawa, N., and Nakagawa, Z., Jpn. J. Appl. Phys. 28, L424 (1989).CrossRefGoogle Scholar
9Concalves, A. P., Santos, I. C., Almeida, M., Figueitedo, M. O., Alves, J. Maia, Godhino, M. M., Costa, F., and Vieira, J. M., J. Less-Comm. Met. 150, 305 (1989).CrossRefGoogle Scholar
10Yoshimura, M., Sung, T., Nakagawa, Z., and Nakamura, T., J. Mater. Sci. Lett. 8, 687 (1989).CrossRefGoogle Scholar
11Miller, T.A., Sanders, S. C.. Ostenson, J.E., Finnemore, D. K., LeBeau, S.E., and Righi, J., Appl. Phys. Lett. 56, 584 (1990).CrossRefGoogle Scholar
12Yusheng, H., Jincang, Z., Aisheng, H., Jinsong, W., and Yujing, H., Supercond. Sci. Technol. 4, S154 (1991).CrossRefGoogle Scholar
13Sato, R., Komatsu, T., and Matusita, K., J. Mater. Sci. Lett. 10, 355 (1991).CrossRefGoogle Scholar
14Asthana, A., Han, P. D., Xu, Z., Chang, L., Payne, D. A., and Gilbert, P. J., Physica C 174, 33 (1991).CrossRefGoogle Scholar
15Tai, M. F., Shieh, M. J., and Nee, C. C., Physica B 169, 649 (1991).CrossRefGoogle Scholar
16Jayavel, R., Murugakoothan, P., Rao, C. R. Venkateswara, Subramanian, C., Ramasamy, P., Chakravarti, A., Ranganathan, R., and Raychaudhuri, A. K., Solid State Commun. 79, 421 (1991).CrossRefGoogle Scholar
17Gan, F. and Li, G., J. Non-Cryst. Solids 130, 67 (1991).CrossRefGoogle Scholar
18Hirata, K. and Abe, Y., J. Mater. Res. 6, 1156 (1991).CrossRefGoogle Scholar
19S.J. Kim, Birnie, D. P., Aruchamy, A., Uhlman, D. R., EloBayoumi, O.H., and Suscavage, M. J., Physica C 191, 316 (1992).Google Scholar
20McGinnis, W. C. and Briggs, J. S., J. Mater. Res. 7, 585 (1992).CrossRefGoogle Scholar
21Tohge, N., Tsuboi, S., Tatsumisago, M., and Minami, T., Jpn. J. Appl. Phys. 28, L1742 (1989).CrossRefGoogle Scholar
22Chaviv, R. and Baram, J., unpublished.Google Scholar
23The thermal treatments wre slightly altered sometimes.Google Scholar
24A sample is defined as glass if there are no detectable x-ray diffraction peaks.Google Scholar
25Mukherjee, P.S., Simin, A., Koshy, J., Guruswamy, P., and Damodaran, A. D., Solid State Commun. 76, 659 (1990).CrossRefGoogle Scholar
26Tallon, J.L., Buckley, R. G., Gilberd, P.W., and Presland, M. R., Physica C 158, 247 (1989).CrossRefGoogle Scholar
27The analyses of two commercial specimens (details on the heat treatment procedure were not available), said to consist of "pure" high Tc phases (L 2212 and H 2223), also show the presence of Al.Google Scholar
28Holesinger, T. G., Miller, D. J., and Chumbley, L. S., J. Mater. Res. 7, 1658 (1992).CrossRefGoogle Scholar
29Hatano, T., Aota, K., Hattori, H., Ikada, S., Nakamura, K., and Ogawa, K., Cryogenics 30, 611 (1990).CrossRefGoogle Scholar
30Specimen 9 and, with small changes, specimen 10, as examples.Google Scholar
31Nagai, M., Nishino, T., Hattori, T., Matsuda, M., and Takata, M., J. Mater. Sci. 26, 5681 (1991).CrossRefGoogle Scholar
32The proposed reactions show a stoichiometric balance. This is, however, not a proof that these reactions do indeed occur. More convincing is the fact that the quantitative changes observed by the x-ray diffraction are in good coordinateness with the “balanced” reaction schemes.Google Scholar
33Tatsumisago, M., Tsuboi, S., Tohge, N., and Minami, T., Appl. Phys. Lett. 57, 195 (1990).CrossRefGoogle Scholar
34Idemoto, Y., Ichikawa, S., and Fieki, K., Physica C 181,171 (1991).CrossRefGoogle Scholar
35The numbers in Table II are relative intensities of one or more characteristic diffraction peaks for each crystallographic phase. They are shown for comparison only.Google Scholar
36Ibara, Y., Nasu, H., Imura, T., and Osaka, Y., Jpn. J. Appl. Phys. 28, L37 (1989).CrossRefGoogle Scholar
37In Ref. 28, the superconducting “2212” phase appears after 1 min (!) treatment at 650 °C in oxygen. The Bi2Sr3−xCaxOy, phase appears first at 500 °C.Google Scholar
38Hatano, T., Aota, K., Ikada, S., Nakamura, K., and Ogawa, K., Jpn. J. Appl. Phys. 27, L2055 (1988).CrossRefGoogle Scholar
39Softening of the specimens has indeed been observed in the furnace at the mentioned temperatures.Google Scholar
40If evaporation of Pb occurs at 650 °C, it did so in both samples, but could have been somehow accelerated in the powders, due to higher surface to volume ratio.Google Scholar
41O'Bryan, H. M., Rhodes, W. W., and Gallagher, P. K., Chem. Mater. 2, 421 (1990).CrossRefGoogle Scholar
42The critical current characteristics of the melt-quenched specimens are currently evaluated, with relation to several melttexturing methods, and will be reported elsewhere.Google Scholar