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Subsolidus phase relationships of the BaO-R2O3-CuOz (R=Eu, Dy, and Ho) systems under carbonate-free conditions at T=810 deg C and
For applications of phase equilibria to second-generation coated-conductor high-Tc superconductor processing, phase diagrams constructed under carbonate-free conditions are needed. Using a procedure for preparing carbonate-free precursors based on BaO, the phase diagrams of three BaO-R2O3-CuOz syste...
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Published in: | Physica. C, Superconductivity Superconductivity, 2006-06, Vol.439 (2), p.93-100 |
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Main Authors: | , , , , |
Format: | Article |
Language: | English |
Online Access: | Get full text |
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Summary: | For applications of phase equilibria to second-generation coated-conductor high-Tc superconductor processing, phase diagrams constructed under carbonate-free conditions are needed. Using a procedure for preparing carbonate-free precursors based on BaO, the phase diagrams of three BaO-R2O3-CuOz systems (R=Eu, Dy, and Ho) were determined at 810 deg C and (0.1% O2 by volume). The three phase diagrams are substantially different from one another. Among the three systems, Eu3+ has the largest ionic radius and therefore most closely matches the ionic size of Ba2+. Two solid solution series, namely, Ba2-xEuxCuO3+z and Ba2-xEu1+xCu3O6+z were found in the BaO-Eu2O3-CuOz system. The BaO-Dy2O3-CuOz and the BaO-Ho2O3-CuOz systems do not contain solid solution phases. In these systems, which contain the smaller R=Dy, and Ho rare earths, the Ba2-xEuxCuO3+z solid solution and Eu2CuO4 phases of the Eu-system are replaced by the Ba6RCu3Oz (613) phase and the R2Cu2O5 phase, respectively. Additionally, the Ba4RCu3Oz (413) phase appears in systems with smaller R (Dy and Ho) but not in the Eu-system. The Ho-system contains the Ba3R4O9 phase, as well. Consequently, the tie-line relationships are substantially different in these three systems. Among the three diagrams, the diagram for R=Ho is most similar to that of the R=Y system. |
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ISSN: | 0921-4534 |
DOI: | 10.1016/j.physc.2006.03.001 |