Abstract
The phase diagram of the Y-Ba-Cu-O system is given as a function of temperature and partial pressure of oxygen over the range between 500°C and 1000°C and 10-6<P(O2)<102 bar. Conversion of 124 into 123+CuO is interesting because it can produce nonsuperconducting CuO islands and highly strained local regions, both of which may act as flux pinning centers. The partial pressure of oxygen necessary for conversion from YBa2Cu4O8 (124) to YBa2Cu3O7 (123) decreases with decreasing temperatures, and below 850°C the boundary between 123 and 124 phase regions is found to fall approximately as logP(O2)=19.3-22000/T. The 123 decomposition boundary is known to lie near logP(O2)=10.2-14000/T. Since these two curves interest at about 600°C, the 123 phase is unstable at lower temperatures for all P(O2), and so 123 cannot be synthesized near thermodynamic equilibrium at low temperatures.
| Original language | English |
|---|---|
| Pages (from-to) | 153-160 |
| Number of pages | 8 |
| Journal | Physica C: Superconductivity and its applications |
| Volume | 168 |
| Issue number | 1-2 |
| DOIs | |
| State | Published - Jun 1 1990 |
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