Abstract
The effects of composition, processing time (t), temperature (T) and O2 partial pressure (pO2) on the superconducting transition temperature, Tc, were investigated for La1+zBa2-zCu3Oy. Tallon and Flower's prediction of T c ≈ 100 K [Physica C 204 (1993) 237] at z = 0 could not be attained. Instead, the Tc maximum of 93-94K is similar to that of the yttria analog. As z was increased, the Tc values increased gradually by a few kelvin until z = 0.2, which is at the orthorhombic to tetragonal transition, and then decreased more abruptly, with no superconductivity for z≥0.5. Crucial steps in the process at all z values include the highest temperature anneal (1065°C) in 0.1 MPa O2, reduction of the oxygen content at 950°C and cooling to 300-400°C, both at 100-1000 Pa O2, and reoxygenation at 0.1 MPa O2 during slow cooling (5-20°C/min) to < 150°C. Additional experiments demonstrated that the intragranular critical current was less than that for the yttria analog. Values of Tc decreased fairly monotonically with decreasing y at z = 0.08, and a La excess of 0.2 and Cu nonstoichiometry on both sides of Cu/(La+Ba) = 1 generally depressed Tc.
Original language | English |
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Pages (from-to) | 80-90 |
Number of pages | 11 |
Journal | Physica C: Superconductivity and its Applications |
Volume | 231 |
Issue number | 1-2 |
DOIs | |
State | Published - Sep 20 1994 |
Funding
The primary motivation for this investigation was the prediction by Tallon and Flower \[1 \] that a superconducting transition temperature, T¢, of ~ 100 K should be achievable for the z = 0 composition of the "123"-type Laj+zBa2_,Cu3Oy solid solution (La-123) t. Most earlier work \[2-12\] demonstrated the maximum Tc at z ---0, onset of superconductivity several degrees below 100 K, and zero resistance at 80--92 K. Specimens were synthesized by the usual high- * Correspondinga uthor. '~ Research sponsored by the Division of Materials Sciences, US Department of Energy, under contract DE-AC05-84OR21400 with Martin Marietta Energy Systems, Inc.
Funders | Funder number |
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Division of Materials Sciences | |
U.S. Department of Energy | DE-AC05-84OR21400 |