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Flux Pinning in Melt-Grown NdBa<sub>2</sub>Cu<sub>3</sub>O<sub>y</sub> and SmBa<sub>2</sub>Cu<sub>3</sub>O<sub>y</sub> Superconductors
426
Citations
8
References
1994
Year
Superconducting MaterialEngineeringReba 2Critical CurrentsSuperconductivityQuantum MaterialsHigh Tc SuperconductorsRare EarthLow-temperature SuperconductivityMaterials ScienceHigh-tc SuperconductivityPhysicsNiobium-based SuperconductorsHigh-temperature SuperconductivityCryogenicsCondensed Matter PhysicsApplied PhysicsFlux PinningO Y Superconductors
REBa₂Cu₃O_y superconductors with large rare‑earth ions such as La, Nd, and Sm exhibit relatively low Tc because of a RE–Ba solid solution. Melt processing in a reduced oxygen atmosphere suppresses this solid solution, raising critical current densities above those of melt‑processed YBa₂Cu₃O_y with fine Y₂BaCuO₅ inclusions, shifting the irreversibility line to higher H‑T, and attributing enhanced flux pinning to a finely distributed RE(Ba₁₋ₓ,REₓ)₂Cu₃O_y phase.
REBa 2 Cu 3 O y superconductors with rare earth (RE) ions with large radii (RE: La, Nd, Sm) exhibit relatively low T c due to the presence of RE-Ba solid solution. We have found that this solid solution can be suppressed if these superconductors are melt processed in a reduced oxygen atmosphere. We have also found that critical current densities of these superconductors are higher than those of melt processed YBa 2 Cu 3 O y with fine Y 2 BaCuO 5 inclusions in a high field region. The irreversibility line was also shifted toward the higher H-T region. We believe that flux pinning in these superconductors is ascribable to a finely distributed RE(Ba 1- x , RE x ) 2 Cu 3 O y phase in a good superconductive matrix.
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1990 | 781 | |
1989 | 763 | |
1989 | 761 | |
1988 | 217 | |
1993 | 166 | |
1988 | 96 | |
1987 | 73 | |
1987 | 18 |
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