Investigation of inter-grain critical current density in Bi2Sr2CaCu2O8+∞ superconducting wires and its relationship with the heat treatment protocol

被引:7
作者
Pallecchi, I. [1 ]
Leveratto, A. [1 ]
Braccini, V. [1 ]
Zunino, V. [1 ,2 ]
Malagoli, A. [1 ]
机构
[1] Natl Res Council CNR SPIN Genoa, Cso Perrone 24, I-16152 Genoa, Italy
[2] Univ Genoa, Dept Phys, Via Dodecaneso 33, I-16146 Genoa, Italy
关键词
inter-grain critical current density; grain boundary transparency; temperature dependence of Jc; GRAIN-BOUNDARIES; TEMPERATURE; CONDUCTORS; DEPENDENCE; TAPES; ZNO;
D O I
10.1088/1361-6668/aa77e6
中图分类号
O59 [应用物理学];
学科分类号
摘要
In this work we investigate the effect of each different heat treatment stage in the fabrication of Bi2Sr2CaCu2O8+infinity superconducting wires on intra-grain and inter-grain superconducting properties. We measure magnetic critical temperature T-c values and transport critical current density J(c) at temperatures from 4 K to 40 K and in fields up to 7 T. From an analysis of the temperature dependence of the self-field critical current density J(c)(T) that takes into account weak link behavior and the proximity effect, we study grain boundary (GB) transparency to supercurrents; we also establish a relationship between GB oxygenation in the different steps of the fabrication process and GB transparency to supercurrents. We find that GB oxygenation starts in the first crystallization stage, but it becomes complete in the plateau at 836 degrees C and in slow cooling stages and is further enhanced in the prolonged post-annealing step. Such oxygenation makes GBs more conductive, thus improving the inter-grain J(c) value and temperature dependence. On the other hand, from inspection of the T-c values in the framework of the phase diagram dome, we find that grains are already oxygenated in the crystallization step up to the optimal doping, while successive slow cooling and post-annealing treatments further enhance the degree of overdoping, especially if carried out in oxygen atmosphere rather than in air.
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页数:10
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