Effect of excess Ca on T<sub>c</sub> and J<sub>c</sub> of melt-quenched Bi<sub>2</sub>Sr<sub>2</sub>Ca<sub>1.2</sub>Cu<sub>2</sub>O<sub>x</sub>
J Danusantoso; T K Chaki; J Danusantoso; Dept. of Mech. Eng., State Univ. of New York, Buffalo, NY, USA; T K Chaki; Dept. of Mech. Eng., State Univ. of New York, Buffalo, NY, USA
Журнал:
Superconductor Science and Technology
Дата:
1991-10-01
Аннотация:
The authors present the results of a study investigating how evolution of Ca-rich precipitates (Ca<sub>2</sub>CuO<sub>3</sub>) in melt-quenched Bi<sub>2</sub>Sr<sub>2</sub>Ca<sub>1.2</sub>Cu<sub>2</sub>O<sub>x</sub> affects the superconducting transition temperature (T<sub>c</sub>) and the transport critical current density (J<sub>c</sub>). An excess of 20 at.% Ca raised the transition temperature at zero resistance (T<sub>c,zero</sub>) and the transport critical current density (J<sub>c</sub>) of the melt-quenched material to (85.6+or-0.8) K and (18.9+or-0.5) A cm<sup>-2</sup> at 77 K respectively, compared with (80.2+or-0.6) K and (10.2+or-0.7) A cm<sup>-2</sup> at 70 K for melt-quenched material of stoichiometric composition, with both materials annealed at 840 degrees C for 100 h. The formation of Ca-rich precipitates (Ca<sub>2</sub>CuO<sub>3</sub>) in melt-quenched material with excess Ca was studied with the help of a scanning electron microscope. As the time of anneal at 840 degrees C was increased from 1 min to 150 h, the volume fraction and the average size of Ca<sub>2</sub>CuO<sub>3</sub> precipitates initially increased, reaching maximum values of 27.2% and 1.08 mu m, respectively, at 30 min of annealing, and then started to decrease. However, as the annealing time was increased from 30 min to 150 h, T<sub>c,zero</sub> increased from (35.0+or-0.5) to (85.0+or-0.8) K and the transport critical current density (J<sub>c0</sub>) extrapolated at absolute zero temperature increased from (2.1+or-0.4) to (107.0+or-3.3) A cm<sup>-2</sup>. It is thought that dissolution of Ca<sub>2</sub>CuO<sub>3</sub> precipitates converts Bi<sub>2</sub>Sr<sub>2</sub>CuO<sub>x</sub> (2201) phase at the grain boundaries to superconducting Bi<sub>2</sub>Sr<sub>2</sub>CaCu<sub>2</sub>O<sub>x</sub> (2212) phase, thereby reducing the weak link at the interfaces.
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