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Formation of the 110-K superconducting phase via the amorphous state in the Bi-Sr-Ca-Cu-O system
89
Citations
10
References
1989
Year
Superconducting MaterialEngineeringCrystal Growth TechnologyAmorphous StateSuperconductivityQuantum MaterialsLow-temperature SuperconductivityMaterials Science110-K Superconducting PhaseMagnetic ShieldingHigh-tc SuperconductivityPhysicsCrystalline DefectsBi-sr-ca-cu-o SystemCrystallographyCopper DiffusionHigh-temperature SuperconductivityNatural SciencesApplied PhysicsCondensed Matter PhysicsKinetic Behavior
Eutectic crystallization during annealing of rapidly solidified Bi‑Sr‑Ca‑Cu‑O glasses initiates the formation of superconducting phases. The study examines crystallization mechanisms, calcium and copper diffusion phenomena, and their influence on superconducting properties. Annealing produces a 110‑K superconducting phase that nucleates at eutectic interfaces, grows to a maximum volume fraction before vanishing, while 85‑K and Ca₂CuO₃ phases co‑grow from the amorphous matrix, with the kinetics and phase‑change cycling governed by calcium and copper diffusion and dependent on initial composition.
The thermodynamic and kinetic behavior of both the 85 and 110-K superconducting phases during the crystallization annealing process have been observed and analyzed using x-ray diffraction, magnetic shielding, and resistivity measurements in crystallized Bi-Sr-Ca-Cu-O glasses with nominal compositions ${\mathrm{Bi}}_{2}$${\mathrm{Sr}}_{2}$${\mathrm{Ca}}_{2}$${\mathrm{Cu}}_{3}$${\mathrm{O}}_{\mathit{x}}$ (2:2:2:3), ${\mathrm{Bi}}_{2}$${\mathrm{Sr}}_{2}$${\mathrm{Ca}}_{3}$${\mathrm{Cu}}_{4}$${\mathrm{O}}_{\mathit{x}}$ (2:2:3:4), and ${\mathrm{Bi}}_{2}$${\mathrm{Sr}}_{2}$${\mathrm{Ca}}_{4}$${\mathrm{Cu}}_{5}$${\mathrm{O}}_{\mathit{x}}$ (2:2:4:5). A single superconducting transition near 110 K has been observed in both resistive and magnetization shielding experiments for crystallized samples with 2:2:3:4 and 2:2:4:5 nominal compositions. Eutectic crystallization occurs during annealing of rapidly solidified glass samples. Both the 85-K and ${\mathrm{Ca}}_{2}$${\mathrm{CuO}}_{3}$ phases cooperatively nucleate and grow from the amorphous matrix. The 110-K phase subsequently forms at the interfaces between the eutectic products, controlled by calcium and copper diffusion. A phase-change cycling has been observed, during which the 110-K phase increases in volume percent with increasing annealing time at 870 \ifmmode^\circ\else\textdegree\fi{}C in calcium- and copper-rich samples. It then vanishes as annealing is prolonged at the same temperature. This behavior also occurs with different time periods depending on the initial calcium and copper composition of the samples. Microstructural changes associated with such cycling have also been observed. Also discussed are crystallization mechanisms, diffusion phenomena, and related superconducting properties.
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