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Critical Current Densities and Irreversibility Fields of High T<sub>c</sub> Superconductors, GaSr<sub>2</sub>Ca<sub>2</sub>Cu<sub>3</sub>O<sub>9</sub> and BSr<sub>2</sub>Ca<sub>n-1</sub>Cu<sub>n</sub>O<sub>2n+3</sub> (n= 3, 4)
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Citations
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References
1996
Year
Superconducting MaterialEngineeringCritical Current DensitiesMagnetoresistanceCritical CurrentsMagnetismSuperconductivityQuantum MaterialsHigh PressureHigh Tc SuperconductorsN= 3Gasr 2Low-temperature SuperconductivityMaterials ScienceHigh-tc SuperconductivityPhysicsSpintronicsFerromagnetismHigh-temperature SuperconductivityNatural SciencesApplied PhysicsCondensed Matter PhysicsDc Magnetization LoopsCritical PhenomenonIrreversibility Fields
From the hystereses in DC magnetization loops, we measured critical current densities J c and irreversibility fields B irr of high T c superconductors, GaSr 2 Ca 2 Cu 3 O 9 (Ga-1223) and BSr 2 Ca n -1 Cu n O 2 n +3 ( B-12( n -1) n , n =3, 4) prepared at a high pressure of 6 GPa. These three phases with blocking layers consisting of single metal planes were expected to have high J c and high B irr . However, the present experiment revealed that their values for both J c and B irr were much smaller than those of the (Cu, C)-based oxides. This result suggests that the electronic structures of the present three phases are more anisotropic than those in the (Cu, C) phases in spite of their thinner blocking layers and that the thickness of the blocking layer, i.e., the spacing between the CuO 2 multilayers, is not always a key parameter determining J c and B irr .
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