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Transport Critical Current Densities in Uniaxially and Biaxially Oriented Tl<sub>1</sub>(Ba<sub>0.8</sub>Sr<sub>0.2</sub>)<sub>2</sub>Ca<sub>2</sub>Cu<sub>3</sub>O<sub>9</sub>Superconducting Films on Ag and SrTiO<sub>3</sub>Substrates Prepared by a Spray Pyrolysis Method
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Citations
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References
1994
Year
Superconducting MaterialMagnetic PropertiesEngineeringSpray Pyrolysis MethodCrystal Growth TechnologySolid-state ChemistryThin Film Process TechnologyTl 1Critical CurrentsSr 0.2SuperconductivityQuantum MaterialsCharge Carrier TransportThin Film ProcessingMaterials ScienceMaterials EngineeringHigh-tc SuperconductivityMaterial AnalysisHigh-temperature SuperconductivitySurface ScienceApplied PhysicsCondensed Matter PhysicsThin FilmsBa 0.8
Tl 1 (Ba 0.8 Sr 0.2 ) 2 Ca 2 Cu 3 O 9 films were prepared by a spray pyrolysis method on SrTiO 3 (100) single crystal substrates and on polycrystalline Ag tapes. The biaxially ( c - and a -axes) oriented Tl 1 (Ba 0.8 Sr 0.2 ) 2 Ca 2 Cu 3 O 9 film on SrTiO 3 single crystal substrate showed very high performance of the transport J c , i.e. 2.8×10 5 A/cm 2 at 77 K, 0 T and 5.0×10 4 A/cm 2 at 77 K, 1 T ( H // c - axis). In contrast, the c -axis oriented film was obtained on Ag tape with the J c of 8.0×10 4 A/cm 2 , at 77 K, 0 T, and of 6.9×10 3 A/cm 2 , at 77 K, 1 T ( H // c - axis). In the c -axis oriented Tl 1 (Ba 0.8 Sr 0.2 ) 2 Ca 2 Cu 3 O 9 film, the weak link behavior remained, however the weak magnetic field dependence of the J c and the very high J c in the biaxially oriented film suggested that the weak link problem was eliminated. We concluded it would be necessary to get the biaxial orientation to produce practical wires of Tl-1223.
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