Absence of pair breaking effect in Cu0.5Tl0.5Ba2Ca2Cu3−yZnyO10−δ(y = 0, 0.75, 1.5, 2.25, 2.5, 2.65) superconductor
Author:
Publisher
EDP Sciences
Subject
Condensed Matter Physics,Instrumentation,Electronic, Optical and Magnetic Materials
Link
http://epjap.epj.org/10.1051/epjap:2007044/pdf
Reference36 articles.
1. Effect of 3d metal ion doping on the structure and superconductivity of (Tl0.5Pb0.5)Sr2CaCu2O7
2. Zn-impurity effects on high-temperature superconductivity
3. Substitution for Cu in the electron-doped infinite-layer superconductorSr0.9La0.1CuO2:Ni reducesTcmuch faster than Zn
4. Tcdepression in theYBa2Cu4−xMxO8system forM=Fe, Ni, Zn, and Ga
5. Influence of Cu-site substitution on the structure and superconducting properties of theNdBa2Cu3−xMxO7+δ(M=Fe,Co) andNdBa2Cu3−xMxO7−δ(M=Ni,Zn) systems
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1. The Role of Mass of Doped Atoms in the Superconductivity of Cu0.5Tl0.5Ba2Ca2Cu3O10−d and Cu0.5Tl0.5Ba2Ca2Cu1.5 M1.5O10−d (M = Cd, Zn, and Ni);Journal of Superconductivity and Novel Magnetism;2016-12-12
2. Synthesis and superconductivity of (Ag) x /CuTl-1223 composites;Progress in Natural Science: Materials International;2015-06
3. Highly coercive cobalt ferrite nanoparticles-CuTl-1223 superconductor composites;Journal of Magnetism and Magnetic Materials;2015-03
4. Comparison of the superconducting properties of Cu0.5Tl0.5Ba2Ca2(Cu3−yZny)O10−δ prepared at different synthesis temperatures;Ceramics International;2012-12
5. Resistive transition in Mn doped Cu0.5Tl0.5Ba2Ca2Cu3O10-y superconductor;Solid State Sciences;2011-12
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