journal article·2017-03

Determination of optimum diffusion annealing temperature for Au surface-layered Bi-2212 ceramics and dependence of transition temperatures on disorders

G. Yildirim

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Abstract

Abstract This study aims not only to declare experimentally the effect of diffusion annealing temperature (600 °C-850 °C) on the crystal structure, electrical and superconducting properties of Au surface-layered Bi-2212 ceramics by dc resistivity and powder X-ray diffraction measurements, but also to advance in-depth understanding of empirical relationship between the disorders and transition temperatures. It is found that the diffusion annealing temperature of 800 °C is found to be optimum for the improvement of crystal structure due to the retrogression of disorders and local structural-distortions in the layers, increasing metastability, σ-gap anisotropy and softening of Ag and B1g phonons. Accordingly, the Au nanoparticles transit from inherently over-doped nature of the compound to optimally-doped state. Additionally, the empirical relations between critical temperatures and Δ ρ parameters (related to disorders) show that it is possible to achieve maximum onset and offset critical temperature values of 90.467 K and 90.359 K for the Bi-2212 ceramics.
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Research context

OpenAlex topics: Physics of Superconductivity and Magnetism · Iron-based superconductors research · Superconductivity in MgB2 and Alloys

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References (37)

Show source-provided references
1. Ginzburg · 2004
2. Joining of Bi-2212 high-T-c superconductors and metals using indium solders10.1016/j.physc.2007.05.040 ↗
3. 6.4 MVA resitive fault current limiter based on Bi-2212 superconductor10.1016/S0921-4534(02)01096-1 ↗
4. A resistive fault current limiter based on high temperature superconductors10.1016/0964-1807(95)00074-7 ↗
5. Development of a high-efficiency conduction cooling technology for SMES coils10.1109/TASC.2012.2235751 ↗
6. Recycling failed bulk YBCO superconductors using the NdBCO/YBCO/MgO film-seeded top-seeded melt growth method10.1063/1.4720400 ↗
7. Buckel · 2004
8. Determination of solid solubility level of Ho nanoparticles in Y-123 superconducting matrix and strong Cu-1 site preference of nanoparticles10.1016/j.jallcom.2014.04.037 ↗
9. A new high-Tc oxide superconductor without a rare-earth element10.1143/JJAP.27.L209 ↗
10. Structural and physical properties of Cd-doped Bi1.64Pb0.36Sr2Ca2-xCdxCu3Oy superconductor10.1016/j.physb.2010.08.053 ↗
11. Enhanced critical current density in Gd-added (Bi, Pb)-2212 bulk superconductor10.1088/0953-2048/18/11/007 ↗
12. Electrical, magnetic and superconducting properties of the quenched Bi2Sr2Ca1-xNdxCu2O8+γ system10.1143/JJAP.29.L53 ↗
13. Anisotropic normal-state transport-properties predicted and analyzed for high-Tc oxide superconductors10.1103/PhysRevB.37.7482 ↗
14. Nonlinear temperature-dependence of the normal-state resistivity in YBa2Cu4O8+/-γ films10.1103/PhysRevB.39.9611 ↗
15. Role of vanhove singularity in high-temperature superconductors - Mean field10.1103/PhysRevB.43.3075 ↗
16. Investigation of Lu effect on YBa2Cu3O7-γ superconducting compounds10.1007/s10854-012-0846-y ↗
17. Ekin · 2006
18. Granular superconductivity in polycrystalline Bi2Sr2CaCu2O8+γ by homovalent La substitution on Bi sites10.1016/j.jnoncrysol.2010.09.036 ↗
19. The role of Ag in the pulsed laser growth of YBCO thin films10.1063/1.370172 ↗
20. Universal T-c depression by irradiation defects in underdoped and overdoped cuprates?10.1209/epl/i2000-00238-x ↗
21. Low 1/f normal-state resistance noise in high-resistivity YBa2Cu3Oy films10.1063/1.115507 ↗
22. A correlation between transport current density and grain connectivity in MgB2/Fe wire made from ball-milled boron10.1063/1.3129314 ↗
23. The influence of Sno2 nano-particles addition on the vickers microhardness of (Bi, Pb)-2223 superconducting phase10.1007/s10948-011-1334-y ↗
24. Optical characterization and microstructure of BaTiO(3) thin films obtained by RF-magnetron sputtering10.1016/j.apsusc.2006.06.008 ↗
25. Growth-kinetics of high-Tc and low-Tc phases in Bi2-xPbxCa2Sr2Cu3Oy superconducting compounds10.1002/crat.2170280302 ↗
26. Characteristics of hopping conductivity in one-dimensional binary disordered system with off-diagonal correlations10.7498/aps.56.2852 ↗
27. Tendency towards local spin compensation of holes in the high-Tc copper-compounds10.1103/PhysRevLett.61.1415 ↗
28. Role of annealing time and temperature on structural and superconducting properties of (Bi, Pb)-2223 thin films produced by sputtering10.1007/s10854-011-0522-7 ↗
29. Raman-active phonons in Bi2Sr2Ca1-xYxCu2O8+d(x=0-1): effects of hole filling and internal pressure induced by Y doping for Ca, and implications for phonon assignments10.1103/PhysRevB.53.11796 ↗
30. Role of diffusion-annealing temperature on the microstructural and superconducting properties of Cu-doped MgB2 superconductors10.1007/s10854-012-0689-6 ↗
31. The effect of substitution of Eu on the critical current density and flux pinning properties of (Bi, Pb)-2212 superconductor10.1088/0953-2048/21/4/045001 ↗
32. Improved microstructure and flux pinning properties of Gd-substituted (Bi,Pb)-2212 superconductor sintered between 846 and 860 degrees10.1016/j.matlet.2008.07.052 ↗
33. Flux pinning properties of Yb substituted (Bi,Pb)-2212 superconductor10.1016/j.jallcom.2006.12.100 ↗
34. Superconductivity and X-ray photoelectron spectroscopy studies of Bi2Sr2-xLaxCaCu2O8+γ10.1023/A:1018571832434 ↗
35. Detailed analysis on electrical conduction transition from 2D variable range hopping to phonon-assisted 3D VRH mechanism belonging to Bi-site La substituted Bi-2212 system10.1016/j.jallcom.2014.10.150 ↗
36. Textured BSSCO/Ag superconducting microcomposites with improved critical current-density through mechanical deformation10.1088/0953-2048/5/5/008 ↗
37. Topotactical reactions with ferrimagnetic oxides having hexagonal crystal structures–I10.1016/0022-1902(59)80070-1 ↗