Critical Current Densities and Irreversibility Fields of High Temperature SuperconductorsSr2Ca2Cu3O7+δandSr2Can-1CunO2n+δF2+y(n=2, 3)

1996 ◽  
Vol 35 (Part 1, No. 8) ◽  
pp. 4293-4296 ◽  
Author(s):  
Shan Yu ◽  
Yuichi Okuda ◽  
Tetsuya Kawashima ◽  
Eiji Takayama-Muromachi
2014 ◽  
Vol 792 ◽  
pp. 21-26 ◽  
Author(s):  
Tatiana Prikhna ◽  
Michael Eisterer ◽  
Wolfgang Gawalek ◽  
Athanasios G. Mamalis ◽  
Artem Kozyrev ◽  
...  

The high pressure (50 MPa - 2 GPa) – high temperature synthesized MgB2 bulk materials are characterized by nearly theoretical density (1-2% porosity), 80-98% connectivity, extremely high critical current densities (e.g. at 20 K, in 0–1 T jc=1.3–1.0 MA·cm-2 (with 10% SiC) and jc= 0.92 – 0.73 MA·cm-2 (without doping)), large irreversibility fields (Birr(18.4 K) =15 T and Birr (0 K) = 32.5 T) and high upper critical fields (Bc2 (22 K) =15 T and Bc2(0 K) ~ 42.1 T). The transformation of grain boundary pinning to point pinning in MgB2-based materials with increasing manufacturing temperature (from 800 to 1050 oC) under pressures from 0.1 to 2 GPa correlates well with an increase in critical current density in low external magnetic fields caused by the redistribution of boron and the oxygen impurities in the material structure. As the manufacturing temperature increases, the discontinuous oxygen enriched layers transform into distinct Mg-B-O inclusions and the size and amount of inclusions of higher magnesium borides MgBX (X>4) are reduced. The effect of oxygen and boron redistribution can be enhanced by Ti or SiC additions.


1996 ◽  
Vol 35 (Part 1, No. 6A) ◽  
pp. 3378-3382 ◽  
Author(s):  
Shan Yu ◽  
Yuichi Okuda ◽  
Tetsuya Kawashima ◽  
Eiji Takayama-Muromachi

2016 ◽  
Vol 213 (12) ◽  
pp. 3214-3220 ◽  
Author(s):  
M. Muralidhar ◽  
K. Furutani ◽  
Dinesh Kumar ◽  
M. R. Koblischka ◽  
M. S. Ramachandra Rao ◽  
...  

1996 ◽  
Vol 35 (Part 1, No. 5A) ◽  
pp. 2619-2623 ◽  
Author(s):  
Shan Yu ◽  
Yuichi Okuda ◽  
Eiji Takayama-Muromachi

1998 ◽  
pp. 533-536
Author(s):  
Akira Iyo ◽  
Kazuyasu Tokiwa ◽  
Yasumoto Tanaka ◽  
Norio Terada ◽  
Masayuki Hirabayashi ◽  
...  

1997 ◽  
Vol 12 (11) ◽  
pp. 2924-2940 ◽  
Author(s):  
A. Goyal ◽  
D. P. Norton ◽  
D. M. Kroeger ◽  
D. K. Christen ◽  
M. Paranthaman ◽  
...  

Much of the conductor development effort in the last decade has focused on optimizing the processing of (Bi, Pb)2Sr2Ca2Cu3Ox oxide-powder-in-tube conductors and (Bi, Pb)2Sr2CaCu2O8 (Bi-2212) and TlBa2Ca2Cu3Ox thick film conductors. It is demonstrated that in each of these conductors, critical current densities are dictated by the grain boundary misorientation distributions (GBMD's). Percolative networks of low-angle boundaries with fractions consistent with the active cross-sectional area of the conductor exist in each of these conductors. Further enhancements in the properties require increased numbers of small-angle grain boundaries. Given the processing methods used to fabricate these materials, no clear route employing a simple modification of the established processing method is apparent. To address this need, conductors with controlled or predetermined GBMD's are necessary. Development of biaxial texture appears to be the only possible way to increase the number of small-angle boundaries in a practical and controllable manner. We summarize in this paper recent results obtained on epitaxial superconducting films on rolling-assisted-biaxially-textured-substrates (RABiTS). This technique uses well established, industrially scalable, thermomechanical processes to impart a strong biaxial texture to a base metal. This is followed by vapor deposition of epitaxial buffer layers (metal and/or ceramic) to yield structurally and chemically compatible surfaces. Epitaxial YBa2Cu3O7–δ films grown using laser ablation on such substrates have critical current densities exceeding 106 A/cm2 at 77 K in zero field and have a field dependence similar to epitaxial films on single crystal ceramic substrates. Deposited conductors made using this technique offer a potential route for the fabrication of the next generation high temperature superconducting (HTS) wire capable of carrying high currents in high magnetic fields and at elevated temperatures.


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