Critical current densities in single‐crystal Bi2.2Sr2Ca0.8Cu2O8+δ

1988 ◽  
Vol 52 (22) ◽  
pp. 1910-1912 ◽  
Author(s):  
R. B. van Dover ◽  
L. F. Schneemeyer ◽  
E. M. Gyorgy ◽  
J. V. Waszczak
Cryogenics ◽  
1994 ◽  
Vol 34 (11) ◽  
pp. 941-945 ◽  
Author(s):  
A. Wahl ◽  
V. Hardy ◽  
A. Maignan ◽  
C. Martin ◽  
B. Raveau

2012 ◽  
Vol 36 ◽  
pp. 704-709 ◽  
Author(s):  
Baorong Ni ◽  
Jun Ge ◽  
Masaru Kiuchi ◽  
Edmund Soji Otabe ◽  
Teruo Matsushita ◽  
...  

2013 ◽  
Author(s):  
M. Babu Suresh ◽  
A. Thamizhavel ◽  
S. Ramakrishnan ◽  
A. K. Grover ◽  
D. Pal

Author(s):  
I-Fei Tsu ◽  
D.L. Kaiser ◽  
S.E. Babcock

A current theme in the study of the critical current density behavior of YBa2Cu3O7-δ (YBCO) grain boundaries is that their electromagnetic properties are heterogeneous on various length scales ranging from 10s of microns to ˜ 1 Å. Recently, combined electromagnetic and TEM studies on four flux-grown bicrystals have demonstrated a direct correlation between the length scale of the boundaries’ saw-tooth facet configurations and the apparent length scale of the electrical heterogeneity. In that work, enhanced critical current densities are observed at applied fields where the facet period is commensurate with the spacing of the Abrikosov flux vortices which must be pinned if higher critical current density values are recorded. To understand the microstructural origin of the flux pinning, the grain boundary topography and grain boundary dislocation (GBD) network structure of [001] tilt YBCO bicrystals were studied by TEM and HRTEM.


2006 ◽  
Vol 89 (13) ◽  
pp. 132510 ◽  
Author(s):  
Xianping Zhang ◽  
Zhaoshun Gao ◽  
Dongliang Wang ◽  
Zhengguang Yu ◽  
Yanwei Ma ◽  
...  

Cryogenics ◽  
1994 ◽  
Vol 34 (4) ◽  
pp. 329-334
Author(s):  
H.L Ji ◽  
Z.X Shi ◽  
Z.Y Zeng ◽  
X Jin ◽  
H.C Fan ◽  
...  

2015 ◽  
Vol 5 (1) ◽  
Author(s):  
Zhigang Li ◽  
Weike Wang ◽  
Li Zhang ◽  
Zhaorong Yang ◽  
Mingliang Tian ◽  
...  

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