The angular dependence of critical currents in Nb3Sn — Effect of some preparation conditions

1977 ◽  
Vol 27 (5) ◽  
pp. 571-576 ◽  
Author(s):  
S. Takács ◽  
D. Čabelka ◽  
V. Černuško ◽  
M. Jergel
1977 ◽  
Vol 27 (4) ◽  
pp. 468-476 ◽  
Author(s):  
M. Jergel ◽  
D. čabelka ◽  
V. černuško ◽  
S. Takács ◽  
P. A. Cheremnykh ◽  
...  

1973 ◽  
Vol 23 (6) ◽  
pp. 644-651 ◽  
Author(s):  
M. Jergel ◽  
S. Takács ◽  
D. Čabelka ◽  
V. Černuško ◽  
J. KruŽliak

1995 ◽  
Vol 252 (3-4) ◽  
pp. 211-220 ◽  
Author(s):  
Q.Y. Hu ◽  
H.W. Weber ◽  
H.K. Liu ◽  
S.X. Dou ◽  
H.W. Neumüller

2007 ◽  
Vol 460-462 ◽  
pp. 1188-1189 ◽  
Author(s):  
K.R. Schöppl ◽  
H.W. Weber ◽  
J.H. Durrell

1994 ◽  
Vol 235-240 ◽  
pp. 2531-2532
Author(s):  
S. de Brion ◽  
W.R. White ◽  
A. Kapitulnik ◽  
M.R. Beasley

Author(s):  
D.J. Li ◽  
J.P. Zhang ◽  
L.C. Qin ◽  
L. D. Marks

A problems with bulk high temperature superconductors for some time has been obtaining specimens which show high critical currents; typical critical currents in bulk materials lie in the range of 103 Amps/cm2 whereas thin film specimens now routinely reach the 106 Amps/cm2 range. There has recently been indications of higher critical currents in some materials, with suggestions that there is flux pinning by 1/3(301) type defects. We have previously studied in some detail bulk materials with excess copper that contain large number of such defects. In the light of the recent results, we have returned to these materials to study the critical current in addition to the structure.Details of the specimen preparation will be reported elsewhere. The key point is that with the correct preparation conditions, the bulk materials show a fairly sharp transition at 9IK and magnetization measurements indicate (reproducibly) a Jc of more than 106 at 4.5K, using the total size of the specimen and not a smaller grain size.


1963 ◽  
Vol 132 (2) ◽  
pp. 577-580 ◽  
Author(s):  
G. W. Cullen ◽  
G. D. Cody ◽  
J. P. McEvoy

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