scholarly journals Persistent currents in the presence of a transport current

1995 ◽  
Vol 51 (15) ◽  
pp. 10175-10178 ◽  
Author(s):  
A. M. Jayannavar ◽  
P. Singha Deo
Author(s):  
T. F. Kelly ◽  
P. J. Lee ◽  
E. E. Hellstrom ◽  
D. C. Larbalestier

Recently there has been much excitement over a new class of high Tc (>30 K) ceramic superconductors of the form A1-xBxCuO4-x, where A is a rare earth and B is from Group II. Unfortunately these materials have only been able to support small transport current densities 1-10 A/cm2. It is very desirable to increase these values by 2 to 3 orders of magnitude for useful high field applications. The reason for these small transport currents is as yet unknown. Evidence has, however, been presented for superconducting clusters on a 50-100 nm scale and on a 1-3 μm scale. We therefore planned a detailed TEM and STEM microanalysis study in order to see whether any evidence for the clusters could be seen.A La1.8Sr0.2Cu04 pellet was cut into 1 mm thick slices from which 3 mm discs were cut. The discs were subsequently mechanically ground to 100 μm total thickness and dimpled to 20 μm thickness at the center.


2001 ◽  
Vol 86 (14) ◽  
pp. 3124-3127 ◽  
Author(s):  
W. Rabaud ◽  
L. Saminadayar ◽  
D. Mailly ◽  
K. Hasselbach ◽  
A. Benoît ◽  
...  
Keyword(s):  

1996 ◽  
Vol 10 (28) ◽  
pp. 1397-1406 ◽  
Author(s):  
AXEL VÖLKER ◽  
PETER KOPIETZ

We use the Lanczos method to calculate the variance σ2(E, ϕ) of the number of energy levels in an energy window of width E below the Fermi energy for noninteracting disordered electrons on a thin three-dimensional ring threaded by an Aharonov–Bohm flux ϕ. We confirm numerically that for small E the flux-dependent part of σ2(E, ϕ) is well described by the Altshuler–Shklovskii-diagram involving two Cooperons. However, in the absence of electron–electron interactions this result cannot be extrapolated to energies E where the energy-dependence of the average density of states becomes significant. We discuss consequences for persistent currents and argue that for the calculation of the difference between the canonical- and grand canonical current it is crucial to take the electron–electron interaction into account.


1996 ◽  
Vol 46 (S5) ◽  
pp. 2823-2824 ◽  
Author(s):  
B. J. Vleeming ◽  
A. V. Zakarian ◽  
A. N. Omelyanchouk ◽  
R. de Bruyn Ouboter
Keyword(s):  

2013 ◽  
Vol 88 (5) ◽  
Author(s):  
A. I. Yakimenko ◽  
K. O. Isaieva ◽  
S. I. Vilchinskii ◽  
M. Weyrauch

2010 ◽  
Vol 20 (3) ◽  
pp. 1300-1303 ◽  
Author(s):  
Jun Ogawa ◽  
Satoshi Fukui ◽  
Tetsuo Oka ◽  
Takao Sato ◽  
Kazuya Shinkai ◽  
...  

1997 ◽  
Vol 55 (24) ◽  
pp. 16300-16305 ◽  
Author(s):  
Jia-Lin Zhu ◽  
Xi Chen ◽  
Yoshiyuki Kawazoe

2021 ◽  
Vol 11 (6) ◽  
pp. 2741
Author(s):  
Sergey Zanegin ◽  
Nikolay Ivanov ◽  
Vasily Zubko ◽  
Konstantin Kovalev ◽  
Ivan Shishov ◽  
...  

The article is devoted to the study of losses in devices based on high-temperature superconductors of the 2nd generation. The complexity of the devices under study increases from a single rack coil to a winding assembled from several coils, and finally to an electric machine operating in generator mode. This is the way to experimentally study the behavior of 2nd generation high temperature superconductor (2G HTS) carrying a transport current in various conditions: self-field, external DC, and AC magnetic field. Attention is also paid to the losses in the winding during its operation from the inverter, which simulates the operating conditions in the motor mode of a propulsion system.


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