Dielastic interaction of the flux line lattice with internal stresses of crystal imperfections. II. Second-order interaction force between flux lines and crystal dislocations

1978 ◽  
Vol 31 (3-4) ◽  
pp. 357-373 ◽  
Author(s):  
E. Schneider
1972 ◽  
Vol 50 (5) ◽  
pp. 421-427 ◽  
Author(s):  
R. I. Coote ◽  
J. E. Evetts ◽  
A. M. Campbell

The pinning of flux lines by large normal particles has been investigated as a function of field and temperature. The results are compared with a model for the magnetic pinning interaction at a phase boundary. The problem of the summation procedure for individual pinning interactions is discussed and it is concluded that the distortion of the flux line lattice caused by large normal particles is large enough for a simple direct summation to apply. This conclusion is supported by the experimental results. The experimental results also indicate that Anderson flux creep is not significant in this type of pinning system.


2005 ◽  
Vol 19 (23) ◽  
pp. 3575-3601
Author(s):  
A. M. ETTOUHAMI

We study translational correlations of the vortex center of mass positions of the Abrikosov flux line lattice in superconducting samples of finite thickness L (along the direction of flux lines). The Larkin correlation lengths for the center of mass mode of the flux lines in the presence of point and correlated disorder are computed, and we find that in the case of point disorder the average (i.e. center of mass) position of flux lines maintains positional order on length scales which scale like [Formula: see text] in 2+1 dimensions. On still longer length scales, however, we find using a replica Gaussian variational approach that center of mass correlations cross over to a power law growth of the form r⊥/L, which should be observable in superconducting thin films.


2000 ◽  
Vol 276-278 ◽  
pp. 818-819
Author(s):  
P. Manuel ◽  
A.D. Hillier ◽  
S.H. Kilcoyne

2000 ◽  
Vol 61 (18) ◽  
pp. 12394-12403 ◽  
Author(s):  
S. Sarkar ◽  
D. Pal ◽  
S. S. Banerjee ◽  
S. Ramakrishnan ◽  
A. K. Grover ◽  
...  

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