On magnetic flux dynamics in 1D arrays of underdamped Josephson junctions

1993 ◽  
Vol 183 (5-6) ◽  
pp. 383-389 ◽  
Author(s):  
M. Cirillo ◽  
Britt H. Larsen ◽  
A.V. Ustinov ◽  
V. Merlo ◽  
V.A. Oboznov ◽  
...  
1994 ◽  
Vol 235-240 ◽  
pp. 285-288 ◽  
Author(s):  
A.V. Ustinov ◽  
H. Kohlstedt ◽  
C. Heiden

JETP Letters ◽  
2000 ◽  
Vol 72 (1) ◽  
pp. 26-29 ◽  
Author(s):  
S. M. Ishikaev ◽  
É. V. Matizen ◽  
V. V. Ryazanov ◽  
V. A. Oboznov ◽  
A. V. Veretennikov

1998 ◽  
Vol 72 (12) ◽  
pp. 1513-1515 ◽  
Author(s):  
Y. Chong ◽  
B. Ruck ◽  
R. Dittmann ◽  
C. Horstmann ◽  
A. Engelhardt ◽  
...  

Science ◽  
1994 ◽  
Vol 263 (5150) ◽  
pp. 1112-1114 ◽  
Author(s):  
G. M. Fischer ◽  
B. Mayer ◽  
R. Gross ◽  
T. Nissel ◽  
K. -D. Husemann ◽  
...  

1992 ◽  
Vol 290 ◽  
Author(s):  
M. R. Freeman

AbstractA fast time-domain magneto-optical technique is used to explore magnetic flux dynamics in the optically driven nonequilibrium state of Type I superconducting Pb films. It is found that the effective penetration of flux through the nonequilibrium intermediate state can be dramatically faster than through the normal metal. The system is probed through the application of rapid transient magnetic field pulses. Above the superconducting transition temperature, a direct measure of the diffusion coefficient of the magnetic field in the normal metal is obtained, on a time scale where the inhomogeneous spatial distribution of scattering sites is relevant. In the nonequilibrium superconductor the observations are dominated by coupling of the field transients to local motion of magnetic flux threading the normal domains. Studies as a function of how far the system is driven from equilibrium, and of the effect of a static applied magnetic field, indicate that the observations reflect the dynamics of normal/superconducting interfaces, and are strongly dependent on the microscopic arrangement of the intermediate state. By contrasting the response of pure Pb films to that of Pb1−xInx alloys, a comparison to Type II superconductivity is made.


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