EPR Study of the Local Magnetic Field Distribution over the Bi2Sr2Ca1−x Y x Cu2O8+y Crystal Surface above the Superconducting Transition Temperature

2015 ◽  
Vol 46 (8) ◽  
pp. 897-907 ◽  
Author(s):  
Y. Talanov ◽  
L. Salakhutdinov ◽  
T. Adachi ◽  
T. Noji ◽  
Y. Koike
1999 ◽  
Vol 13 (29n31) ◽  
pp. 3715-3717 ◽  
Author(s):  
D. G. NAUGLE ◽  
K. D. D. RATHNAYAKA ◽  
K. CLARK ◽  
P. C. CANFIELD

In-plane resistance as a function of magnitude and direction of the magnetic field and the temperature has been measured for TmNi2B2C from above the superconducting transition temperature at 10.7 K to below the magnetic transition TN=1.5 K. The superconducting upper critical field HC2(T) exhibits a large anisotropy and structure in the vicinity of TN. The magnetoresistance above TC is large and changes sign as the direction of the magnetic field is rotated from in-plane to parallel with the c-axis.


1991 ◽  
Vol 6 (6) ◽  
pp. 1135-1147 ◽  
Author(s):  
Thomas R. Askew ◽  
Richard B. Flippen ◽  
Kevin J. Leary ◽  
Milind N. Kunchur

The transport critical current density Jc has been measured in high quality polycrystalline YBa2Cu3O7 samples made from extruded preforms. The hysteretic response of Jc to applied magnetic fields was studied as a function of temperature (77–87 K) and sample morphology for various field sweeps in the 0–5 KOe range. A variety of samples show a basic Jc ∼ H−n behavior where n depends on temperature, but is independent of the other variables. A simple model of the local magnetic field distribution is presented and compared to the data, and the theoretical implications of the power law behavior are considered.


2005 ◽  
Vol 2 (5) ◽  
pp. 1644-1649 ◽  
Author(s):  
A. Chiodoni ◽  
L. Gozzelino ◽  
F. Laviano ◽  
P. Przyslupski ◽  
A. Tsarev ◽  
...  

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