Granular superconductivity inR1Ba2Cu3O7−δthin films

1988 ◽  
Vol 38 (10) ◽  
pp. 7125-7128 ◽  
Author(s):  
P. England ◽  
T. Venkatesan ◽  
X. D. Wu ◽  
A. Inam
1988 ◽  
Vol 02 (08) ◽  
pp. 1011-1015
Author(s):  
YONG ZHAO ◽  
QIRUI ZHANG ◽  
WEIYAN GUAN ◽  
JIANSHENG XIA ◽  
ZHENHUI HE ◽  
...  

The dependence of the resistance on the magnetic field and the current-voltage characteristics of the single phase Ba 2 YCu 3 O 7−δ have been measured. The nonmonotonic behavior and a hysteresis of R(H) and the current-voltage characteristics suggest that the granular superconductivity exist in this material, and it plays an important role in transport properties.


2010 ◽  
Vol 43 (37) ◽  
pp. 374019 ◽  
Author(s):  
B L Willems ◽  
G Zhang ◽  
J Vanacken ◽  
V V Moshchalkov ◽  
S D Janssens ◽  
...  

2014 ◽  
Vol 115 (22) ◽  
pp. 223910 ◽  
Author(s):  
Alberto Riminucci ◽  
Walther Schwarzacher

1991 ◽  
Vol 05 (16) ◽  
pp. 1105-1108
Author(s):  
C. X. FAN ◽  
K. W. WONG

The property of periodic magnetic field dependence observed on high temperature material is temperature sensitive. Experimental results show a linear relationship between τ2 and T4, where τ is the rf quantum interference period and T is temperature. This relation emerge from the entirety of weaklinks network system of granular superconductivity.


1998 ◽  
Vol 12 (29n31) ◽  
pp. 3074-3079 ◽  
Author(s):  
Howard A. Blackstead ◽  
John D. Dow ◽  
Israel Felner ◽  
H. Luo ◽  
David B. Pulling ◽  
...  

Pr 2-z Ce z Sr2Cu2NbO10 (Pr222Nb10), is widely believed to not superconduct, although its homologues in which Pr is replaced by Nd, Sm, Eu, or Gd do (with Tc ≈ 28 K). On the basis of bulk resistivity, bulk diamagnetism, electron spin resonance, and surface resistance measurements of Pr222Nb10, we conclude that it does exhibit granular superconductivity (as predicted) with a critical temperature in the range 25–28 K, but is not currently a bulk superconductor. Neutron diffraction studies show that our Pr222Nb10 is multi-phase, but does not contain significant amounts of any (known) superconducting phase other than Pr222Nb10. It does contain ~ 23% PrSr defects, but far fewer SrPr impurities (<2%), so that the predicted antistructure defect ( SrPr , PrSr ) is probably not responsible for breaking Cooper pairs and destroying superconductivity, but the important half of it, PrSr , almost certainly is.


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