scholarly journals The Superconducting Order Parameter in High-Tc Superconductors – A Point-Contact Spectroscopy Viewpoint

Author(s):  
M. Tortello ◽  
D. Daghero
1996 ◽  
Vol 46 (S2) ◽  
pp. 711-712
Author(s):  
Yuri G. Naidyuk ◽  
Hilbert von Löhneysen ◽  
Igor K. Yanson

1988 ◽  
Vol 153-155 ◽  
pp. 1381-1382 ◽  
Author(s):  
N. Hohn ◽  
R. Koltun ◽  
H. Schmidt ◽  
S. Blumenro¨der ◽  
H. General ◽  
...  

1988 ◽  
Vol 153-155 ◽  
pp. 1389-1390 ◽  
Author(s):  
P. Nozar ◽  
M. Solanki-Moser ◽  
E. Kaldis ◽  
P. Wachter

1989 ◽  
Vol 169 ◽  
Author(s):  
Xinsheng Ling ◽  
M. E. Filipkowski ◽  
E. K. Heller ◽  
J. I. Budnick

AbstractWe have studied the variation of dissipative effects with doping in the high Tc superconductors La2-xSrxCuO4-y and YBa2Cu3O7-y by studying the lossy component of ac susceptibility as a function of temperature. We find relatively strong excess losses at low temperature in both systems, which indicate stronger flux creep at grain boundaries, in lower level doped ceramic samples produced by a similar process. This effect is more significant in the La2-xSrxCuO4-y (214) system than in the YBa2Cu3O7-y(123) system. We suggest that the microscopic mechanisms of weakening of the order parameter in the grain boundaries may be different in the two systems. In the 214 system, as the charge carrier density in the CuO2 planes is reduced, the spatial fluctuation of the order parameter in the CuO2 planes is enhanced. In the 123 system, the initial removal of O from the sample, which weakens the coupling between planes and increases the spatial fluctuation of the order parameter between CuO2 planes. The grain boundaries are degraded in both systems. The degradation in the 214 samples is more significant than in the 123 samples.


1994 ◽  
Vol 235-240 ◽  
pp. 1881-1882 ◽  
Author(s):  
Y. Kitaoka ◽  
K. Ishida ◽  
G.-q. Zheng ◽  
S. Ohsugi ◽  
K. Yamazoe ◽  
...  

1998 ◽  
Vol 12 (29n31) ◽  
pp. 3027-3030
Author(s):  
Alexander B. Nazarenko ◽  
Ernst A. Pashitskii ◽  
Alexander E. Pashitskii

We show that the zero-bias conductance peak observed in tunnel and point junctions of cuprates can be a consequence of "unitary" elastic scattering of the carriers by non-magnetic impurities in the vicinity of the junction interface and d-wave symmetry of the order parameter.


Sign in / Sign up

Export Citation Format

Share Document