Line node positions of the superconducting gap function ofUPd2Al3

2009 ◽  
Vol 79 (13) ◽  
Author(s):  
Peter Thalmeier ◽  
David Parker
2018 ◽  
Vol 123 (5) ◽  
pp. 57001 ◽  
Author(s):  
Y. T. Shao ◽  
X. X. Wu ◽  
L. Wang ◽  
Y. G. Shi ◽  
J. P. Hu ◽  
...  

2011 ◽  
Vol 7 (3) ◽  
pp. 198-202 ◽  
Author(s):  
Y-M. Xu ◽  
Y-B. Huang ◽  
X-Y. Cui ◽  
E. Razzoli ◽  
M. Radovic ◽  
...  

2003 ◽  
Vol 17 (18n20) ◽  
pp. 3373-3376
Author(s):  
Hidemi Nagao ◽  
Hiroyuki Kawabe ◽  
Sergei P. Kruchinin ◽  
Kizashi Yamaguchi

We investigate the superconductivity in a two-band model by using the renormalization group approach. We discuss the superconducting gap function in the two-band model.


2011 ◽  
Vol 170 ◽  
pp. 118-121
Author(s):  
H. Okuyama ◽  
K. Takase ◽  
Yoshiki Takano ◽  
Tadataka Watanabe ◽  
Fumiko Yoshida ◽  
...  

We performed experimentally the electron-density mapping on the crystal structure of the iron-based superconductor Lu2Fe3Si5 which revealed the Fe-Si covalent-bonding network with the fully ionized Lu-sites. And, for Lu2Fe3Si5, we investigated the effect of Fe- and Si-site substitutions on the superconductivity. The Fe-site-substitution study revealed that, in addition to the disorder-sensitive superconductivity, the additionally-provided 3d electrons or holes tend to be itinerant rather than localized. Taking into account that the localized magnetic moments introduced on the Lu-sites are inactive as magnetic pair breakers, the present results suggest that, in Lu2Fe3Si5, the Fe-Si bonding network should be the playground for the exotic superconductivity which is characterized by the sign-reversed superconducting gap function.


1995 ◽  
Vol 140-144 ◽  
pp. 1275-1276
Author(s):  
L. Kowalewski ◽  
M.M. Nogala ◽  
M. Thomas ◽  
R.J. Wojciechowski

2006 ◽  
Vol 97 (5) ◽  
Author(s):  
E. Blackburn ◽  
A. Hiess ◽  
N. Bernhoeft ◽  
M. C. Rheinstädter ◽  
W. Häußler ◽  
...  

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