Superconducting phase diagram of a narrow-band system atT=0: A mean-field study

1993 ◽  
Vol 48 (22) ◽  
pp. 16673-16679 ◽  
Author(s):  
A. N. Das ◽  
Sujit Sarkar ◽  
P. Choudhury
1988 ◽  
Vol 37 (16) ◽  
pp. 9410-9422 ◽  
Author(s):  
R. Micnas ◽  
J. Ranninger ◽  
S. Robaszkiewicz ◽  
S. Tabor

1997 ◽  
Vol 79 (13) ◽  
pp. 2486-2489 ◽  
Author(s):  
Silvio Franz ◽  
Giorgio Parisi

2005 ◽  
Vol 19 (01n03) ◽  
pp. 119-121 ◽  
Author(s):  
HONG-WEI CHEN ◽  
QIANG HAN ◽  
Z. D. WANG

The superconducting system in the two dimensional triangular lattice is investigated by the mean-field treatment of a simple effective model. We calculate the phase diagram of this kind of superconductor for various pairing symmetries and interactions as well as electron occupancies. It is found that the px+ipy-, d+id′-, and f- wave superconducting states are stabilized in different doping regions, and there exist superconducting phase transitions by varying the carrier concentration in the system. The relevance of our results to the recently discovered superconductor, Na x CoO 2·y H 2 O , is briefly discussed.


2019 ◽  
Author(s):  
C. Tejera-Centeno ◽  
P. Pérez-Fernández ◽  
J. M. Arias
Keyword(s):  

2019 ◽  
Vol 3 (8) ◽  
Author(s):  
Bin Liu ◽  
Chengcheng Xiao ◽  
Qinqing Zhu ◽  
Jifeng Wu ◽  
Yanwei Cui ◽  
...  

2019 ◽  
Vol 122 (12) ◽  
Author(s):  
D. Geffroy ◽  
J. Kaufmann ◽  
A. Hariki ◽  
P. Gunacker ◽  
A. Hausoel ◽  
...  

2001 ◽  
Vol 16 (17) ◽  
pp. 1129-1138 ◽  
Author(s):  
M. SADZIKOWSKI

The Nambu–Bogoliubov–de Gennes method is applied to the problem of superconducting QCD. The effective quark–quark interaction is described within the framework of the Nambu–Jona-Lasinio model. The details of the phase diagram are given as a function of the strength of the quark–quark coupling constant G′. It is found that there is no superconducting phase transition when one uses the relation between the coupling constants G′ and G of the Nambu–Jona-Lasinio model which follows from the Fierz transformation. However, for other values of G′ one can find a rich phase structure containing both the chiral and the superconducting phase transitions.


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