scholarly journals UPt3: Specific heat, critical fields, and the Ginzburg-Landau models for the superconducting phase diagram

1993 ◽  
Vol 48 (9) ◽  
pp. 6385-6399 ◽  
Author(s):  
T. Vorenkamp ◽  
A. de Visser ◽  
R. Wester ◽  
A. A. Menovsky ◽  
J. J. M. Franse ◽  
...  
2006 ◽  
Vol 73 (10) ◽  
Author(s):  
K. Grube ◽  
S. Drobnik ◽  
C. Pfleiderer ◽  
H. v. Löhneysen ◽  
E. D. Bauer ◽  
...  

1990 ◽  
Vol 81 (5-6) ◽  
pp. 299-315 ◽  
Author(s):  
K. Hasselbach ◽  
A. Lacerda ◽  
K. Behnia ◽  
L. Taillefer ◽  
J. Flouquet ◽  
...  

Coatings ◽  
2021 ◽  
Vol 11 (5) ◽  
pp. 507
Author(s):  
Vasiliy N. Kushnir ◽  
Serghej L. Prischepa ◽  
Michela Trezza ◽  
Carla Cirillo ◽  
Carmine Attanasio

The stray fields produced by ferromagnetic layers in Superconductor/Insulator/Ferromagnet (S/I/F) heterostructures may strongly influence their superconducting properties. Suitable magnetic configurations can be exploited to manipulate the main parameters of the hybrids. Here, the nucleation of the superconducting phase in an external magnetic field that periodically oscillates along the film width is studied on the base of the numerical solution of the linearized system of Usadel equations. In addition, the effect of the magnetic configuration of the F-layer on the temperature dependence of the critical current density, Jc(T), is investigated in the framework of the Ginzburg–Landau phenomenological theory on the base of the oscillating model of a stray field. By following this approach, the Jc(T) dependence of a Nb/SiO2/PdNi trilayer is reproduced for different magnetic configurations of the PdNi layer.


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

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.


1993 ◽  
Vol 71 (12) ◽  
pp. 1957-1957 ◽  
Author(s):  
I. Luk’yanchuk ◽  
M. Sigrist ◽  
M. Zhitomirsky

2013 ◽  
Vol 103 (1) ◽  
pp. 17001 ◽  
Author(s):  
Joshua D. Bocarsly ◽  
Daigorou Hirai ◽  
M. N. Ali ◽  
R. J. Cava

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