Die Methode der Korrelationsfunktion in der Theorie der Supraleitung

1966 ◽  
Vol 21 (11) ◽  
pp. 1842-1849 ◽  
Author(s):  
Gerhart Lüders

The method of correlation function is extended to the case of paramagnetic impurities. The BOLTZMANN equation is obtained and subsequently applied to a derivation of the concentration dependence of the transition temperature, of the linearized GINZBURG—LANDAU equation, and of the diffusion approximation.


1966 ◽  
Vol 21 (9) ◽  
pp. 1415-1425 ◽  
Author(s):  
Gerhart Lüders

The method of correlation function is, without complete justification, extended to superconductors in the presence of a magnetic field. Applying this method, we derive the linearized and generalized GINZBURG—LANDAU equation and DE GENNES’ diffusion approximation in simple way. The results agree with those obtained previously by DE GENNES, GORKOV, MAKI, TEWORDT, and others. In special cases (no magnetic field, pure superconductor or isotropic scattering) they can also be derived from WERTHAMER’S kernel. In connection with this kernel, we discuss the limits of validity of both the linearized and generalized GINZBURG—LANDAU equation and of the diffusion approximation.



1998 ◽  
Vol 12 (10) ◽  
pp. 1069-1095 ◽  
Author(s):  
Wonkee Kim ◽  
C. S. Ting

Ginzburg–Landau (GL) equations for a d-wave superconductor with a repulsive s-wave interaction between electrons in the presence of paramagnetic impurities are microscopically derived based on the Born approximation. The diagrammatic relationships for the impurity-averaged product of Green's functions are algebraically established. The effect of paramagnetic impurities on the transition temperature and the London penetration depth are discussed. GL equations for a superconductor with both s-wave and d-wave pairing interactions are also examined. We show that the transition temperature for a superconductor with an s-wave symmetry is suppressed twice as rapidly as that with a d-wave symmetry in the dilute impurity limit if the strength of the spin-non-flip scattering is much weaker than the spin-flip interaction.





1969 ◽  
Vol 3 (3) ◽  
pp. 377-385
Author(s):  
M. J. Bell ◽  
M. D. Kostin

A stochastic method has been employed to investigate the distribution function of free electrons in gases in the field of a positive ion. Stochastic results have been obtained for several pressures and for both large (Langevin) and small ions, and the results have been compared with the solutions of the diffusion approximation and Pitaevskii's Fokker—Planck approximation to the Boltzmann equation.



1979 ◽  
Vol 50 (5) ◽  
pp. 3185-3188 ◽  
Author(s):  
J. H. Jacob ◽  
B. N. Srivastava ◽  
M. Rokni ◽  
J. A. Mangano






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