Abstract
We analyze the influence of randomness of local pair (LP) site energies on the superconducting properties of a mixture of coexisting local pairs and itinerant electrons coupled via charge exchange mechanism. It has been found that the diagonal disorder effects depend in a crucial way on the total particle concentration n and the LP level position Δ0. Depending on the parameters, the system can exhibit various types of superconducting behaviors, including the LP-like, intermediate (MIXED), and the BCS-like.
Similar content being viewed by others
REFERENCES
S. Robaszkiewicz, R. Micnas, and J. Ranninger, Phys. Rev. B 36 180 (1987); J. Ranninger and S. Robaszkiewicz, Physica B 135 468 (1985).
R. Micnas, J. Ranninger, and S. Robaszkiewicz, Rev. Mod. Phys. 62 113 (1990), and references therein.
R. Micnas and S. Robaszkiewicz, in NATO ASI Series E, Vol. 343, E. Kaldis, E. Liarokapis, and K. A. Müller, eds. Kluwer Academic, Dordrecht, The Netherlands, (1997), p. 31, and references therein.
V. B. Geshkenbein, L. B. Ioffe, and A. I. Larkin, Phys. Rev. B 55 3173 (1997).
P. Devillard and J. Ranninger, Phys. Rev. Lett. 84 5200 (2000); T. Domanski and J. Ranninger, Phys. Rev. B 63 134505 (2001).
G. Pawłowski and S. Robaszkiewicz, Mol. Phys. Rep. 34(1), 76 (2001); Phys. Stat. Sol. 236 400 (2003); T. Domanski and K. I. Wysokiński, Phys. Rev. B 66 064517 (2002).
R. Micnas, S. Robaszkiewicz, and A. Bussmann-Holder, Phys. Rev. B 66 104516 (2002).
S. Robaszkiewicz and G. Pawłowski, J. Supercond. 17(1), 37 (2004).
G. Pawłowski and S. Robaszkiewicz, Physica A 299 475 (2001).
G. Pawłowski, S. Robaszkiewicz, and R. Micnas, in preparation.
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Pawłowski, G., Robaszkiewicz, S. & Micnas, R. Superconductivity of the Induced Pairing Model in the Presence of Diagonal Disorder. Journal of Superconductivity 17, 33–36 (2004). https://doi.org/10.1023/B:JOSC.0000011836.87330.f3
Issue Date:
DOI: https://doi.org/10.1023/B:JOSC.0000011836.87330.f3