
arXiv: cond-mat/0607303
handle: 11588/900129 , 10446/21489
We propose a simple model for superconductors endowed with two critical temperatures, corresponding to two second-order phase transitions, in the framework of the Ginzburg-Landau mean-field theory. For very large Cooper pair self-interaction, in addition to the standard condensation occurring in the Ginzburg-Landau theory, we find another phase transition at a lower temperature with a maximum difference of 15% between the two critical temperatures.
revtex, 3 pages, one eps figure
High Energy Physics - Theory, Superconductivity (cond-mat.supr-con), High Energy Physics - Phenomenology, High Energy Physics - Phenomenology (hep-ph), High Energy Physics - Theory (hep-th), Theories and models of superconducting state;Phenomenological theories (two-fluid, Ginzburg-Landau, etc.);Spontaneous breaking of gauge symmetries, Condensed Matter - Superconductivity, FOS: Physical sciences
High Energy Physics - Theory, Superconductivity (cond-mat.supr-con), High Energy Physics - Phenomenology, High Energy Physics - Phenomenology (hep-ph), High Energy Physics - Theory (hep-th), Theories and models of superconducting state;Phenomenological theories (two-fluid, Ginzburg-Landau, etc.);Spontaneous breaking of gauge symmetries, Condensed Matter - Superconductivity, FOS: Physical sciences
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