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High-Tc superconductivity via superpropagators revisited
We revisit our earlier paper because it was perceived in some quarters to be based on a formulation that took into account the electron-pairs (e-pairs), but not the hole-pairs (h-pairs). Through a more comprehensive study of the basic equation on which our earlier work was based, we present here tem...
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Published in: | Physica. C, Superconductivity Superconductivity, 2008-07, Vol.468 (13), p.949-954 |
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Main Author: | |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We revisit our earlier paper because it was perceived in some quarters to be based on a formulation that took into account the electron-pairs (e-pairs), but not the hole-pairs (h-pairs). Through a more comprehensive study of the basic equation on which our earlier work was based, we present here temperature-generalized equations for the Bethe–Salpeter amplitudes for Cooper pairs (CPs) of the (e–e), (h–h), and (e–h/h–e) varieties (our earlier paper seemed to deal with only the first category of pairs). We then show that solution of the (e–e) or the (h–h) equation, at T=0, yields a pair of pure imaginary binding energies (W); this result is in agreement with the one obtained long ago by Thouless, by Abrikosov et al., by Schrieffer, and others, and signifies that both the e-pairs and the h-pairs have been taken into account in our work. A salient feature of our approach is that it determines the all-important Tc and Hc in the limit of vanishing W whereas, in the BCS theory, Tc is obtained in the limit gap→0, and Hc is determined via the condensation energy of the CPs. |
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ISSN: | 0921-4534 1873-2143 |
DOI: | 10.1016/j.physc.2008.03.002 |