1982
DOI: 10.1007/bf01014801
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Equations of superconductivity for transition metals in the Wannier representation

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Cited by 7 publications
(18 citation statements)
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“…We derive the equations for superconductivity in the site representation by means of the irreducible Green's function method 33-35 in Section 2, using ideas developed previously in connection with the derivation of Eliashberg-type equations for pure transition metals in the Wannier representation. 35 Various attempts at configurational averaging are discussed in Section 3, where the formula for Tc is also obtained. Section 4 contains a discussion and conclusions.…”
Section: Introductionmentioning
confidence: 99%
“…We derive the equations for superconductivity in the site representation by means of the irreducible Green's function method 33-35 in Section 2, using ideas developed previously in connection with the derivation of Eliashberg-type equations for pure transition metals in the Wannier representation. 35 Various attempts at configurational averaging are discussed in Section 3, where the formula for Tc is also obtained. Section 4 contains a discussion and conclusions.…”
Section: Introductionmentioning
confidence: 99%
“…One should note that the BCS-Bogoliubov superconductivity theory [1,3,5,10,15] is formulated in terms of a trial (approximating) Hamiltonian H mod , which is a quadratic form with respect to the second-quantized creation and annihilation operators, including the terms responsible for anomalous (or non-diagonal) averages. For the single-band Hubbard model the BCS-Bogoliubov functional of generalized mean fields can be written in the following form [92,93,94,95]…”
Section: The Mean Field Conceptmentioning
confidence: 99%
“…It is important to emphasize that the BCS-Bogolyubov theory of superconductivity [12,41,42] was formulated on the basis of a trial Hamiltonian which consists of a quadratic form of creation and annihilation operators, including "anomalous" (off-diagonal) averages. The functional of the mean field (for the superconducting single-band Hubbard model) is of the following form [57]:…”
Section: Effective and Generalized Mean Fieldsmentioning
confidence: 99%
“…It is important to emphasize that the BCS-Bogolyubov theory of superconductivity [12,41,42] was formulated on the basis of a trial Hamiltonian which consists of a quadratic form of creation and annihilation operators, including "anomalous" (off-diagonal) averages [13]. The strong-coupling BCS-Bogolyubov theory of superconductivity was formulated for the Hubbard model in the localized Wannier representation in [57,60,61]. Therefore, instead of the algebra of the operator of a normal state a iσ , a motivated an intensification of research in superconductivity, not only because applications are promising, but because they also represent a new state of matter that breaks certain fundamental symmetries.…”
Section: -15mentioning
confidence: 99%
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