2010
DOI: 10.1088/0953-8984/22/6/065702
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Superconductivity in the Anderson lattice: a finite-Uslave boson description

Abstract: Using the Kotliar and Ruckenstein slave boson formalism we consider the finite-U Anderson lattice. We study the appearance of superconductivity as a function of the Coulomb repulsion, density and f-level location for s-wave and d-wave pairing symmetries. The results extend previous studies where the infinite-U limit was considered, confirming that superconductivity remains as the Coulomb coupling increases, if the attractive interaction is not weak. Superconductivity disappears for large U as the filling of th… Show more

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Cited by 9 publications
(17 citation statements)
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“…For instance, for n ≈ 0.5, as well as n ≈ 3.5 and even symmetry of hybridization, two superconducting regions are obtained: one with the usual initial decrease of the superconducting critical temperature with V and a second with a dome for higher values of hybridization. The Coulomb repulsion is also an important ingredient affecting superconductivity: for certain values of band-filling it can lead to a suppression of the superconducting phase, instead of a continuous asymptotic decrease as reported in previous works 8,20 .…”
Section: Discussionmentioning
confidence: 56%
See 1 more Smart Citation
“…For instance, for n ≈ 0.5, as well as n ≈ 3.5 and even symmetry of hybridization, two superconducting regions are obtained: one with the usual initial decrease of the superconducting critical temperature with V and a second with a dome for higher values of hybridization. The Coulomb repulsion is also an important ingredient affecting superconductivity: for certain values of band-filling it can lead to a suppression of the superconducting phase, instead of a continuous asymptotic decrease as reported in previous works 8,20 .…”
Section: Discussionmentioning
confidence: 56%
“…and where the square root term ensures that the mapping becomes trivial at the mean-field level in the non-interacting limit (U → 0). The usual procedure consists in taking a mean-field approach where we assume the slave bosons to be condensed 8,20,32 . Then all bosons operators are replaced by their expectation values as,…”
Section: The Modelmentioning
confidence: 99%
“…(1) shows the BCS-BEC crossover from the analysis of the order parameter amplitude and the chemical potential, as functions of the density of particles (not shown). It is worth also to point out that superconductivity can be enhanced by a small momentum-independent hybridization, as in heavy-fermions systems with large local Coulomb repulsion, or even with U ¼ 1, as shown, for example, using the slave boson formalism [24]. Since hybridization can be tuned by external parameters, increasingλ, by pressure or doping provides a mechanism not only for increasing the critical temperatures in d-wave superconductors but also to drive the BCS-BEC crossover.…”
Section: Enhancement Of Critical Temperature With a Non-symmetrical Hmentioning
confidence: 98%
“…This one-body mixing term can be tuned by external parameters such as pressure permitting the exploration of the phase diagram and quantum phase transitions of the model. The last term explicitly describes an effective attraction between f -electrons in neighboring sites (J ij > 0), which is responsible for superconductivity [9]. Notice that this term also describes antiferromagnetic (AF), xy-type, exchange interactions between these electrons, such that, magnetic and superconducting ground states are in competition.…”
Section: The Modelmentioning
confidence: 99%
“…The Anderson lattice model (ALM) is generally accepted as an appropriate model for describing both magnetic and superconducting instabilities [8,9,10,11,12] in strongly correlated multi-band systems. Many studies have shown that the pairing between the nearly localized d of f -electrons is the responsible for the appearance of superconductivity [13,14].…”
Section: Introductionmentioning
confidence: 99%