The Kohn-Luttinger superconductivity in idealized doped graphene
arXiv:1411.3795 · doi:10.1016/j.ssc.2014.03.001
Abstract
Idealized graphene monolayer is considered neglecting the van der Waals potential of the substrate and the role of the nonmagnetic impurities. The effect of the long-range Coulomb repulsion in an ensemble of Dirac fermions on the formation of the superconducting pairing in a monolayer is studied in the framework of the Kohn-Luttinger mechanism. The electronic structure of graphene is described in the strong coupling Wannier representation on the hexagonal lattice. We use the Shubin-Vonsowsky model which takes into account the intra- and intersite Coulomb repulsions of electrons. The Cooper instability is established by solving the Bethe-Salpeter integral equation, in which the role of the effective interaction is played by the renormalized scattering amplitude. The renormalized amplitude contains the Kohn-Luttinger polarization contributions up to and including the second-order terms in the Coulomb repulsion. We construct the superconductive phase diagram for the idealized graphene monolayer and show that the Kohn-Luttinger renormalizations and the intersite Coulomb repulsion significantly affect the interplay between the superconducting phases with , , and wave symmetries of the order parameter.
9 pages, 5 figures
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- Electronic Structure and Kohn-Luttinger Superconductivity of Heavily-Doped Single-Layer Graphene
- Kohn-Luttinger superconductivity in monolayer and bilayer semimetals with the Dirac spectrum
- Renormalization-group approach to the Kohn-Luttinger superconductivity: Amplification of the pairing gap from to
- Pairing around a Single Dirac Point: A Unifying View of Kohn-Luttinger Superconductivity in Chern Bands, Quarter Metals, and Topological Surface States