Fermi surface pockets in electron-doped iron superconductor by Lifshitz transition
Jose P. Rodriguez, Ronald Melendrez

TL;DR
This paper models the Fermi surface evolution in electron-doped iron selenide superconductors, revealing a Lifshitz transition driven by strong correlations and magnetic frustration, consistent with experimental observations.
Contribution
It introduces an extended Hubbard model capturing Fermi surface pockets and predicts a Lifshitz transition with experimental relevance in iron selenide superconductors.
Findings
Fermi surface pockets are explained by the model.
Lifshitz transition occurs with increasing on-site repulsion.
Low-energy spin excitations form a 'floating ring' around (pi,pi).
Abstract
The Fermi surface pockets that lie at the corner of the two-iron Brillouin zone in heavily electron-doped iron selenide superconductors are accounted for by an extended Hubbard model over the square lattice of iron atoms that includes the principal 3d xz and 3d yz orbitals. At half filling, and in the absence of intra-orbital next-nearest neighbor hopping, perfect nesting between electron-type and hole-type Fermi surfaces at the the center and at the corner of the one-iron Brillouin zone is revealed. It results in hidden magnetic order in the presence of magnetic frustration within mean field theory. An Eliashberg-type calculation that includes spin-fluctuation exchange finds that the Fermi surfaces undergo a Lifshitz transition to electron/hole Fermi surface pockets centered at the corner of the two-iron Brillouin zone as on-site repulsion grows strong. In agreement with angle-resolved…
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