Non-trivial role of interlayer cation states in iron-based superconductors
arXiv:1610.08626 · doi:10.1103/PhysRevLett.118.017204
Abstract
Unconventional superconductivity in iron pnictides and chalcogenides has been suggested to be controlled by the interplay of low-energy antiferromagnetic spin fluctuations and the particular topology of the Fermi surface in these materials. Based on this premise, one would also expect the large class of isostructural and isoelectronic iron germanide compounds to be good superconductors. As a matter of fact, they, however, superconduct at very low temperatures or not at all. In this work we establish that superconductivity in iron germanides is suppressed by strong ferromagnetic tendencies, which surprisingly do not originate from changes in bond-angles or -distances with respect to iron pnictides and chalcogenides, but are due to changes in the electronic structure in a wide range of energies happening upon substitution of atom species (As by Ge and the corresponding spacer cations). Our results indicate that superconductivity in iron-based materials may not always be fully understood based on or model Hamiltonians only.
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Cited by in corpus (10)
- Iron-based superconductivity extended to the novel silicide LaFeSiH
- Emergent magnetic degeneracy in iron pnictides due to the interplay between spin-orbit coupling and quantum fluctuations
- Novel Fe-based superconductor LaFe2As2 in comparison with traditional pnictides
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- PhD Thesis: Electronic correlations in multiorbital systems