Least momentum space frustration as a condition for "high sweet spot" in the iron-based superconductors
arXiv:1204.1717 · doi:10.1088/0953-2048/25/8/084004
Abstract
In the present paper, we describe how the band structure and the Fermi surface of the iron-based superconductors vary as the Fe-As-Fe bond angle changes. We discuss how these Fermi surface configurations affect the superconductivity mediated by spin fluctuations, and show that in several situations, frustration in the sign of the gap function arises due to the repulsive pairing interactions that requires sign change of the order parameter. Such a frustration can result in nodes or very small gaps, and generally works destructively against superconductivity. Conversely, we propose that the optimal condition for superconductivity is realized for the Fermi surface configuration that gives the least frustration while maximizing the Fermi surface multiplicity. This is realized when there are three hole Fermi surfaces, where two of them have orbital character and one has {\it for all } in the three dimensional Brillouin zone. Looking at the band structures of various iron-based superconductors, the occurrence of such a "sweet spot" situation is limited to a narrow window.
9 figures, submitted to focus issue, SUST
References in corpus (13)
- Unconventional pairing originating from disconnected Fermi surfaces in superconducting LaFeAsOF}
- LaFeAsOF: A low carrier density superconductor near itinerant magnetism
- Near-degeneracy of several pairing channels in multiorbital models for the Fe-pnictides
- Effect of Structural Parameters on Superconductivity in Fluorine-Free LnFeAsO1-y (Ln=La,Nd)
- A review of Fe-chalcogenide superconductors: the simplest Fe-based superconductor
- Bandwidth and Fermi surface of Iron-Oxypnictides: covalency and sensitivity to structural changes
- On the multi-orbital band structure and itinerant magnetism of iron-based superconductors
- Nodes in the Gap Function of LaFePO, the Gap Function of the Fe(Se,Te) Systems, and the STM Signature of the s Pairing
- Superconductivity at 28.3 and 17.1 K in (Ca4Al2O6-y)(Fe2Pn2) (Pn = As and P)
- The Delicate Electronic and Magnetic Structure of the LaOFePn System (Pn = pnictogen)
- Maximizing Fermi surface multiplicity optimizes superconductivity in iron pnictides
- Electronic Structure of Novel Superconductor Ca4Al2O6Fe2As2
- First-principles Electronic Structure of Superconductor CaAlOFeP: Comparison with LaFePO and CaAlOFeAs
Cited by in corpus (9)
- Iron-Based Superconductors: current status of materials and pairing mechanism
- Model of the Electronic Structure of Electron-Doped Iron-Based Superconductors: Evidence for Enhanced Spin Fluctuations by Diagonal Electron Hopping
- The electronic specific heat of Ba1-xKxFe2As2 (x=0 to 1.0) from 2K to 380K
- The poisoning effect of Mn in LaFe(1-x)Mn(x)AsO(0.89)F(0.11): unveiling a quantum critical point in the phase diagram of iron-based superconductors
- Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H-substitution
- Hidden robust presence of a hole Fermi surface in a heavily electron doped iron based superconductor LaFeAs
- NMR Investigation of the iron-based superconductors Ca4(Mg,Ti)3Fe2As2O8-y and Ca5(Sc,Ti)4Fe2As2O11-y
- Understanding the re-entrant superconducting phase diagram of an iron-pnictide CaAlOFe(AsP)
- Observation of the bands with orbital character near the Fermi level in NdFeAsPOF using angle-resolved photoemission spectroscopy