Abstract

The occurrence of high-temperature superconductivity, and the competition with magnetism, in stoichiometric and doped LaFeAsO and isostructural iron oxypnictides is raising many fundamental questions about the electronic structure and magnetic interactions in this class of materials. There are now sufficient experimental data that it may be possible to identify the important issues whose resolution will lead to the understanding of this system. In this paper, we address a number of the important issues. One important characteristic is the Fe–As distance (or more abstractly the pnicogen (Pn) height z(Pn)); we present results for the effect of z(Pn) on the electronic structure, energetics and Fe magnetic moment. We also study LaFeAsO under pressure, and investigate the effects of both electron and hole doping within the virtual crystal approximation. The electric field gradients for all atoms in the LaFeAsO compound are presented (undoped and doped) and compared with available data. The observed (π, π, π) magnetic order is studied and compared with the computationally simpler (π, π, 0) order which is probably a very good model in most respects. We investigate the crucial role of the pnicogen atom in this class, and predict the structures and properties of the N and Sb counterparts that have not yet been reported experimentally. At a certain volume a gap opens at the Fermi level in LaFeNO, separating bonding from antibonding bands. This is the first evidence that this class of materials indeed has an underlying semimetallic character, and this separation suggests directions for a better simple understanding of the seemingly intricate electronic structure of this system. Finally, we address briefly differences resulting from substitution of post-lanthanum rare earth atoms, which have been observed to enhance the superconducting critical temperature substantially.

Highlights

  • The occurrence of high temperature superconductivity, and the competition with magnetism, in stoichiometric and doped LaOFeAs and isostructural iron-oxypnictides is raising many fundamental questions about the electronic structure and magnetic interactions in this class of materials

  • Stoichiometric LaOFeAs is AFM; ∼0.05 carriers/Fe doping of either sign destroys magnetic order and impressive superconductivity arises, with Tc seemingly depending little on the carrier concentration

  • It undergoes a structural phase transition at lower temperature[2,3], the doped material LaO1−xFxFeAs remains in this structure down to low temperature, so the study of LaOFeAs in the high symmetry structure is a necessary step towards the understanding of the electronic structure of the whole family of compounds

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Summary

CRYSTAL STRUCTURE

The Fe and O atoms lie in planes,. We will refer to this antiferromagnetic order as FIG. 2: (Color online) The QM magnetic structure of the Fe-As substructure of LaOFeAs, showing alternating chains of Fe spin up (red circles with black dots) and Fe spin down (blue circles with black crosses). The As atoms above (below) the Fe plane are represented as large (small) squares. The QM AFM order, or equivalently as (π, π, 0), while the Q0 AFM order corresponds to an antiferromagnetic order of the original cell (dashed lines in Fig. 2) with two Fe atoms. FM will refer to a ferromagnetic arrangement of the spins, while NM means non-magnetic

CALCULATION METHOD
STUDY OF LAOFEAS IN THE TETRAGONAL STRUCTURE
Influence of XC functionals and codes on the electronic structure of LaOFeAs
Effect of virtual crystal doping on the electronic structure of LaOFeAs
Electric field gradients
Effect of pressure on the electronic structure of LaOFeAs
ROLE OF THE PNICTOGEN ATOM
LaOFeP
LaOFeSb
LaOFeN
ROLE OF THE RARE EARTH ATOM IN REOFEAS
VIII. SUMMARY
Full Text
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