Abstract

Despite the fact that 1111-type iron arsenides hold the record transition temperature of iron-based superconductors, their electronic structures have not been studied much because of the lack of high-quality single crystals. In this study, we completely determine the Fermi surface in the antiferromagnetic state of CaFeAsF, a 1111 iron-arsenide parent compound, by performing quantum oscillation measurements and band-structure calculations. The determined Fermi surface consists of a symmetry-related pair of Dirac electron cylinders and a normal hole cylinder. From analyses of quantum-oscillation phases, we demonstrate that the electron cylinders carry a nontrivial Berry phase $\pi$. The carrier density is of the order of 10$^{-3}$ per Fe. This unusual metallic state with the extremely small carrier density is a consequence of the previously discussed topological feature of the band structure which prevents the antiferromagnetic gap from being a full gap. We also report a nearly linear-in-$B$ magnetoresistance and an anomalous resistivity increase above about 30 T for $B \parallel c$, the latter of which is likely related to the quantum limit of the electron orbit. Intriguingly, the electrical resistivity exhibits a nonmetallic temperature dependence in the paramagnetic tetragonal phase ($T >$ 118 K), which may suggest an incoherent state. Our study provides a detailed knowledge of the Fermi surface in the antiferromagnetic state of 1111 parent compounds and moreover opens up a new possibility to explore Dirac-fermion physics in those compounds.

Highlights

  • Since the discovery of superconductivity at Tc 1⁄4 26 K in LaFeAsðO1−xFxÞ by Kamihara et al [1], iron-based superconductors have been studied extensively

  • The determined Fermi surface consists of a symmetry-related pair of Dirac electron cylinders and a normal hole cylinder

  • Our study provides a detailed knowledge of the Fermi surface in the antiferromagnetic state of 1111 parent compounds and opens up a new possibility to explore Dirac-fermion physics in those compounds

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Summary

Introduction

Since the discovery of superconductivity at Tc 1⁄4 26 K in LaFeAsðO1−xFxÞ by Kamihara et al [1], iron-based superconductors have been studied extensively. By replacing La with smaller rare-earth elements, Tc of up to 56 K was achieved in the same 1111-type structure immediately after the discovery [2,3,4,5]. It is crucial to unravel the normalstate electronic structure of the 1111 iron arsenides from which the highest Tc among the iron-based superconductors emerges. Such studies suffer from difficulty in obtaining high-quality single crystals of the 1111-type iron arsenides

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