In-plane anisotropy of transport coefficients in the electronic nematic states: Universal origin of the nematicity in Fe-based superconductors
arXiv:1612.08841 · doi:10.1103/PhysRevB.96.094527
Abstract
The origin of the electronic nematicity and its remarkable material-dependence are famous longstanding unsolved issues in Fe-based superconductors. To attack these issues, we focus on the in-plane anisotropy of the resistivity: In the nematic state in FeSe, the relation holds, where is the resistivity along the longer (shorter) Fe-Fe axis. In contrast, the opposite anisotropy is realized in other undoped Fe-based superconductors. Such nontrivial material dependence is naturally explained in terms of the strongly orbital-dependent inelastic quasiparticle scattering realized in the orbital-ordered state. The opposite anisotropy between FeSe () and other undoped compounds () reflects the difference in the number of hole-pockets. We also explain the large in-plane anisotropy of the thermoelectric power in the nematic state.
10 pages, 10 figures
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Cited by in corpus (10)
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- A Rigorous Formalism of Unconventional Symmetry Breaking in Fermi Liquid Theory and Its Application to Nematicity in FeSe
- Spontaneous orbital polarization in the nematic phase of FeSe
- Elastoresistance measurements on CaKFeAs and KCaFeAsF with the Fe site of symmetry
- Superconducting Order Parameter and Bosonic Mode in Hydrogen-Substituted NdFeAsOH Revealed by Multiple Andreev Reflection Spectroscopy
- Anisotropy of the DC conductivity due to orbital-selective spin fluctuations in the nematic phase of iron superconductors
- Superconducting Order Parameters in overdoped BaFeNiAs Revealed by Multiple Andreev Reflection Spectroscopy of Planar Break-Junctions
- Drude weight anisotropy in the doped iron pnictides: the primary role of orbital weight redistribution along the reconstructed Fermi surfaces
- Resistivity anisotropy from the multiorbital Boltzmann equation in nematic FeSe