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Origin of the Resistivity Anisotropy in the Nematic Phase of FeSe

2015/11/15 by M. A. Tanatar, A. E. Böhmer, Erik Timmons +15 · 130 citations
Materials Science · Physics and Astronomy · #Anisotropy #Condensed matter physics #Electrical resistivity and conductivity #Iron-based superconductors research #Liquid crystal #Materials science #Optics #Phase (matter) #Physics #Quantum mechanics #Rare-earth and actinide compounds #Superconductivity #cond-mat.supr-con

paper · pdf · doi:10.1103/physrevlett.117.127001

published in Physical Review Letters 117(12), 127001 (American Physical Society)

arxiv created 2015/11/15 · openalex publication_date 2016/09/16 · arxiv updated 2016/09/21 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05

Abstract

The in-plane resistivity anisotropy is studied in strain-detwinned single crystals of FeSe. In contrast to other iron-based superconductors, FeSe does not develop long-range magnetic order below the tetragonal-to-orthorhombic transition at Ts≈90 K. This allows for the disentanglement of the contributions to the resistivity anisotropy due to nematic and magnetic orders. Comparing direct transport and elastoresistivity measurements, we extract the intrinsic resistivity anisotropy of strain-free samples. The anisotropy peaks slightly below Ts and decreases to nearly zero on cooling down to the superconducting transition. This behavior is consistent with a scenario in which the in-plane resistivity anisotropy is dominated by inelastic scattering by anisotropic spin fluctuations.

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