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Local structural study of Fe<sub>1.1</sub>Te using pair distribution function techniques

ORAL

Abstract

The link between electronic nematicity, magnetic and orbital order and their influence on high-Tc superconductivity is a highly controversial aspect in the physics of iron-based superconductors (FeSCs). It is believed that nematicity and superconductivity has a deep connection since optimal superconductivity occurs near nematic instabilities in FeSCs. Fe1+yTe are promising candidates to understand the mechanism of superconductivity in the family of Fe-based superconductors. Here, we used the neutron pair distribution function (PDF) techniques to study the local structure of Fe1.1Te above and below the structural transition temperature. We observed the first order transition from paramagnetic to commensurate antiferromagnetic ordering at 75 K corresponding to a tetragonal P4/nmm to monoclinic P21/m transition around 70 K. By tracking the monoclinicity parameter we observe the local scale distortions of the tetragonal and monoclinic structure in a typical range of 1-2 nm. These spatially limited distortions represent fluctuating nematic order which suggests the ubiquity of nematic fluctuations in iron-based superconductors. Our results agree well with the recent local structure study on FeSe and (Sr, Na)Fe2As2 which reveal the presence of short range orthorhombic distortions.

Presenters

  • Bhupendra Karki

    Department of Physics and Astronomy, University of Louisville

Authors

  • Bhupendra Karki

    Department of Physics and Astronomy, University of Louisville

  • Alaa Alfailakawi

    Department of Physics and Astronomy, University of Louisville

  • Benjamin Frandsen

    Physics and Astronomy, Brigham Young University, Department of Physics, Brigham Young University, Brigham Young University, Department of Physics and Astronomy, Brigham Young University

  • Joerg Neuefeind

    Neutron Scattering Division, Oak Ridge National Laboratory

  • Michelle Everett

    Neutron Scattering Division, Oak Ridge National Laboratory

  • Byron Freelon

    Department of Physics and Texas Center for Superconductivity, University of Houston, Massachusetts Institute of Technology