Spin reorientation and 'quasi-nematic' order in the re-entrant tetragonal phase of Ba$_{0.76}$K$_{0.24}$Fe$_2$As$_2$

POSTER

Abstract

Clarifying the phase diagram and the nature of the competing or coexisting orders between magnetism, nematicity and superconductivity is of primary importance for the understanding of the mechanism of iron-based superconductors. Here, we investigate the re-entrant tetragonal phase in Ba$_{0.76}$K$_{0.24}$Fe$_{2}$As$_{2}$ in detail by DC magnetisation, resistivity, thermal expansion, thermal conductivity and thermo-electrical measurements. The thermal expansion indicates that the transition into the re-entrant phase is incomplete, but becomes more complete in high magnetic fields. The magnetization provides strong evidence that the spin alignment in the re-entrant C$_{4}$ phase is out-of-plane. The Nernst coefficient shows a large negative value in the stripe-type spin density wave (SDW) state owing to the Fermi surface reconstruction associated with nematic order. At the transition into the re-entrant C$_{4}$ tetragonal phase it hardly changes, suggesting that a similar ‘quasi-nematic’ electronic order could be present in this phase, in a novel form that preserves the tetragonal crystal symmetry. We propose a chequerboard type of charge or orbital ordering that replaces the nematic order of the stripe-type SDW phase below the C$_{4}$ re-entrant transition.

Authors

  • Chang-woo Cho

    • Department of Physics, The Hong Kong University of Science and Technology
  • Jianqiang Hou

    • Department of Physics, The Hong Kong University of Science and Technology
  • Junying SHEN

    • Department of Physics, The Hong Kong University of Science and Technology
  • Pok Man Tam

    • Department of Physics, The Hong Kong University of Science and Technology
  • I-Hsuan Kao

    • Department of Physics, The Hong Kong University of Science and Technology
  • Mang Hei Gordon Lee

    • Department of Physics, The Hong Kong University of Science and Technology
  • Thomas Wolf

    • Institute for Solid State Physics, Karlsruhe Institute of Technology
  • Christoph Meingast

    • Institute for Solid State Physics, Karlsruhe Institute of Technology
  • Rolf Lortz

    • Department of Physics, The Hong Kong University of Science and Technology