Tuning the flat bands of the kagome metal CoSn with Fe, In, or Ni doping

B. C. Sales, W. R. Meier, A. F. May, J. Xing, J.-Q. Yan, S. Gao, Y. H. Liu, M. B. Stone, A. D. Christianson, Q. Zhang, and M. A. McGuire
Phys. Rev. Materials 5, 044202 – Published 15 April 2021

Abstract

CoSn is a Pauli paramagnet with relatively flat d bands centered about 100 meV below the Fermi energy, EF. Single crystals of CoSn lightly doped with Fe, In, or Ni are investigated using x-ray and neutron scattering, magnetic susceptibility and magnetization, AC susceptibility, specific heat, and resistivity measurements. Within the rigid-band approximation, hole doping with a few percent of Fe or In should move the flat bands closer to EF, whereas electron doping with Ni should move the flat bands further away from EF. We provide evidence that this indeed occurs. Fe and In doping drive CoSn toward magnetism, while Ni doping suppresses CoSn's already weak magnetic response. The resulting ground state is different for Fe versus In doping. For Fe-doped crystals, Co1xFexSn, with 0.02<x<0.27, the magnetic and specific-heat data are consistent with the formation of a spin glass, with a glass temperature, Tg, ranging from 1 K for x=0.02 to 10 K for x=0.27. Powder and single-crystal neutron diffraction found no evidence of long-range magnetic order below Tg for samples with x0.17. For In-doped crystals, CoSn1yIny, both the magnetic susceptibility and the Sommerfeld coefficient, γ, increase substantially relative to pure CoSn, but with no clear indication of a magnetic transition for 0.05<y<0.2. CoSn crystals doped with Ni (Co0.93Ni0.07Sn) have a significantly smaller magnetic susceptibility and γ than pure CoSn, consistent with flat bands further from EF.

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  • Received 16 February 2021
  • Accepted 1 April 2021

DOI:https://doi.org/10.1103/PhysRevMaterials.5.044202

©2021 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

B. C. Sales1, W. R. Meier1, A. F. May1, J. Xing1, J.-Q. Yan1, S. Gao1,2, Y. H. Liu2, M. B. Stone2, A. D. Christianson1, Q. Zhang2, and M. A. McGuire1

  • 1Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge Tennessee 37831, USA
  • 2Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge Tennessee 37831, USA

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Vol. 5, Iss. 4 — April 2021

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