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Low-Temperature Competing Magnetic Energy Scales in the Topological Ferrimagnet TbMn6Sn6

S. X. M. Riberolles1,*, Tyler J. Slade1,2, D. L. Abernathy3, G. E. Granroth3, Bing Li1,2, Y. Lee1, P. C. Canfield1,2, B. G. Ueland1, Liqin Ke1 et al.

R. J. McQueeney1,2,†

  • 1Ames Laboratory, Ames, Iowa 50011, USA
  • 2Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA
  • 3Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA

  • *simon.riberolles@gmail.com
  • †mcqueeney@ameslab.gov

Phys. Rev. X 12, 021043 – Published 23 May, 2022

DOI: https://doi.org/10.1103/PhysRevX.12.021043

Abstract

TbMn6Sn6 is a metallic ferrimagnet displaying signatures of both topological electrons and topological magnons arising from ferromagnetism and spin-orbit coupling within its Mn kagome layers. Inelastic neutron scattering measurements find strong ferromagnetic (FM) interactions within the Mn kagome layer and reveal a magnetic bandwidth of ∼230  meV. The low-energy magnetic excitations are characterized by strong FM Mn-Mn and antiferromagnetic (AFM) Mn-Tb interlayer magnetic couplings. We observe weaker, competing long-range FM and AFM Mn-Mn interlayer interactions similar to those driving helical magnetism in the YMn6Sn6 system. Combined with density-functional theory calculations, we find that competing Mn-Mn interlayer magnetic interactions occur in all RMn6Sn6 compounds with R=Y, Gd-Lu, resulting in magnetic instabilities and tunability when Mn-R interactions are weak. In the case of TbMn6Sn6, strong AFM Mn-Tb coupling ensures a highly stable three-dimensional ferrimagnetic network.

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