Topological Weyl Altermagnetism in CrSb

ORAL  · Invited

Abstract

Altermagnets constitute a novel, third fundamental class of collinear magnetic ordered materials, alongside with ferro- and antiferromagnets. They share with conventional antiferromagnets the feature of a vanishing net magnetization. At the same time they show a spin-splitting of electronic bands, just as in ferromagnets, caused by the atomic exchange interaction. On the other hand, topology has recently revolutionized our understanding of condensed matter physics, introducing new phases of matter classified by intrinsic topological order. Here we connect the worlds of altermagnetism and topology, showing that the electronic structure of the altermagnet CrSb is topological and hosts a novel Weyl semimetallic state. Using high-resolution and spin angle-resolved photoemission spectroscopy, we observe a large momentum-dependent spin-splitting in CrSb, reaching up to 1 eV, that induces altermagnetic Weyl nodes with an associated magnetic quantum number. At the surface we observe their spin-polarized topological Fermi-arcs. This establishes that in altermagnets the large energy scale intrinsic to the spin-splitting – orders of magnitude larger than the relativistic spin-orbit coupling – creates its own realm of robust electronic topology.

Publication: Cong Li, Mengli Hu, Zhilin Li, Yang Wang, Wanyu Chen, Balasubramanian Thiagarajan, Mats Leandersson, Craig Polley, Timur Kim, Hui Liu, Cosma Fulga, Maia G. Vergniory, Oleg Janson, Oscar Tjernberg & Jeroen van den Brink, arXiv:2405.14777

Presenters

  • Jeroen Van den Brink

    • IFW Dresden

Authors

  • Jeroen Van den Brink

    • IFW Dresden
  • Cong Li

    • KTH Royal Institute of Technology
  • Mengli HU

    • IFW Dresden
  • Zhilin Li

    • Institute of physics,chinese academy of sciences
    • Chinese Academy of Sciences
    • Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • Yang Wang

    • Department of Applied Physics, KTH Royal Institute of Technology, Stockholm 11419, Sweden
  • Wanyu Chen

    • Department of Applied Physics, KTH Royal Institute of Technology, Stockholm 11419, Sweden
  • Balasubramanian Thiagarajan

    • MAX IV Laboratory, Lund University, 22100 Lund, Sweden
    • MAX IV Laboratory
  • Craig Polley

    • MaxIV laboratory
    • MAX IV Laboratory, Lund University, 22100 Lund, Sweden
    • MAX IV Laboratory
  • Mats Leandersson

    • MAX IV Laboratory, Lund University, 22100 Lund, Sweden
  • Timur Kim

    • Diamond Light Source
    • Diamond Light Source, Harwell Campus, Didcot, OX11 0DE, United Kingdom
  • Hui Liu

    • Department of Physics, Stockholm University, AlbaNova University Center, 10691 Stockholm, Sweden
    • Stockholm University
  • Cosma Fulga

    • Leibniz Institute for Solid State and Materials Research, IFW Dresden, Helmholtzstraße 20, 01069 Dresden, Germany
  • Maia Vergniory

    • Max Planck Institute for Chemical Physics of Solids
    • Max Planck Institute for Chemical Physics of Solids, Dresden, Germany
    • Max Planck Institute for Chemical Physics of Solids, 01187 Dresden, Germany
  • Oleg Janson

    • Leibniz Institute for Solid State and Materials Research, IFW Dresden, Helmholtzstraße 20, 01069 Dresden, Germany
  • Oscar Tjernberg

    • KTH Royal Institute of Technology
    • Department of Applied Physics, KTH Royal Institute of Technology, Stockholm 11419, Sweden