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  • Letter

Spin-polarized gap in the magnetic Weyl semimetal Co3Sn2S2

Fei Sun1,2,3,†, Tan Zhang1,2,†, C. J. Yi1,2, Y. L. Wu1, H. Zhao1,2, Q. Wu1,2, Y. G. Shi1,2, Hongming Weng1,2,4,*, and Jimin Zhao1,2,4,*

  • 1Beijing National Research Center for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 2School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3Max Planck Institute for Chemical Physics of Solids, Dresden 01187, Germany
  • 4Songshan Lake Materials Laboratory, Dongguan, Guangdong 523808, China

  • *Corresponding authors: jmzhao@iphy.ac.cn, hmweng@iphy.ac.cn
  • †These authors contributed equally to this work.

Phys. Rev. B 104, L100301 – Published 7 September, 2021

DOI: https://doi.org/10.1103/PhysRevB.104.L100301

Abstract

We report a unique type of gap in a magnetic Weyl semimetal Co3Sn2S2 where the electrons are spin polarized and preserve the spin-momentum locking feature of Weyl fermions. Such spin-polarized gaps are associated with the Weyl node annihilation, where a pair of Weyl nodes with opposite chirality touch each other at ∼210 meV above the Fermi energy. These are revealed by both time- and spin-resolved ultrafast spectroscopy experiments, combined with first-principles calculations. The spin-polarized gap opening is accompanied by a topological phase transition, and the gap magnitude exhibits an unconventional temperature dependence originated from the Weyl physics. Furthermore, we propose possible circularly polarized terahertz-midinfrared radiation from such a spin-polarized gap. Our results shed light on exploring the topological properties of excited states and endow application potentials for gapped materials based on chirality.

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