Dirac cone, flat band and saddle point in kagome magnet YMn<sub>6</sub>Sn<sub>6</sub>.

Li, Man; Wang, Qi; Wang, Guangwei; Yuan, Zhihong; Song, Wenhua; Lou, Rui; Liu, Zhengtai; Huang, Yaobo et al. · Nat Commun · 2021

basic_science · Level V

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Abstract

Kagome-lattices of 3d-transition metals hosting Weyl/Dirac fermions and topological flat bands exhibit non-trivial topological characters and novel quantum phases, such as the anomalous Hall effect and fractional quantum Hall effect. With consideration of spin-orbit coupling and electron correlation, several instabilities could be induced. The typical characters of the electronic structure of a kagome lattice, i.e., the saddle point, Dirac-cone, and flat band, around the Fermi energy (E<sub>F</sub>) remain elusive in magnetic kagome materials. We present the experimental observation of the complete features in ferromagnetic kagome layers of YMn<sub>6</sub>Sn<sub>6</sub> helically coupled along the c-axis, by using angle-resolved photoemission spectroscopy and band structure calculations. We demonstrate a Dirac dispersion near E<sub>F</sub>, which is predicted by spin-polarized theoretical calculations, carries an intrinsic Berry curvature and contributes to the anomalous Hall effect in transport measurements. In addition, a flat band and a saddle point with a high density of states near E<sub>F</sub> are observed. These multi-sets of kagome features are of orbital-selective origin and could cause multi-orbital magnetism. The Dirac fermion, flat band and saddle point in the vicinity of E<sub>F</sub> open an opportunity in manipulating the topological properties in magnetic materials.