Abstract

Topological nodal-line semimetals are characterized by line-contact bulk band crossings and topological surface states. Breaking certain protecting symmetry turns this system into a Dirac semimetal or Weyl semimetal that hosts zero-dimensional isolated nodal points. Recent advances in band theory predicted a topological nodal-line semimetal state possessing a new type of nodal line in AlB2-type diborides. Here, we report an experimental realization of nodal-line fermions and associated surface states near the Fermi energy in ZrB2 by angle-resolved photoemission spectroscopy combined with first-principles calculations. The Dirac nodal lines in ZrB2 wind into two groups of nodal rings, which are linked together along the Γ-K direction. We further observe a distinct surface state connecting to each nodal line, indicative of the nontrivial topological nature of the bulk nodal lines. Therefore, our results provide convincing experimental evidence of nodal-line semimetal states in ZrB2 both in the bulk and on the surface, suggesting ZrB2 as a remarkable platform for discovering unique phenomena induced by nodal-line fermions.

Highlights

  • The realization of novel quantum states of matter with nontrivial topology beyond topological insulators has become a significant objective in current condensed-matter physics research.[1,2,3] Very recently, the discovery of topological semimetals has achieved this goal, which ignites extensive work focusing on the exotic topological properties and their underlying connection with the electronic structure.[4]

  • We investigate the electronic structure of ZrB2, which is predicted to host similar nodal-line configurations and surface states to that of TiB2.26,27 By using angle-resolved photoemission spectroscopy (ARPES) and firstprinciples calculations, we clearly observe two groups of nodal rings embedded in different mirror planes

  • In order to clarify the nontrivial topology of the bulk nodal lines realized in ZrB2, which are protected by the mirror-reflection symmetries and the combination of spatial-inversion symmetry (P) and time-reversal symmetry (T), i.e., the P·T symmetry, here we illustrate the connection between the nodal lines and the surface states by combining both the bulk and surface observations

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Summary

Introduction

The realization of novel quantum states of matter with nontrivial topology beyond topological insulators has become a significant objective in current condensed-matter physics research.[1,2,3] Very recently, the discovery of topological semimetals has achieved this goal, which ignites extensive work focusing on the exotic topological properties and their underlying connection with the electronic structure.[4]. In Dirac and Weyl semimetals, the bulk nodes are discrete in the BZ and their surface projections are connected by surface Fermi arcs.[4] While in nodal-line semimetals, the bulk nodes extend along one-dimensional curves and the corresponding surface states are flat in dispersion according to the previous nodal-line modelings,[7] where the band crossings of a nodal line should occur at zero energy with a constraint chiral symmetry. The flat surface bands are dubbed the drumhead states. The chiral symmetry is not exact in a real crystal, resulting in the nodal line does not generally occur at a constant energy, the associated topological surface states are not flat either.[8,9]

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