Abstract

The rare-earth monopnictide LaBi exhibits exotic magneto-transport properties, including an extremely large and anisotropic magnetoresistance. Experimental evidence for topological surface states is still missing although band inversions have been postulated to induce a topological phase in LaBi. In this work, we have revealed the existence of surface states of LaBi through the observation of three Dirac cones: two coexist at the corners and one appears at the centre of the Brillouin zone, by employing angle-resolved photoemission spectroscopy in conjunction with ab initio calculations. The odd number of surface Dirac cones is a direct consequence of the odd number of band inversions in the bulk band structure, thereby proving that LaBi is a topological, compensated semimetal, which is equivalent to a time-reversal invariant topological insulator. Our findings provide insight into the topological surface states of LaBi’s semi-metallicity and related magneto-transport properties.

Highlights

  • The rare-earth monopnictide LaBi exhibits exotic magneto-transport properties, including an extremely large and anisotropic magnetoresistance

  • A topological surface state (TSS) of a topological insulators (TIs) is commonly observed as a Dirac-cone type dispersion inside an insulating bulk energy gap[9,10,11], while a TSS of a Dirac or Weyl semimetal is characterized by Fermi arcs[12,13,14,15,16]

  • We have investigated its TSSs by angle-resolved photoelectron spectroscopy (ARPES) and ab initio calculations

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Summary

Introduction

The rare-earth monopnictide LaBi exhibits exotic magneto-transport properties, including an extremely large and anisotropic magnetoresistance. It is challenging to identify the topological nature of surface states for a family of gapless TIs that are characterized by the non-trivial Z2 type topological invariants, dubbed Z2-topological metals, due to the lack of a bulk energy gap. Dirac-like surface states have been found to overlap strongly with bulk states below the Fermi energy in the gapless Heusler TI compounds[17].

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