2019
DOI: 10.1039/c9nr04551a
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A type of robust superlattice type-I Weyl semimetal with four Weyl nodes

Abstract: We investigate the topological properties of the Janus superlattices WTeS and WTeSe by first-principles methods and Wannier-based tight-binding Hamiltonians.

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Cited by 14 publications
(5 citation statements)
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“…Weyl points with different chiral appear at different momentum positions, and their projections on the surface are connected by the Fermi arc. Because the emergence of WSM needs to break the time reversal symmetry or space inversion symmetry, and in IH and FH, inversion symmetry is naturally broken, so many Heusler compounds are Weyl semimetals, such as LnPtBi (Ln=Y, Gd, or Nd) [22] , WTeS and WTeSe [23], LaAlGe [24], and Co2TiX (X=Si, Ge, or Sn) [25] in FH. The time reversal symmetry of magnetic WSM is guaranteed by the system magnetism and can be controlled by the external field.…”
Section: 4magnetic Structurementioning
confidence: 99%
“…Weyl points with different chiral appear at different momentum positions, and their projections on the surface are connected by the Fermi arc. Because the emergence of WSM needs to break the time reversal symmetry or space inversion symmetry, and in IH and FH, inversion symmetry is naturally broken, so many Heusler compounds are Weyl semimetals, such as LnPtBi (Ln=Y, Gd, or Nd) [22] , WTeS and WTeSe [23], LaAlGe [24], and Co2TiX (X=Si, Ge, or Sn) [25] in FH. The time reversal symmetry of magnetic WSM is guaranteed by the system magnetism and can be controlled by the external field.…”
Section: 4magnetic Structurementioning
confidence: 99%
“…The Dirac and Weyl fermions exhibit massless nature and behave in a fundamentally different manner from that of conventional Schro ¨dinger fermions. [5][6][7][8] Furthermore, it is responsible for the realization of specific properties in TSMs such as Fermi arcs, drumhead surface states, chiral anomaly and extreme magnetoresistance. [9][10][11][12][13] As a result, TSMs have become a focus of scientific investigation in the fields of solid-state chemistry, condensed matter physics and materials science.…”
Section: Introductionmentioning
confidence: 99%
“…According to the Nielsen-Ninomiya theorem [29], each pair of nodes carries Berry curvature monopoles of opposite chirality which are connected via Fermi arcs lying at opposite sur-faces of the slab [30]. Type I WSMs, such as elemental Tellurium [31], Janus superlattices [32] and Ta or As compounds [33][34][35], are characterized by point-like Fermi surface in the bulk and vanishing density of states. Type II WSMs, such as MoTe 2 [36,37] and WTe 2 [38,39] but also the magnetic candidate Co 3 Sn 2 S 2 [40][41][42][43][44][45], offer a slightly different paradigm as the Weyl cone spectrum is tilted in momentum space, breaking Lorentz invariance.…”
Section: Introductionmentioning
confidence: 99%