2022
DOI: 10.1103/physrevb.105.085410
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Phonon-limited transport and Fermi arc lifetime in Weyl semimetals

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Cited by 9 publications
(3 citation statements)
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“…Since the Berry curvature acts on the semiclassical trajectories of the electrons similarly to a magnetic field [70], a discontinuity bears many resem-blances with a magnetic field jump in a graphene layer: in particular, the interface states can be seen as threedimensional analogues of the "snake states" [71]. Interestingly, the chirality of the interface arcs implies that they are to some extent robust to backscattering arising from the interaction with, e.g., phonons, while dissipation of the current in the bulk modes is generally possible and most prominent for states in the vicinity of the merging points with the bulk Fermi surface [63]. It will be interesting to extend the analysis of this paper to related models, including type-II, multi-Weyl and triplepoint Weyl semimetals [72][73][74][75].…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…Since the Berry curvature acts on the semiclassical trajectories of the electrons similarly to a magnetic field [70], a discontinuity bears many resem-blances with a magnetic field jump in a graphene layer: in particular, the interface states can be seen as threedimensional analogues of the "snake states" [71]. Interestingly, the chirality of the interface arcs implies that they are to some extent robust to backscattering arising from the interaction with, e.g., phonons, while dissipation of the current in the bulk modes is generally possible and most prominent for states in the vicinity of the merging points with the bulk Fermi surface [63]. It will be interesting to extend the analysis of this paper to related models, including type-II, multi-Weyl and triplepoint Weyl semimetals [72][73][74][75].…”
Section: Discussionmentioning
confidence: 99%
“…For θ = 0, we impose the boundary conditions [62] on the wave function Ψ, for every value of x. These boundary conditions do not break inversion symmetry [63] and imply that the charge current vanishes across the surfaces at y = 0 and y = L. The wave function reduces then to the eigenvectors ξ ± of the Pauli matrix σ x . For simplicity, we consider the large-L limit.…”
Section: A Bike Lanesmentioning
confidence: 99%
“…which ensures that the component of the current density normal to the boundary vanishes [51,52]. The matrix B depends on a phenomenological boundary angle α,…”
Section: B Boundary Modes For Semi-infinite Geometrymentioning
confidence: 99%