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Nonlocal annihilation of Weyl fermions in correlated systems

, , , , , and . Phys. Rev. Res., 2 (1): 012023 (Jan 22, 2020)cite arxiv:1904.11836Comment: 6 pages, 4 figures.
DOI: 10.1103/PhysRevResearch.2.012023

Abstract

Weyl semimetals (WSMs) are characterized by topologically stable pairs of nodal points in the band structure that typically originate from splitting a degenerate Dirac point by breaking symmetries such as time-reversal or inversion symmetry. Within the independent-electron approximation, the transition between an insulating state and a WSM requires the local creation or annihilation of one or several pairs of Weyl nodes in reciprocal space. Here, we show that strong electron-electron interactions may qualitatively change this scenario. In particular, we reveal that the transition to a Weyl semimetallic phase can become discontinuous, and, quite remarkably, pairs of Weyl nodes with a finite distance in momentum space suddenly appear or disappear in the spectral function. We associate this behavior with the buildup of strong many-body correlations in the topologically nontrivial regions, manifesting in dynamical fluctuations in the orbital channel. We also highlight the impact of electronic correlations on the Fermi arcs.

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Phys. Rev. Research 2, 012023(R) (2020) - Nonlocal annihilation of Weyl fermions in correlated systems

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