Stability of Weyl semimetals with quasiperiodic disorder
arXiv:2003.01499 · doi:10.1103/PhysRevB.102.045101
Abstract
Weyl semimetals are phases of matter with excitations effectively described by massless Dirac fermions. Their critical nature makes unclear the persistence of such phase in presence of disorder. We present a theorem ensuring the stability of the semimetallic phase in presence of weak quasiperiodic disorder. The proof relies on the subtle interplay of the relativistic Quantum Field Theory description combined with number theoretical properties used in KAM theory.
7 pages, 3 figures
References in corpus (6)
- Localization of interacting fermions at high temperature
- Rare region effects dominate weakly disordered 3D Dirac points
- Transport properties across the many-body localization transition in quasiperiodic and random systems
- Effective field theory of the disordered Weyl semimetal
- Interacting Weyl semimetals: characterization via the topological Hamiltonian and its breakdown
- Weyl semimetallic phase in an interacting lattice system
Cited by in corpus (9)
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- Critical Filaments and Superconductivity in Quasiperiodic Twisted Bilayer Graphene
- Connecting the avoided quantum critical point to the magic-angle transition in three-dimensional Weyl semimetals
- Universality in the 2d quasi-periodic Ising model and Harris-Luck irrelevance
- Vanishing of Drude weight in interacting fermions on Zd with quasi-periodic disorder
- Incommensurate Twisted Bilayer Graphene: emerging quasi-periodicity and stability