Quantum transport in 3D Weyl semimetals: Is there a metal-insulator transition?
arXiv:1501.00268 · doi:10.1140/epjb/e2016-70454-2
Abstract
We calculate the transport properties of three-dimensional Weyl fermions in a disordered environment. The resulting conductivity depends only on the Fermi energy and the scattering rate. First we study the conductivity at the spectral node for a fixed scattering rate and obtain a continuous transition from an insulator at weak disorder to a metal at stronger disorder. In the self-consistent Born approximation the scattering rate depends on the Fermi energy. Then it is crucial that the limits of the conductivity for a vanishing Fermi energy and a vanishing scattering rate do not commute. As a result, there is also metallic behavior in the phase with vanishing scattering rate and only a quantum critical point remains as an insulating state.
9 pages, 5 figures
References in corpus (12)
- The electronic properties of graphene
- Quantum Spin Hall Insulator State in HgTe Quantum Wells
- Rare region effects dominate weakly disordered 3D Dirac points
- Topological electronic structure and Weyl semimetal in the TlBiSe class of semiconductors
- Diffusive Quantum Criticality in Three Dimensional Disordered Dirac Semimetals
- Random gap model for graphene and graphene bilayers
- Stability of Weyl metals under impurity scattering
- Diffusion in the random gap model of mono- and bilayer graphene
- Conductivity of graphene: How to distinguish between samples with short and long range scatterers
- Long-range correlations in disordered graphene
- Renormalized transport properties of randomly gapped 2D Dirac fermions
- Two-parameter scaling theory of transport near a spectral node
Cited by in corpus (6)
- Single particle excitations in disordered Weyl fluids
- Robust quantum transport at particle-hole symmetry
- Short note on the density of states in 3D Weyl semimetals
- Nonlocal electrodynamics in Weyl semi-metals
- Corrections to the self-consistent Born approximation for Weyl fermions
- Ballistic transport in disordered Dirac and Weyl semimetals