Abstract

Motivated by Weyl semimetals and weakly doped semiconductors, we study transport in a weakly disordered semiconductor with a power-law quasiparticle dispersion ξk∝kαξ_{\bf k}\propto k^α. We show, that in 2α2α dimensions short-correlated disorder experiences logarithmic renormalisation from all energies in the band. We study the case of a general dimension dd using a renormalisation group, controlled by an ε=2α−d\varepsilon=2α-d-expansion. Above the critical dimensions, conduction exhibits a localisation-delocalisation phase transition or a sharp crossover (depending on the symmetries of the Hamiltonian) as a function of disorder strength. We utilise this analysis to compute the low-temperature conductivity in Weyl semimetals and weakly doped semiconductors near and below the critical disorder point.

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