Weak antilocalization and interaction-induced localization of Dirac and Weyl Fermions in topological insulators and semimetals
Lu Hai-Zhou1, Shen Shun-Qing2
       

The magnetoconductivity δσqi(B) for different phase coherence length ϕ at ηI = η* = 0 (a), for different ηI at η* = 0 (b), and for different ηI at finite η* (c). The magnetic field B is applied along arbitrary directions. Parameters = 10 nm and ϕ = 1000 nm in panels (b) and (c). (d) The diagrams show the difference between ηI and η*, with ηI related to the intervalley scattering and η* measuring the intervalley correlation of intravalley scattering. The dashed lines represent the correlation of two scattering processes. ν = ± is the valley index. Adapted from Ref. [24].