“…The optical selections rules imposed by the matrix elements are such that only the dipolar transitions |n| = |n| ± 1 (here n = 0, ±1, ±2, ...) are permitted in χ χ,(α,β) with α , β = x, y while only the transitions −n → n are permitted in χ χ,(z,z) . (A tilt of a Weyl cone allows for a much richer interband spectrum 15,22 ). We limit our study to the ultra-quantum regime where the Fermi level lies in the chiral level.…”