Fig. 5: Fermi arcs.
From: Tunable chirality of noncentrosymmetric magnetic Weyl semimetals in rare-earth carbides
a Bulk Fermi surface of NdRhC2. b Fermi surface of the RhC2-terminated (100)-surface without canting of the magnetization, fixing the Fermi energy at the Weyl node energy (εF = 43 meV). c Same for Fermi energy at the charge-neutrality chemical potential (εF = 0). d Same as c for a canting angle θ = 25°.
