Strain-induced axial gauge fields B5 produce angle-independent linear-in-B5 contributions to planar Hall conductivity in gapped nodal rings due to alignment with Berry curvature and orbital magnetic moment, with one component remaining completely strain-immune.
Unlike set-up II, there is noB 2 z contribution fromN 2,2
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Interplay of strain-induced axial gauge fields and intrinsic band-topology in the magnetoelectric conductivity of gapped nodal rings
Strain-induced axial gauge fields B5 produce angle-independent linear-in-B5 contributions to planar Hall conductivity in gapped nodal rings due to alignment with Berry curvature and orbital magnetic moment, with one component remaining completely strain-immune.