In the quantum limit of a lattice Dirac semimetal, impurity scattering yields sigma_zz = |e|^3|B|v_F/(4pi^2 hbar eps) * (1-|M|^2)/(2|M|^2), carried by chiral modes with J = v_F rho_5, a microscopic derivation of the chiral magnetic effect picture.
McCann, Non-hermitian su-schrieffer-heeger model with the energy levels of free parafermions, Physical Re- view B113, 10.1103/hdzd-94qm (2026)
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Chiral Magnetic Conductivity in the Tight-Binding Model of Dirac Semimetals
In the quantum limit of a lattice Dirac semimetal, impurity scattering yields sigma_zz = |e|^3|B|v_F/(4pi^2 hbar eps) * (1-|M|^2)/(2|M|^2), carried by chiral modes with J = v_F rho_5, a microscopic derivation of the chiral magnetic effect picture.