An exact beyond-relaxation-time Boltzmann calculation for a Rarita-Schwinger-Weyl node predicts opposite curvature in the two conduction bands and a sign flip controlled by interband scattering.
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Distinguishing features of longitudinal magnetoconductivity for a Rarita-Schwinger-Weyl node
An exact beyond-relaxation-time Boltzmann calculation for a Rarita-Schwinger-Weyl node predicts opposite curvature in the two conduction bands and a sign flip controlled by interband scattering.