Electronic transport of Lorentz plasma with collision and magnetic field effects

Lv Chong¹, Wan Feng¹, Jia Mo-Ran¹, Li Zi-Liang¹, Sang Hai-Bo¹, Xie Bai-Song^{1, 2, †,}

Transverse electric conductivity σ_⊥ (a) and thermal conductivity κ_⊥ (b) against Ω for the case of Maxwellian distribution. The black dashed line (case 1) and red solid line (case 2) represent the condition of weak collision (ω_Be ≫ ν_T, see Refs. [28] and [29]) and the full condition without any limitation to the magnetic field and collision.