\begin{document}$ m = 0 $\end{document} limit of different components of Wigner functions for massive fermions. Comparing with the chiral kinetic theory, we separated the vanishing and non-vanishing parts of vector and axial-vector components, up to the first order of \begin{document}$ \hbar $\end{document}. Then, we discussed the possible physical meaning of the vanishing and non-vanishing parts and their different behaviors at thermal equilibrium."> Massless limit of transport theory for massive Fermions -
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