where n, e, μ, h, k B , m*, κ l , and L represent the charge carrier density, charge of the electron, mobility of the charge carrier, Plank constant, Boltzmann constant, effective mass of charge carrier near the Fermi level, lattice thermal conductivity, and temperature dependent Lorenz number, respectively. Among them Equation (4) is only valid for metals and degenerate semiconductors described by a parabolic band and the energy-independent scattering approximation. Therefore, it is challenging to decouple the S 2 σ and κ.