“…As early raised by Chasmar and Stratton 6 , the transport coefficients which characterize the thermoelectric efficiency can be written as a function of Fermi integrals in the frame of the semi-classical treatment of the Boltzmann equation within the relaxation time approximation 7 . This description can be extended by including different scattering mechanisms 8 – 12 , bipolar effects 9 , multiple bands and valley degeneracy 13 – 17 . If one considers for instance that the relaxation time, the velocity and the density of states vary as a function of the energy according power laws 18 with the exponents , and respectively, then the electrical conductivity , the thermopower and the Lorentz number , with the electronic thermal conductivity , can be defined as it follows 6 , 8 – 10 .…”