“…The existence of PF was first considered by Wannier [9] in insulators, by Shockley and Bardeen [10] in crystalline semiconductors, by Fritzsche [11] in amorphous semiconductors, and by Shklovskii and Efros [12,13] who have shown that randomly distributed donors and acceptors create large scale PF of magnitude comparable with the forbidden bandwidth. Pistoulet et al [14][15][16] derived general expressions of the dc transport coefficients by band carriers in the presence of PF ; dc conductivity activation energy and preexponential factor, photoconductivity, thermopower are drastically changed by PF. The expression of the complex conductivity 0'a, (,w, T) + i W Eac ('W, T) from dc to very high frequencies, when the effect of PF on band carriers is considered, was derived by Pistoulet, Roche, Abdalla [17] (PRA) ; the validity of the model was numerically confirmed by Soegandi, Roche, Pistoulet [18].…”