“…Table 3 summarizes the finding conduction parameters where the quantity µ a V was computed, confirming that V reduced from ~10 15 to ~10 6 cm −3 , which aligns with the growing number of disorderly stacked carbon sheets in the graphite samples. For all of the graphite samples, µ a = 250 cm 2 /Vs was used [11]. Besides, phenomenological description related to the internal states at the α-Fe 2 O 3 /graphite interface, as a function the conduction polarity at each half-cycle of the sine wave, is given below: In order to know how the α-Fe 2 O 3 /graphite interface acts as conducting channel at the positive electric field applied, a nonlinear diffusion of the charge carriers is caused through the interface and limited by attractive and repulsive electrostatic forces, where oxygen vacancies are acting as positive-charge trapping sites and the negative space-charge region, being the electrostatic length, l e , results inside the graphite layer, as shown in Figure 4a.…”