“…At higher temperatures 0 are strongly temperature dependent, but at low temperature the ac conductivity becomes temperature independent; 0 ðTÞ plateaus are strongly frequency-dependent, which suggests that the hopping or tunneling of localized charge carriers governs the electrical transport in the whole temperature range. 6 Like in many other amorphous materials 7-10 similar temperature dependence of the ac electrical conductivity has been observed in many semiconductor systems, i.e., lithium phthalocyanine and its iodinated version 11 and in many semiconductor glassy systems: bismuth-vanadate, 12 iron bismuthate, 13 vanadium germinate, 14 silver vanadate 15 and other semiconductor glassy systems. Figure 2(a) shows the frequency dependence of the logarithm of the real part of the ac electric conductivity, log 0 , at various temperatures and the logarithm of the real part of the dielectric constant, log " 0 , versus frequency at the same temperatures (Fig.…”