Lead vanadate glasses of the system $$(\hbox {V}_{2}\hbox {O}_{5})_{1-x}(\hbox {PbO})_{x}$$(V2O5)1-x(PbO)x with $$x = 0.4$$x=0.4, 0.45, 0.5, 0.55, 0.6 have been prepared by the press-quenching technique. The dc ($$\sigma (0)$$σ(0)) and… Click to show full abstract
Lead vanadate glasses of the system $$(\hbox {V}_{2}\hbox {O}_{5})_{1-x}(\hbox {PbO})_{x}$$(V2O5)1-x(PbO)x with $$x = 0.4$$x=0.4, 0.45, 0.5, 0.55, 0.6 have been prepared by the press-quenching technique. The dc ($$\sigma (0)$$σ(0)) and ac $$(\sigma (\omega ))$$(σ(ω)) electrical conductivities were measured in the temperature range from 150 to 420 K and the frequency range from $$10^{2}$$102 to $$10^{6}$$106 Hz. The electrical properties are shown to be sensitive to composition. The experimental results have been analyzed within the framework of different models. The dc conductivity is found to be proportional to $$T^{p}$$Tp with the exponent p ranging from 8.2 to 9.8, suggesting that the transport is determined by a multi-phonon process of weak electron-lattice coupling. The ac conductivity is explained by the percolation path approximation (PPA). In this model, $$\sigma $$σ$$(\omega )$$(ω) is closely related to the $$\sigma (0)$$σ(0) and fitting the experimental data produces a dielectric relaxation time $$\tau $$τ in good agreement with the expected value in both magnitude and temperature dependence.
               
Click one of the above tabs to view related content.