Effect of Sodium Iodide Dopant Concentration on the Electrical Behavior of AgPO3 Glassy Networks

Abstract

The ionic and dielectric behavior of (AgPO 3 ) (1 -x) -NaI x (x = 0, 0.02, 0.04, …, 0.14) systems were tested in the frequency range of 1-10 6 Hz at different temperatures using impedance spectroscopy technique. Samples were prepared using the melt quenching method to obtain the desired ratios between NaI and AgPO 3 . Results of impedance measurements showed a switching from resistive-like (at low frequency) to capacitive-like (at higher frequency) behavior with a single relaxation peak that shifts to higher frequency with increasing either the temperature or the dopant concentration. In addition, the Nyquist plots showed a decrease in the values of the bulk resistance of the samples with increasing temperature and dopant concentration. The measured AC-conductivity shows a cross-over at frequency f > 10 5 Hz. The conductivity shows an increase as function of temperature regardless the frequency range and it is almost constant at low frequency up to the crossover frequency, in addition to that, the power law dispersive behavior was also observed at higher frequency ( f > 10 5 Hz). The DC-conductivity can be explained in terms of silver ions successful diffusion process that take place due to the applied alternative electric field. On the other hand, the diffusion controlled relaxation (DCR) model can be used to explain the power law conductivity. Finally, the values of the activation energy calculated from the linear plot of Arrhenius equation were found to decrease with the dopant concentration from 0.65 eV at zero concentration to 0.36 eV at 14% concentration.

Electrical properties of epoxy/graphite flakes microcomposite at the percolation threshold concentration

“…According to Koop's theory, the lower σ′ value at the low-frequencies range can be attributed to the presence of low conductivity grains, while the higher σ′ higher frequencies are associated with high conductivity grains [34]. The displacement of charge carriers diminishes as the frequency increases, and beyond 10 5 Hz, σ′ conforms to the formula: σ ac ∼ ω s , where 0 s 1, indicating hopping conductivity [8,[51][52][53][54]. The numerical value S assumes the extremes of 0 and 1 for ideal ionic-type crystals and ideal Debye-type crystals, respectively.…”

“…A critical parameter to investigate is the activation energy, representing the energy required for an ion to surpass the energy barrier for a successful jump. The activation energy value is determined through the application of the Arrhenius equation [51,52].…”