Effects of $\gamma$ irradiation on the electric conduction of PZT ceramic system

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Authors

  • R. Zachariasz University of Silesia, Faculty of Computer and Materials Science, Żeromskiego 3, 41-200 Sosnowiec, Poland
  • J. Rymarczyk University of Silesia, Faculty of Computer and Materials Science, Żeromskiego 3, 41-200 Sosnowiec, Poland
  • J. Ilczuk University of Silesia, Faculty of Computer and Materials Science, Żeromskiego 3, 41-200 Sosnowiec, Poland

Abstract

In the work, the results of investigations of the electric conduction $\sigma$ of the PZT ceramics with the two following compositions: Pb$_{0.94}$Sr$_{0.06}$(Zr$_{0.5}$Ti$_{0.5}$)O$_{3}$ + 0.25% wt. Cr$_{2}$O$_{3}$ (hard material) and (Pb$_{0.9}$Ba$_{0.1}$)(Zr$_{0.53}$Ti$_{0.47}$)O$_3$ + 1.67% wt. Nb$_2$O$_5$ (soft material), are presented. The “soft” ceramics are characterized by high electric values ($\epsilon^T_{33}/\epsilon_0 > 1300$ (in room temperature), $d_{31} = 120 \cdot 10^{−12}$ C/N) and electromechanical coupling coefficient ($k_p > 0.5$). Due to good parameters it is used in electromechanical transducers of low frequency. The “hard” PZT ceramics, which are used in resonators, filters and ultrasound transducers are characterized by the following parameters: $\epsilon^T_{33}/\epsilon_0 > 900$ (in room temperature), $d_{31} = 65\cdot 10^{−12}$ C/N and electromechanical coupling coefficient $k_p > 0.35$. The temperature dependences of the electric conduction $\sigma$ for all samples before and after $\gamma$ irradiation with dose of 20 kGy were performed. The activation energy $E_a$ was calculated on the basis of the ln $\sigma = f(1/T)$ dependences.

Keywords:

electric conduction, PZT materials, $\gamma$ radiation, activation energy.