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Abstract Ferroelectric ceramics, un-doped Ba1-xSrxTiO3 (BST) where x has the values: 0.0, 0.1, 0.15, 0.25, 0.3 and 0.5 mol. %, rare earth–doped [(1-x) (B0.75 Sr0.25 TiO3)+ 0.2 mol. % Sm2O3 +x Dy2O3] (BSTR), where x = 0, 0.1, 0.3 and 0.5, respectively were all prepared by a solid state reaction technique. X-ray diffraction (XRD) patterns confirmed the formation of the perovskite phase for all prepared un-doped and doped samples. Also, size of crystallites and the parameter, a, c and c/a ratio were found to be decreased with increasing of Sr content in un- doped samples, but they are increased for Dy2O3 doped BSTR ceramics. Field emission scanning electron microscopy (FESEM) of doped samples confirmed (XRD) results revealed that, as x Dy2O3 content increases, particle size increases. Energy dispersive X-ray (EDX) analysis for doped samples indicates that the increase of Dy2O3 content in the sample resulting in formation of perovskite tetragonal phase of large grains BSTR and small ones BST residing on the boundaries of the former as confirmed by SEM micrographs. Mechanical properties such as ultrasonic attenuation, ultrasonic wave velocities, and elastic moduli were studied by employing an ultrasonic pulse echo method at 2 MHz frequency for both doped and un-doped samples. Obtained results revealed strong compositional dependence of all previous mechanical properties. Also, high temperature ultrasonic studies for both Dy2O3-doped and un-doped samples showed the Curie transition temperatures of tested ceramics in addition to some relaxations peaks which occur in these materials to be dependent on composition for both BST and BSTR ceramics. For un-doped, BST samples, increasing Sr content, resulted in decreasing bulk density while increasing Dy2O3 in doped samples increased the density. The ultrasonic attenuation decreased for all tested ceramics and ultrasonic velocities and elastic moduli are all increased upon increasing amounts of dopants, Sr in BST and Dy2O3 in BSTR ceramics. Finally, dielectric investigations are performed on un-doped and rare earth-doped samples at room temperature in the range of frequency from 0.1 Hz up to one MHz for un-doped samples and from 100 Hz up to one MHz for doped samples. Variations of all parameters, the complex impedance Z*, the real and imaginary components of dielectric constant ε` and ε``, dissipation factor, tan δ and the ac-conductivity with frequency (log f) revealed the nature of polarization, dielectric loss and types of conduction mechanisms in tested ceramics. The acquired structural, mechanical, and electrical results were discussed and correlated. |