14 research outputs found
Composition-dependent xBa(Zr0.2Ti0.8)O3-(1-x)(Ba0.7Ca0.3)TiO3 bulk ceramics for high energy storage applications
This work reports the composition dependent microstructure, dielectric, ferroelectric
and energy storage properties, and the phase transitions sequence of lead free
xBa(Zr0.2Ti0.8)O3-(1-x)(Ba0.7Ca0.3)TiO3 [xBZT-(1-x)BCT] ceramics, with x = 0.4, 0.5
and 0.6, prepared by solid state reaction method. The XRD and Raman scattering results
confirm the coexistence of rhombohedral and tetragonal phases at room temperature
(RT). The temperature dependence of Raman scattering spectra, dielectric permittivity
and polarization points a first phase transition from ferroelectric rhombohedral phase to
ferroelectric tetragonal phase at a temperature (TR-T) of 40 0C and a second phase
transition from ferroelectric tetragonal phase - paraelectric pseudocubic phase at a
temperature (TT-C) of 110 0C. The dielectric analysis suggests that the phase transition at
TT-C is of diffusive type and the BZT-BCT ceramics are a relaxor type ferroelectric
materials. The composition induced variation in the temperature dependence of
dielectric losses was correlated with full width half maxima (FWHM) of A1, E(LO)
Raman mode. The saturation polarization (Ps) ≈ 8.3 μC/cm2 and coercive fields ≈ 2.9
kV/cm were found to be optimum at composition x = 0.6 and is attributed to grain size
effect. It is also shown that BZT-BCT ceramics exhibit a fatigue free response up to 105
cycles. The effect of a.c. electric field amplitude and temperature on energy storage
density and storage efficiency is also discussed. The presence of high TT-C (110 0C), a
high dielectric constant (εr ≈ 12285) with low dielectric loss (0.03), good polarization
(Ps) ≈ 8.3 μC/cm2) and large recoverable energy density (W = 121 mJ/cm3) with an
energy storage efficiency (η) of 70 % at an electric field of 25 kV/cm in 0.6BZT
0.4BCT ceramics make them suitable candidates for energy storage capacitor
applications.This work was supported by (i) DST-SERB, Govt. of India through grant ECR/2017/000068 and (ii) UGC through Grant Nos. F.4-5(59-FRP/ 2014(BSR)). The authors AR Jayakrishnan acknowledges Central University of Tamil Nadu, India for his Ph.D fellowship. K.V.A. acknowledges the DST for the Inspire fellowship IF170601. J.P.B.S. is grateful for the financial support through the FCT Grant SFRH/BPD/92896/2013.The authors thank to Vivek Sudarsanan from the Central University of Kerala for XRD measurements.info:eu-repo/semantics/publishedVersio