Y.D. Kolekar
Savitribai Phule Pune University
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Archive | 2018
Bhavna C. Keswani; S. I. Patil; Y.D. Kolekar
Lead free ferroelectric with composition 0.55Ba0.92Ca0.08TiO3-0.45BaTi0.96Zr0.04O3 (BCT8-BZT4) was synthesized by solid state reaction method and investigated their structural, ferroelectric, piezoelectric and dielectric properties. X-ray diffraction analysis shows that BCT8-BZT4 ceramic possess both tetragonal (space group P4mm) and orthorhombic (space group Amm2) crystal structure which was further confirmed from Raman spectra spectroscopy. The micronized grains were observed from scanning electron micrographs while the presence of polarization-electric field hysteresis loop confirms ferroelectric nature of BCT8-BZT4 ceramic. Higher values of maximum polarization (Pmax = 22.27 μC/cm2), remnant polarization (Pr = 11.61 μC/cm2), coercive electric field (Ec = 4.77 kV/cm) and direct piezoelectric coefficient (d33) approximately 185 pC/N were observed. The real part of dielectric constant with frequency shows the usual dielectric dispersion behaviour at RT. The observed properties show that the lead free BCT8-BZT4 ceramic is suitable for ferroelectric memory device, piezoelectric sensor, capacitor, etc. applications.Lead free ferroelectric with composition 0.55Ba0.92Ca0.08TiO3-0.45BaTi0.96Zr0.04O3 (BCT8-BZT4) was synthesized by solid state reaction method and investigated their structural, ferroelectric, piezoelectric and dielectric properties. X-ray diffraction analysis shows that BCT8-BZT4 ceramic possess both tetragonal (space group P4mm) and orthorhombic (space group Amm2) crystal structure which was further confirmed from Raman spectra spectroscopy. The micronized grains were observed from scanning electron micrographs while the presence of polarization-electric field hysteresis loop confirms ferroelectric nature of BCT8-BZT4 ceramic. Higher values of maximum polarization (Pmax = 22.27 μC/cm2), remnant polarization (Pr = 11.61 μC/cm2), coercive electric field (Ec = 4.77 kV/cm) and direct piezoelectric coefficient (d33) approximately 185 pC/N were observed. The real part of dielectric constant with frequency shows the usual dielectric dispersion behaviour at RT. The observed properties show that the lead free BCT...
Journal of Applied Physics | 2018
Bhavna C. Keswani; Deepashri Saraf; S. I. Patil; Anjali Kshirsagar; A.R. James; Y.D. Kolekar; C. V. Ramana
We report on the combined experimental and theoretical simulation results of lead-free ferroelectrics, Ba(1-x)CaxTiO3 (x = 0.0–0.3) and BaTi(1-y)ZryO3 (y = 0.0–0.2), synthesized by standard solid state reaction method. First principles density functional calculations are used to investigate the electronic structure, dynamical charges, and spontaneous polarization of these compounds. In addition, the structural, ferroelectric, piezoelectric, and dielectric properties are studied using extensive experiments. The X-ray diffraction and temperature dependent Raman spectroscopy studies indicate that the calcium (Ca) substituted compositions exhibit a single phase crystal structure, while zirconium (Zr) substituted compositions are biphasic. The scanning electron micrographs reveal the uniform and highly dense microstructure. The presence of polarization-electric field and strain-electric field hysteresis loops confirms the ferroelectric and piezoelectric nature of all the compositions. Our results demonstrate higher values for polarization, percentage strain, piezoelectric coefficients, and electrostrictive coefficient compared to those existing in the literature. For smaller substitutions of Ca and Zr in BaTiO3, a direct piezoelectric coefficient (d33) is enhanced, while the highest d33 value (∼300 pC/N) is observed for BaTi0.96Zr0.04O3 due to the biphasic ferroelectric behavior. Calculation of Born effective charges indicates that doping with Ca or Zr increases the dynamical charges on Ti as well as on O and decreases the dynamical charge on Ba. An increase in the dynamical charges on Ti and O is ascribed to the increase in covalency of Ti-O bond that reduces the polarizability of the crystal. A broader range of temperatures is demonstrated to realize the stable phase in the Ca substituted compounds. The results indicate enhancement in the temperature range of applicability of these compounds for device applications. The combined theoretical and experimental study is expected to enhance the current scientific understanding of the lead-free ferroelectric materials.We report on the combined experimental and theoretical simulation results of lead-free ferroelectrics, Ba(1-x)CaxTiO3 (x = 0.0–0.3) and BaTi(1-y)ZryO3 (y = 0.0–0.2), synthesized by standard solid state reaction method. First principles density functional calculations are used to investigate the electronic structure, dynamical charges, and spontaneous polarization of these compounds. In addition, the structural, ferroelectric, piezoelectric, and dielectric properties are studied using extensive experiments. The X-ray diffraction and temperature dependent Raman spectroscopy studies indicate that the calcium (Ca) substituted compositions exhibit a single phase crystal structure, while zirconium (Zr) substituted compositions are biphasic. The scanning electron micrographs reveal the uniform and highly dense microstructure. The presence of polarization-electric field and strain-electric field hysteresis loops confirms the ferroelectric and piezoelectric nature of all the compositions. Our results demonstrate h...
Journal of Applied Physics | 2017
Shahaji P. Kharat; Roy Swadipta; R.C. Kambale; Y.D. Kolekar; C. V. Ramana
We report on the enhanced magnetostrictive properties of nanocrystalline Dysprosium (Dy3+) substituted iron-rich cobalt ferrites (Co0.8Fe(2.2-x)DyxO4, referred to as CFDO). The CFDO samples with a variable Dy concentration (x = 0.000–0.075) were synthesized by the sol-gel auto-combustion method. The phase purity and crystal structure were confirmed from X-ray diffraction analyses coupled with Rietveld refinement. Surface morphology analysis using scanning electron microscopy imaging indicates the agglomerated magnetic particles with a non-uniform particle size distribution, which is desirable to transfer the strain. The magnetostriction coefficient (λ11) measurements indicate that the CFDO with Dy concentration x = 0.025 exhibits the highest strain sensitivity, (dλ/dH) ∼1.432 nm/A (for H ≤ 1000 Oe). On the other hand, the magnetostriction coefficient (λ12) measurements indicate that the Dy concentration x = 0.075 exhibits the larger (dλ/dH) ∼ 0.615 nm/A (for H ≤ 1000 Oe). The maximum λ11value of 166 ppm (...
Integrated Ferroelectrics | 2017
Sumayya M. Ansari; B. C. Keswani; Y.D. Kolekar; Debasis Sen
ABSTRACT A novel chemical route was used to produce nanosized BaTiO3 at 150°C without mineralizer. The well-defined peaks observed in Raman spectroscopy prove the presence of high quality tetragonal crystal-lattice-symmetry and are used to better understand mechanism of polarization-switching dynamics with molecular-vibrational modes present in the crystal-lattice. Rietveld refinement shows best fit for X-ray diffraction data with tetragonal symmetry. Nanosized BaTiO3 exhibits typical P-E hysteresis-loop and demonstrates ferroelectric nature. Dielectric measurements show Curie temperature at 130°C. These study guarantees that the novel chemical route can be used to synthesize other lead-free-ferroelectric-functional materials suitable for thinner dielectrics in higher-capacitance multilayer-capacitors.
Journal of Physical Chemistry C | 2016
Sandip G. Kakade; Yuan-Ron Ma; Rupesh S. Devan; Y.D. Kolekar; C. V. Ramana
Journal of Physics and Chemistry of Solids | 2016
S. G. Kakade; R.C. Kambale; Y.D. Kolekar; C. V. Ramana
Applied Surface Science | 2017
Sumayya M. Ansari; R.D. Bhor; Kalpana Pai; Debasis Sen; S. Mazumder; K. Ghosh; Y.D. Kolekar; C. V. Ramana
ACS Biomaterials Science & Engineering | 2016
Sumayya M. Ansari; Renuka D. Bhor; Kalpana Pai; S. Mazumder; Debasis Sen; Y.D. Kolekar; C. V. Ramana
Chemical Physics Letters | 2018
Sumayya M. Ansari; S.R. Suryawanshi; Mahendra A. More; Debasis Sen; Y.D. Kolekar; C. V. Ramana
Journal of Alloys and Compounds | 2017
Bhavna C. Keswani; R.S. Devan; R.C. Kambale; A.R. James; S. Manandhar; Y.D. Kolekar; C. V. Ramana