Please use this identifier to cite or link to this item: https://dspace.iiti.ac.in/handle/123456789/7532
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dc.contributor.authorPareek, Tanvien_US
dc.contributor.authorKumar, Sunilen_US
dc.date.accessioned2022-03-17T01:00:00Z-
dc.date.accessioned2022-03-21T11:11:57Z-
dc.date.available2022-03-17T01:00:00Z-
dc.date.available2022-03-21T11:11:57Z-
dc.date.issued2019-
dc.identifier.citationDwivedi, S., Chamoli, N., Pareek, T., Kumar, D., Kumar, P., & Kumar, S. (2019). Structural, dielectric, and piezoelectric properties of lead-free (1 − x)K1/2Na1/2NbO3 − xCa(Zn1/3Ta2/3)O3 perovskite solid solution. Journal of Materials Science: Materials in Electronics, 30(16), 15084-15096. doi:10.1007/s10854-019-01881-1en_US
dc.identifier.issn0957-4522-
dc.identifier.otherEID(2-s2.0-85070732177)-
dc.identifier.urihttps://doi.org/10.1007/s10854-019-01881-1-
dc.identifier.urihttps://dspace.iiti.ac.in/handle/123456789/7532-
dc.description.abstractPolycrystalline ceramics in (1 − x)K1/2Na1/2NbO3 − xCaZn1/3Ta2/3O3 (abbreviated as KNN-CZT) solid solution have been fabricated by using conventional solid-state synthesis route and the effect of CZT addition on the crystal structure, dielectric, and piezoelectric behaviour of KNN has been studied. Rietveld refinement of the room temperature X-ray diffraction data confirmed the crystal structure to be a pure perovskite phase for the compositions in the range x = 0 − 0.10. Further, the crystal structure gradually changed from orthorhombic to cubic via the formation of rhombohedral and tetragonal mixed phases with the increase in x. Raman spectroscopy suggested damping of phonon modes and a strong anharmonicity in the crystal arising due to the increased disorder in the structure as a consequence of multivalent cations occupying the A and B sites in CZT substituted compositions. Dielectric behaviour indicated the shifting of both tetragonal-cubic and orthorhombic–tetragonal phase transitions towards room temperature. The temperature dependent dielectric constant was modelled by Lorentz quadratic law, and the fitted value of diffuseness parameters confirmed an increase in diffuseness of phase transition with increasing substitution. Sample with the composition corresponding to x = 0.02 showed an improved piezoelectric coefficient d33 ~ 125 pC/N and electromechanical coupling coefficient kp ~ 30% at room temperature and d33 ~ 61 pC/N and kp ~ 24% at 300 °C which make this material a potential candidate for high-temperature piezoelectric applications. Variation of voltage coefficient (g33) with the change in compositions are also reported. Improvement in the piezoelectric properties is attributed to the reduced oxygen vacancies. © 2019, Springer Science+Business Media, LLC, part of Springer Nature.en_US
dc.language.isoenen_US
dc.publisherSpringer New York LLCen_US
dc.sourceJournal of Materials Science: Materials in Electronicsen_US
dc.subjectElectromechanical couplingen_US
dc.subjectHigh temperature applicationsen_US
dc.subjectPerovskiteen_US
dc.subjectPiezoelectricityen_US
dc.subjectRietveld refinementen_US
dc.subjectSolid solutionsen_US
dc.subjectZ transformsen_US
dc.subjectDiffuseness parametersen_US
dc.subjectElectromechanical coupling coefficientsen_US
dc.subjectPerovskite solid solutionsen_US
dc.subjectPiezoelectric coefficienten_US
dc.subjectPiezoelectric propertyen_US
dc.subjectPolycrystalline ceramicsen_US
dc.subjectPure perovskite phaseen_US
dc.subjectX-ray diffraction dataen_US
dc.subjectCrystal structureen_US
dc.titleStructural, dielectric, and piezoelectric properties of lead-free (1 − x)K1/2Na1/2NbO3 − xCa(Zn1/3Ta2/3)O3 perovskite solid solutionen_US
dc.typeJournal Articleen_US
Appears in Collections:Department of Metallurgical Engineering and Materials Sciences

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