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Measuring Magnetically-Tuned Ferroelectric Polarization in Liquid Crystals
Published on: August 15, 2018
Room-Temperature Ferroelectric-Antiferroelectric Transitions in NaNbO3 Materials
Amira Bougoffa1, Ala Eddin Mabrouki1,2, Abdessalem Trabelsi1
1Laboratory of Applied Physics, Faculty of Sciences of Sfax, University of Sfax, B. P. 1171, Sfax 3000, Tunisia.
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The recent development of dielectric phase transitions in solid-state materials reveals the main role of structural phase transitions, which generate new properties emerging by external stimulation. In this context, the present study aimed to investigate structural, morphological, dielectric, and electric characteristics of sodium niobate NaNbO3, prepared by solid-state reaction. X-ray powder diffraction results exhibited that this material crystallizes in an orthorhombic perovskite structure, proving the existence of both Pbcm and P21ma space groups at room temperature. Furthermore, a microstructural investigation, based on scanning electron microscopy, showed multigrain agglomerations of about 600 nm consisting of fine crystallites with irregular shapes and sizes. Moreover, dielectric and electrical findings, obtained by wide-range impedance spectroscopy of frequencies [102-106 Hz] and temperatures [220-400 K], revealed the possibility of a FE-AFE dielectric phase transition accompanied by a P21ma-Pbcm structural phase transition at room temperature. Thus, the AC conductivity plots follow Jonscher's power law with thermal activation according to Arrhenius' law by 0.320 and 0.646 eV energies, probably attributed to the FE and AFE phases, respectively. Concerning charge carrier transport, it is demonstrated that the correlated barrier jump (CBH) model or the small polar tunnel model (NSPT) was considered to be the most appropriate to interpret the conduction mechanisms of the NaNbO3 ceramic in the considered temperature range.
