4.6 Article

Relaxor behaviour and phase transition of perovskite ferroelectrics-type complex oxides (1-x)Na0.5Bi0.5TiO3-xCaTiO3 system

期刊

JOURNAL OF ADVANCED CERAMICS
卷 7, 期 2, 页码 124-142

出版社

SPRINGER
DOI: 10.1007/s40145-018-0264-6

关键词

relaxor behaviour; dielectric properties; Vogel-Fulcher relationship; polar nanoregions (PNRs); X-ray diffraction; Raman spectroscopy

资金

  1. French Ministry of Higher Education and Research
  2. Nanosciences Department of Universite de Bourgogne

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Polycrystalline powders of (1-x)Na0.5Bi0.5TiO3-xCaTiO(3) ((1-x)NBT-xCT, 0 <= x <= 0.55) have been synthesized by solid state route. The effects of simultaneous substitution of Na+/Bi3+ at A-site in NBT on structural and dielectric properties were investigated. X-ray diffraction analysis revealed the phase transition from rhombohedral structure (x = 0) to orthorhombic structure (x >= 0.15). A distinct behaviour in dielectric properties was obtained, where for x = 0, a normal ferroelectric behaviour was observed, whereas for x >= 0.15, a broad dielectric anomaly was revealed such that the maximum temperature (T-m) strongly depended on the frequency and shifted towards low temperature with CT. The dielectric dispersion indicated a relaxor behaviour revealed by the degree of diffuseness and modelled via Vogel-Fulcher relation. The study highlighted the relaxor behaviour as a function of frequency and proved the transformation from a relaxor high-frequency dependence to a paraelectric phase at temperature T-s. The distinct variation of the Raman spectra at room temperature was correlated with X-ray diffraction results and proved the already mentioned transition. On heating (-193-500 degrees C), the Raman spectra confirmed the structural stability (Pnma) of the materials. The phonon behaviour for x = 0.15 was discussed in terms of the appearance of polar nanoregions (PNRs) into a non-polar orthorhombic matrix responsible of the relaxor behaviour. For x = 0.20, unchanged phonon behaviour confirmed the variation in dielectric behaviour where the solids transformed from a relaxor to a paraelectric state without structural phase transition.

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