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Non-ambient X-ray and neutron diffraction of novel relaxor ferroelectric xBi(2)(Zn(2/3),Nb(1/3))O(3)–(1 – x)BaTiO(3)

The first determination of the phase diagram of the novel ferroelectric relaxor xBi(Zn(2/3)Nb(1/3))O(3)–(1 − x)BaTiO(3) (BZN-BT) has been achieved with a combination of high-resolution X-ray and neutron diffraction up to the miscibility limit near x(BZN) = 20.0% over a temperature range 20 < T &l...

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Detalles Bibliográficos
Autores principales: Marshall, Jessica, Walker, David, Thomas, Pamela
Formato: Online Artículo Texto
Lenguaje:English
Publicado: International Union of Crystallography 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8493627/
https://www.ncbi.nlm.nih.gov/pubmed/34667450
http://dx.doi.org/10.1107/S160057672100858X
Descripción
Sumario:The first determination of the phase diagram of the novel ferroelectric relaxor xBi(Zn(2/3)Nb(1/3))O(3)–(1 − x)BaTiO(3) (BZN-BT) has been achieved with a combination of high-resolution X-ray and neutron diffraction up to the miscibility limit near x(BZN) = 20.0% over a temperature range 20 < T < 400 K. The combined X-ray and neutron data show that the instability within the xBZN-(1−x)BT system reaches a maximum at x = 3.9% and is driven by B-site displacement and distortion of the oxygen octahedra in the polar phases. Composition-dependent effects include a narrow Amm2-dominated region focused at x = 3.9%, significant convergence of the lattice parameters in both P4mm and Amm2 phases, and sharp maxima in piezoelectric coefficient d (33) and maximum polarization P (max). Lattice parameter dilation at x ≥ 4.0% was observed for both P4mm and Amm2 unit cells, alongside the first appearance of Pm 3 m at 295 K and the onset of significant dielectric relaxation. Low-temperature neutron diffraction indicated a weak or non-existent temperature dependence on the transition from ferroelectric at x = 3.9% to ferroelectric relaxor at x = 4.0%. Temperature-dependent phase transitions were eliminated near x = 3.0%, with the ferroelectric limit observed at x = 5.0% and a transition to a low-loss relaxor dielectric near x = 8.0%.