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Investigation of the structure and phase transitions in the novel A-site substituted distorted perovskite compound Na<sub>0.5</sub>Bi<sub>0.5</sub>TiO<sub>3</sub>

947

Citations

18

References

2002

Year

TLDR

The study aims to investigate phase transition behavior in Na₀.₅Bi₀.₅TiO₃ by using second harmonic generation to determine the centrosymmetric or non‑centrosymmetric nature of its phases. Second harmonic generation measurements were employed to probe the symmetry of the material across its temperature‑dependent phase transitions. Rietveld neutron diffraction from 5 to 873 K revealed a cubic phase above 813 K, a tetragonal phase between 673–773 K, and a rhombohedral phase below 528 K, with coexistence of tetragonal/cubic (773–813 K) and rhombohedral/tetragonal (528–673 K) phases, and detailed structural parameters showing distinct octahedral tilt systems and temperature‑dependent cation displacements.

Abstract

Rietveld neutron powder profile analysis of the compound Na(0.5)Bi(0.5)TiO(3) (NBT) is reported over the temperature range 5-873 K. The sequence of phase transitions from the high-temperature prototypic cubic structure (above 813 K), to one of tetragonal (673-773 K) and then rhombohedral structures (5-528 K) has been established. Coexisting tetragonal/cubic (773-813 K) and rhombohedral/tetragonal (with an upper temperature limit of 145 K between 528 and 673 K) phases have also been observed. Refinements have revealed that the rhombohedral phase, space group R3c, with a(H) = 5.4887 (2), c(H) = 13.5048 (8) A, V = 352.33 (3) A(3), Z = 6 and D(x) = 5.99 Mg m(-3), exhibits an antiphase, a(-)a(-)a(-) oxygen tilt system, omega = 8.24 (4) degrees, with parallel cation displacements at room temperature. The tetragonal phase, space group P4bm, with a(T) = 5.5179 (2), c(T) = 3.9073 (2) A, V = 118.96 (1) A(3), Z = 2 and D(x) = 5.91 Mg m(-3), possesses an unusual combination of in-phase, a(0)a(0)c(+) oxygen octahedra tilts, omega = 3.06 (2) degrees, and antiparallel cation displacements along the polar axis. General trends of cation displacements and the various deviations of the octahedral network from the prototypic cubic perovskite structure have been established and their systematic behaviour with temperature is reported. An investigation of phase transition behaviour using second harmonic generation (SHG) to establish the centrosymmetric or non-centrosymmetric nature of the various phases is also reported.

References

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