Dec 2, 2024
11:15am - 11:30am
Hynes, Level 1, Room 108
Hangfeng Zhang1,Marcin Krynski2,A Dominic Fortes3,Theo Saunders1,Matteo Palma1,Yang Hao1,Franciszek Krok2,Haixue Yan1,Isaac Abrahams1
Queen Mary University of London1,Warsaw University of Technology2,Rutherford Appleton Laboratory3
Hangfeng Zhang1,Marcin Krynski2,A Dominic Fortes3,Theo Saunders1,Matteo Palma1,Yang Hao1,Franciszek Krok2,Haixue Yan1,Isaac Abrahams1
Queen Mary University of London1,Warsaw University of Technology2,Rutherford Appleton Laboratory3
The classical view of the structural changes that occur at the ferroelectric transition in perovskite structured systems, such as BaTiO<sub>3</sub>, is that polarization occurs due to the off-center displacement of the B-site cations. Here we show that in the bismuth sodium titanate (BNT) based composition 0.2(Ba<sub>0.4</sub>Sr<sub>0.6</sub>TiO<sub>3</sub>)-0.8(Bi<sub>0.5</sub>Na<sub>0.5</sub>TiO<sub>3</sub>), this model does not accurately describe the structural situation. Such BNT based systems are of interest as lead-free alternatives to currently used materials in a variety of piezo/ferroelectric applications. A combination of high-resolution powder neutron diffraction, impedance spectroscopy and ab initio calculations reveal that Ti<sup>4+</sup> contributes less than a third in magnitude to the overall polarization and that the displacements of the O<sup>2-</sup> ions and the A-site cations, particularly Bi<sup>3+</sup> are very significant. The detailed examination of the ferroelectric transition in this system offers insights applicable to the understanding of such transitions in other ferroelectric perovskites, particularly those containing lone pair elements.