3 research outputs found
A-site occupancy in the lead-free (Bi1/2Na1/2TiO3)0.94–(BaTiO3)0.06 piezoceramic: Combining first-principles study and TEM
The crystal structure of the lead-free piezoelectric ceramic (Bi1/2Na1/2TiO3)0.94–(BaTiO3)0.06 was investigated by first-principles calculations and high-resolution transmission electron microscopy (HRTEM) imaging. Structures with different A-site occupation were relaxed by total energy calculations within density functional theory and then used for simulating the corresponding HRTEM images. Simulated and experimental HRTEM images were compared and the closest match selected for structure interpretation. By combining these techniques, we have identified the Bi(Ba)/Na distribution on the A-site to be homogeneous. We exclude the possibility that regions visible in HRTEM images within one grain can be attributed to different ordering but to a slight tilting of the structure with respect to the electron beam
Crystallographic and Magnetic Structure of the Perovskite-Type Compound BaFeO<sub>2.5</sub>: Unrivaled Complexity in Oxygen Vacancy Ordering
We
report here on the characterization of the vacancy-ordered perovskite-type
structure of BaFeO<sub>2.5</sub> by means of combined Rietveld analysis
of powder X-ray and neutron diffraction data. The compound crystallizes
in the monoclinic space group <i>P</i>2<sub>1</sub>/<i>c</i> [<i>a</i> = 6.9753(1) Å, <i>b</i> = 11.7281(2) Å, <i>c</i> = 23.4507(4) Å, β
= 98.813(1)°, and <i>Z</i> = 28] containing seven crystallographically
different iron atoms. The coordination scheme is determined to be
Ba<sub>7</sub>(FeO<sub>4/2</sub>)<sub>1</sub>(FeO<sub>3/2</sub>O<sub>1/1</sub>)<sub>3</sub>(FeO<sub>5/2</sub>)<sub>2</sub>(FeO<sub>6/2</sub>)<sub>1</sub> = Ba<sub>7</sub>Fe<sup>[6]</sup><sub>1</sub>Fe<sup>[5]</sup><sub>2</sub>Fe<sup>[4]</sup><sub>4</sub>O<sub>17.5</sub> and is in agreement with the <sup>57</sup>Fe Mössbauer spectra
and density functional theory based calculations. To our knowledge,
the structure of BaFeO<sub>2.5</sub> is the most complicated perovskite-type
superstructure reported so far (largest primitive cell, number of
ABX<sub>2.5</sub> units per unit cell, and number of different crystallographic
sites). The magnetic structure was determined from the powder neutron
diffraction data and can be understood in terms of “G-type”
antiferromagnetic ordering between connected iron-containing polyhedra,
in agreement with field-sweep and zero-field-cooled/field-cooled measurements
Crystallographic and Magnetic Structure of the Perovskite-Type Compound BaFeO<sub>2.5</sub>: Unrivaled Complexity in Oxygen Vacancy Ordering
We
report here on the characterization of the vacancy-ordered perovskite-type
structure of BaFeO<sub>2.5</sub> by means of combined Rietveld analysis
of powder X-ray and neutron diffraction data. The compound crystallizes
in the monoclinic space group <i>P</i>2<sub>1</sub>/<i>c</i> [<i>a</i> = 6.9753(1) Å, <i>b</i> = 11.7281(2) Å, <i>c</i> = 23.4507(4) Å, β
= 98.813(1)°, and <i>Z</i> = 28] containing seven crystallographically
different iron atoms. The coordination scheme is determined to be
Ba<sub>7</sub>(FeO<sub>4/2</sub>)<sub>1</sub>(FeO<sub>3/2</sub>O<sub>1/1</sub>)<sub>3</sub>(FeO<sub>5/2</sub>)<sub>2</sub>(FeO<sub>6/2</sub>)<sub>1</sub> = Ba<sub>7</sub>Fe<sup>[6]</sup><sub>1</sub>Fe<sup>[5]</sup><sub>2</sub>Fe<sup>[4]</sup><sub>4</sub>O<sub>17.5</sub> and is in agreement with the <sup>57</sup>Fe Mössbauer spectra
and density functional theory based calculations. To our knowledge,
the structure of BaFeO<sub>2.5</sub> is the most complicated perovskite-type
superstructure reported so far (largest primitive cell, number of
ABX<sub>2.5</sub> units per unit cell, and number of different crystallographic
sites). The magnetic structure was determined from the powder neutron
diffraction data and can be understood in terms of “G-type”
antiferromagnetic ordering between connected iron-containing polyhedra,
in agreement with field-sweep and zero-field-cooled/field-cooled measurements