Exploring the tetragonal crystal structure of perovskites BaLa <sub>2</sub> Cu <sub> 1− <i>x</i> </sub> Ba <i> <sub>x</sub> </i> Ti <sub>2</sub> O <sub>9</sub> ( <i>x</i>  = 0.00, 0.15, 0.30) via X-ray diffraction and the Rietveld method

Abstract BaLa 2 Cu 1− x Ba x Ti 2 O 9 ( x = 0.00, 0.15, and 0.30) ceramics were synthesized in polycrystalline form via the conventional solid-state reaction techniques in air. The crystal structure of the title compositions was characterized by room-temperature X-ray powder diffraction and analyzed using the Rietveld refinement method. All the compositions crystallize in the tetragonal symmetry of space group I 4/ mcm (No. 140) with cell volumes: 249.43(1) Å 3 for x = 0.00, 249.42(1) Å 3 for x = 0.15, and 250.05(1) Å 3 for x = 0.30. The tilt system of the M O 6 octahedra ( M = Cu(Ba2)/Ti) corresponds to the notation a 0 a 0 c − . The M O 6 octahedra share the corners via oxygen atoms in 3 D. Along the c -axis, the octahedra are connected by O(1) atoms of (0, 0, 1/4) positions; while in the ab -plane, they are linked by O(2) atoms of ( x , x + 1/2, 0) positions. The bond angle of M –O2– M is 168.6(7)° for x = 0.00, 168.6(6)° for x = 0.15, and 166.8(6)° for x = 0.30, whereas the bond angle of M –O1– M is constrained to be 180° by space group I 4/ mcm.

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Publication Details

Journal
Powder Diffraction
Published
2025-11-05
DOI
https://doi.org/10.1017/s0885715625101012
Primary Topic
Dielectric properties of ceramics
Type
article
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article

Exploring the tetragonal crystal structure of perovskites BaLa 2 Cu 1− x Ba x Ti 2 O 9 ( x  = 0.00, 0.15, 0.30) via X-ray diffraction and the Rietveld method

Abdelhadi El Hachmi
Powder Diffraction
Dielectric properties of ceramics
article

Exploring the tetragonal crystal structure of perovskites BaLa 2 Cu 1− x Ba x Ti 2 O 9 ( x  = 0.00, 0.15, 0.30) via X-ray diffraction and the Rietveld method

Abdelhadi El Hachmi
article en

Abstract

Abstract BaLa 2 Cu 1− x Ba x Ti 2 O 9 ( x = 0.00, 0.15, and 0.30) ceramics were synthesized in polycrystalline form via the conventional solid-state reaction techniques in air. The crystal structure of the title compositions was characterized by room-temperature X-ray powder diffraction and analyzed using the Rietveld refinement method. All the compositions crystallize in the tetragonal symmetry of space group I 4/ mcm (No. 140) with cell volumes: 249.43(1) Å 3 for x = 0.00, 249.42(1) Å 3 for x = 0.15, and 250.05(1) Å 3 for x = 0.30. The tilt system of the M O 6 octahedra ( M = Cu(Ba2)/Ti) corresponds to the notation a 0 a 0 c − . The M O 6 octahedra share the corners via oxygen atoms in 3 D. Along the c -axis, the octahedra are connected by O(1) atoms of (0, 0, 1/4) positions; while in the ab -plane, they are linked by O(2) atoms of ( x , x + 1/2, 0) positions. The bond angle of M –O2– M is 168.6(7)° for x = 0.00, 168.6(6)° for x = 0.15, and 166.8(6)° for x = 0.30, whereas the bond angle of M –O1– M is constrained to be 180° by space group I 4/ mcm.

Powder DiffractionVol. 40(4)
Abdelmalek Essaâdi University (MA)
Openalex Percentile: Top 74%
Dielectric properties of ceramics
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