Polycrystalline samples of BaCe x Zr 1؊x O 3 were prepared by solid state reaction. X-ray diffraction measurements show that all compounds are single-phase and XRD patterns can be indexed on the basis of the ideal perovskite structure. However, Raman data show that BaCe x Zr 1؊x O 3 exhibits slight
A High-Pressure Raman Study of Mixed Perovskites BaCexZr1−xO3 (0≤x≤1)
✍ Scribed by C. Chemarin; N. Rosman; T. Pagnier; G. Lucazeau
- Publisher
- Elsevier Science
- Year
- 2000
- Tongue
- English
- Weight
- 302 KB
- Volume
- 149
- Category
- Article
- ISSN
- 0022-4596
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✦ Synopsis
A high-pressure Raman study of polycrystalline samples of BaCe x Zr 1؊x O 3 is performed at room temperature. The evolution of Raman spectra with pressure is compared to the evolution of the Raman spectra of BaZrO 3 and BaCeO 3 . The e4ect of composition on the pressure-induced phase transitions is monitored from the Raman spectra. Transitions toward lower symmetry phases as pressure increases are evidenced. A phase diagram in the binary system BaZrO 3 +BaCeO 3 based on the Raman spectra characteristic of the di4erent structures of BaCeO 3 (Pnma, Imma, R3 c, Pm3m) is proposed. The transition pressures toward low-symmetry structures decrease when Ce is replaced for Zr. This study allows us to interpret the BaCe x Zr 1؊x O 3 (04x41) Raman spectra at ambient pressure on the basis of nanodomains and nanophases. These objects tend to disappear upon pressure increase. The octahedra to dodecahedra volumes ratio is used as a critical parameter that is able to reproduce qualitatively some of the phase transitions in the mixed perovskites BaCe x Zr 1؊x O 3 . In order to calculate this parameter vs pressure, a derivation of the samples: compressibility based on a polyhedral approach is performed and is found in the range [0.7؋10 ؊11 +1.0؋ 10 ؊11 Pa ؊1 ].
📜 SIMILAR VOLUMES
The magnetization and crystal structure of Ca 1؊x Eu x MnO 3 (04x41) perovskites have been studied. It is shown that these compounds present four concentration regions in which different magnetic phases coexist. The antiferromagnetic phase is associated with a regular arrangement of Mn 3؉ and Mn 4؉