A polycrystalline sample of Sr 2 FeIrO 6 has been synthesized and shown by a combination of X-ray di4raction, neutron di4raction, magnetometry, and MoK ssbauer spectroscopy to be a triclinic (space group I1 ; a : 5.54996(3) A s , b : 5.57847(3) A s , c : 7.84165(3) A s , : 89.990(1)3, : 90.059(1)3,
Electronic and structural properties of Sr2YSbO6
✍ Scribed by O. Ortiz-Diaz; M. Jairo Arbey Rodríguez; F. Fajardo; D.A. Landínez Téllez; J. Roa-Rojas
- Publisher
- Elsevier Science
- Year
- 2007
- Tongue
- English
- Weight
- 418 KB
- Volume
- 398
- Category
- Article
- ISSN
- 0921-4526
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✦ Synopsis
The electronic and structural properties of the cubic perovskite Sr 2 YSbO 6 were predicted from ab initio calculations. Such properties were obtained using the density functional theory (DFT). The full-potential (linearized) augmented plane-wave ((L)APW) method was used, as it is implemented in wien2k code. We have optimized the volume of the unitary cell and the internal x parameter. The lattice constant ðaÞ and x determine some length bonds. We have found that a ¼ 8:405 A ˚, x ¼ 0:26177, and the bond lengths Y-O and Sb-O are 2.20 and 2.00 A ˚, respectively. Additionally, Sr 2 YSbO 6 was prepared experimentally by the solid-state reaction method using stoichiometric mixtures of high purity (99.99%). By means of X-ray and Rietveld analysis, the main structural features were determined. The experimental lattice parameter is a ¼ 8:249 A ˚, which differs about 1.9% of the value obtained using DFT. The bulk modulus is $133 GPa, which is not measured experimentally. DFT predicts that Sr 2 YSbO 6 is an indirect semiconductor and magnetic behavior does not have to be expected because at Fermi level the dominant orbitals are p-oxygen. The gap of the material is at least 2.5 eV.
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Synthesis, electrical, and magnetic properties of a layered perovskite-related compound, \(\mathrm{Sr}_{3} \mathrm{~V}_{2} \mathrm{O}_{6.99}\), are reported. Powder \(\mathrm{X}\)-ray diffraction analysis confirmed the body-centered tetragonal (I4/ \(\mathrm{mmm})\) structure as proposed earlier. Th