2017
DOI: 10.1016/j.jssc.2017.02.002
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Phase equilibria, crystal structure and properties of complex oxides in the Nd 2 O 3 –SrO–CoO system

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Cited by 13 publications
(5 citation statements)
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“…Samples with the overall composition corresponding to the Sm 2– z Sr z O 3– z /2 formula, with z = 0.05, 0.1, and 0.15, were annealed at 1100 °C in air for 120 h and quenched to room temperature. XRD examination showed that, in contrast to the Nd‐containing system, where the Nd 2– z Sr z O 3– z /2 solid solution formed within the range 0 ≤ z ≤ 0.15, no signs of solid‐solution formation was detected in the Sm 2 O 3 –SrO system. This fact also emphasizes the distinct difference in the phase formation of the Nd and Sm oxides, as it was similarly shown for the perovskite solid solutions, in spite of the relatively small difference in their ionic radii.…”
Section: Resultsmentioning
confidence: 87%
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“…Samples with the overall composition corresponding to the Sm 2– z Sr z O 3– z /2 formula, with z = 0.05, 0.1, and 0.15, were annealed at 1100 °C in air for 120 h and quenched to room temperature. XRD examination showed that, in contrast to the Nd‐containing system, where the Nd 2– z Sr z O 3– z /2 solid solution formed within the range 0 ≤ z ≤ 0.15, no signs of solid‐solution formation was detected in the Sm 2 O 3 –SrO system. This fact also emphasizes the distinct difference in the phase formation of the Nd and Sm oxides, as it was similarly shown for the perovskite solid solutions, in spite of the relatively small difference in their ionic radii.…”
Section: Resultsmentioning
confidence: 87%
“…Although the difference between the ionic radii of Nd 3+ ( r = 1.27 Å) and Sm 3+ ( r = 1.24 Å) is not so big, the increasing difference of the Ln radii, compared with that for Sr 2+ , is critical for the formation of the Sr 1– x Ln x CoO 3– δ solid solutions. It becomes obvious, if one compares the formation of the orthorhombic Nd‐rich Sr 1– x Nd x CoO 3– δ solid solution (0.5 ≤ x ≤ 1), in contrast with the double‐phase region for the Sm‐containing system and the formation of different superstructure types inside the Ln‐poor region: a p × a p × 2 a p for Nd, or 2 a p × 2 a p × 4 a p for Sm . Such a significant difference in the phase relationship that appears between the Nd‐ and Sm‐containing systems in the row of Ln 2 O 3 –SrO–CoO systems, is similar to that appearing in the row of Ln 2 O 3 –BaO–CoO systems.…”
Section: Resultsmentioning
confidence: 99%
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“…In order to check the possible formation of a superstructure due to the ordering of oxygen vacancies and/or ordering of metal ions in A‐sublattice, which use to appear in the related Sr‐rich perovskite oxides, electron diffraction measurements were performed for the Sr 0.8 Y 0.2 FeO 3−δ sample. Figure demonstrates the ideal perovskite cubic cell without any additional reflections.…”
Section: Resultsmentioning
confidence: 99%
“…The measurement of the interlayer distances revealed the expansion of the La–La distance from a typical 0.38 to 0.46 nm in the V O stripe. Both the appearance of dark contrast Co–O layers and the increase in La–La distances can be attributed to V O layers, as has been previously observed in perovskite structures. Such layers of V O change Co coordination from CoO 6 octahedral to CoO 5 square pyramidal. The formation of V O in the DES-synthesized perovskites is consistent with our previous studies, , where we used a DES route to prepare mixed-valent ternary Zn and Cu vanadates ( M 2 V 2 O 7– m and M V 2 O 6– n , M = Zn or Cu) and found annealing the reaction mixture to intrinsically introduce V O .…”
Section: Resultsmentioning
confidence: 53%