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Structure and phase stability of nanocrystalline Ce(1−x)Ln(x)O(2−x/2−δ) (Ln = Yb, Lu) in oxidizing and reducing atmosphere
The structure and phase evolution of nanocrystalline Ce(1−x)Ln(x)O(2−x/2−δ) (Ln = Yb, Lu, x = 0 − 1) oxides upon heating in H(2) was studied for the first time. Up to 950 °C the samples were single-phase, with structure changing smoothly with x from fluorite type (F) to bixbyite type (C). For the Lu...
Autores principales: | , , , , , |
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Formato: | Texto |
Lenguaje: | English |
Publicado: |
Springer Netherlands
2008
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2847157/ https://www.ncbi.nlm.nih.gov/pubmed/20376179 http://dx.doi.org/10.1007/s11051-008-9577-7 |
Sumario: | The structure and phase evolution of nanocrystalline Ce(1−x)Ln(x)O(2−x/2−δ) (Ln = Yb, Lu, x = 0 − 1) oxides upon heating in H(2) was studied for the first time. Up to 950 °C the samples were single-phase, with structure changing smoothly with x from fluorite type (F) to bixbyite type (C). For the Lu-doped samples heated at 1100 °C in the air and H(2), phase separation into coexisting F- and C-type structures was observed for ~0.40 < x < ~0.70 and ~0.25 < x < ~0.70, respectively. It was found also that addition of Lu(3+) and Yb(3+) strongly hinders the crystallite growth of ceria during heat treatment at 800 and 950 °C in both atmospheres. Valency of Ce and Yb in Ce(0.1)Lu(0.9)O(1.55−δ) and Ce(0.95)Yb(0.05)O(1.975−δ) samples heated at 1100 °C was studied by XANES and magnetic measurements. In the former Ce was dominated by Ce(4+), with small contribution of Ce(3+) after heating in H(2). In the latter, Yb existed exclusively as 3+ in both O(2) and H(2). |
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