Cargando…
Percolating hierarchical defect structures drive phase transformation in Ce(1−x)Gd(x)O(2−x/2): a total scattering study
A new hierarchical approach is presented for elucidating the structural disorder in Ce(1−x)Gd(x)O(2−x/2) solid solutions on different scale lengths. The primary goal of this investigation is to shed light on the relations between the short-range and the average structure of these materials via an an...
Autores principales: | , , , , , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
International Union of Crystallography
2015
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4547819/ https://www.ncbi.nlm.nih.gov/pubmed/26306193 http://dx.doi.org/10.1107/S2052252515011641 |
Sumario: | A new hierarchical approach is presented for elucidating the structural disorder in Ce(1−x)Gd(x)O(2−x/2) solid solutions on different scale lengths. The primary goal of this investigation is to shed light on the relations between the short-range and the average structure of these materials via an analysis of disorder on the mesocopic scale. Real-space (pair distribution function) and reciprocal-space (Rietveld refinement and microstructure probing) analysis of X-ray powder diffraction data and electron spin resonance (ESR) investigations were carried out following this approach. On the local scale, Gd- and Ce-rich droplets (i.e. small regions a few ångströms wide) form, exhibiting either a distorted fluorite (CeO(2)) or a C-type (Gd(2)O(3)) structure in the whole compositional range. These droplets can then form C-type nanodomains which, for Gd concentrations x (Gd) ≤ 0.25, are embedded in the fluorite matrix. At the site percolation threshold p (C) for a cubic lattice (x (Gd) = p (C) ≃ 0.311), C-type nanodomains percolate inside each crystallite and a structural phase transformation is observed. When this occurs, the peak-to-peak ESR line width ΔH (pp) shows a step-like behaviour, which can be associated with the increase in Gd–Gd dipolar interactions. A general crystallographic rationale is presented to explain the fluorite-to-C-type phase transformation. The approach shown here could be adopted more generally in the analysis of disorder in other highly doped materials. |
---|