Article ID Journal Published Year Pages File Type
1331864 Journal of Solid State Chemistry 2006 12 Pages PDF
Abstract

The ErCo3–D2 system has been studied by in situ neutron powder diffraction (NPD) at 60 °C and 0–16 bar deuterium pressure. Two deuteride phases were identified, β-ErCo3D1.07−1.38 and γ-ErCo3D3.7−4.3. They were structurally characterized at the compositions β-ErCo3D1.37 and γ-ErCo3D3.7 by high-resolution neutron and synchrotron powder diffraction. In contrast to the analogous nickel systems RNi3–D2 (R=Er, Ho; see part I, J. Alloys and Compds. 404–406 (2005) 89–94, and part II, J. Alloys and Compds. 2005, in press), their structures preserve the symmetry of the parent alloy (PuNi3-type, space group R-3m). Deuterium occupies mainly AB2 building blocks in the β-phase, and AB2 and AB5 building blocks in the γ-phase. In the AB2 building blocks cobalt is surrounded by an average of 3.8 (β-ErCo3D1.37) and 4.4 D-atoms (γ-ErCo3D3.7) in disordered distorted octahedral configurations (point symmetry −3), in contrast to nickel that is surrounded by ∼3 (β1- and β2-RNi3Dx, R=Er, Ho) and ∼4 (γ-ErNi3D3.7) D-atoms in disordered trigonal (pyramidal) and tetrahedral configurations, respectively (point symmetry 3). These results indicate that the D-atom distributions in this homologous series depend on the nature of the transition element rather than on geometric factors, and that directional bonding effects similar to those in non-metallic complex transition metal hydrides also prevail in metallic interstitial metal hydrides.

Graphical abstractAxial ratio c/a versus rhombohedral cell volume of ErCo3–deuterium system showing single- and two-phase regions.Figure optionsDownload full-size imageDownload as PowerPoint slide

Related Topics
Physical Sciences and Engineering Chemistry Inorganic Chemistry
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