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article
The nonstoichiometric ternary cerium iron sulfide Ce 2Fe 1.82S 5
Abstract
<p>The nonstoichiometric ternary cerium iron sulfide Ce <sub>2</sub>Fe <sub>1.82(6)</sub>S <sub>5</sub> was synthesized through reaction of the elements in a LiCl/KCl flux at 1120 K, and its structure was determined by single-crystal X-ray diffraction. Ce <sub>2</sub>Fe <sub>1.82</sub>S <sub>5</sub> crystallizes in the polar orthorhombic space group Pmn21 with a=3.9590(2) Å, b=16.413(1) Å, c=11.2362(9) Å and Z=4. The structure is a defect variant of the La <sub>2</sub>Fe <sub>2</sub>S <sub>5</sub> structure type. The parent structure contains both octahedral and tetrahedral iron sites, within one-dimensional chains of edge-sharing [FeS <sub>x</sub>]-polyhedra that run along the [100] direction. In Ce <sub>2</sub>Fe <sub>1.82</sub>S <sub>5</sub>, vacancies occur exclusively in the octahedral iron sites. The "tetrahedral" iron sites are split into three closely spaced partially occupied positions with coordination numbers of [4+1]. The presence of vacancies entails the partial oxidation of one of the cations to compensate the charge. The X-ray absorption near-edge structure (XANES) of the Ce M <sub>IV,V</sub> edge of Ce <sub>2</sub>Fe <sub>1.82</sub>S <sub>5</sub> showed no evidence of the occurrence of tetravalent cerium. The presence of Fe <sup>3+</sup> was unambiguously established on the basis of hyperfine fields observed in a <sup>57</sup>Fe-Mößbauer spectrum at 4.2 K. The temperature dependence of the reciprocal magnetic susceptibility (χ-1) of Ce <sub>2</sub>Fe <sub>1.82</sub>S <sub>5</sub> is nearly linear at higher temperatures. A rapid decrease in χ-1 below approximately 90 K suggests a ferrimagnetic transition.</p>