Ln 3 M 1 − δ TX 7 – quasi-isostructural compounds: stereochemistry and silver-ion motion in the Ln 3 Ag 1 − δ GeS 7 (Ln = La–Nd, Sm, Gd–Er and Y; δ = 0.11–0.50) compounds
The crystal structures of the Ln 3 Ag 1 − δ GeS 7 (Ln = La–Nd, Sm, Gd–Er, Y; δ = 0.11–0.50, space group P 6 3 ) compounds were determined by means of X-ray single-crystal diffraction and the similarities among the crystal structures of all Ln 3 M 1 − δ TX 7 (space group P 6 3 ; Ln – lanthanide eleme...
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Veröffentlicht in: | Acta crystallographica. Section B, Structural science Structural science, 2009-04, Vol.65 (2), p.126-133 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | The crystal structures of the Ln 3 Ag 1 − δ GeS 7 (Ln = La–Nd, Sm, Gd–Er, Y; δ = 0.11–0.50, space group P 6 3 ) compounds were determined by means of X-ray single-crystal diffraction and the similarities among the crystal structures of all Ln 3 M 1 − δ TX 7 (space group P 6 3 ; Ln – lanthanide element, M – monovalent element; T – tetravalent element and X – S, Se) compounds deposited in the Inorganic Crystal Structure Database (ICSD) are discussed. Substitutions of each element in Ln 3 M 1 − δ TX 7 result in a different structural effect. On the basis of the data deposited in the ICSD the large family of the Ln 3 M 1 − δ TX 7 compounds was divided into three groups depending on the position of the monovalent element in the lattice. This position determines what kind of stereoisomer is present in the structure, either the ++ enantiomer or the +− diastereoisomer. Since the silver ions can occupy a different position and the energy barriers between positions are low the ions can move through the channel. It was shown that this movement is not a stochastic process but a correlated one. |
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ISSN: | 0108-7681 |
DOI: | 10.1107/S010876810900144X |