Abstract Pure samples of CaPdSn, CaPtSn, SrPtSn, SrAuSn and BaAuSn can be prepared by reacting the elements in glassy carbon crucibles or in sealed tantalum tubes in a water-cooled sample chamber of a high-frequency furnace. The stannides have been investigated by X-ray diffraction on powders. Single crystal data yielded: TiNiSi type, Pnma , a =764.16(7), b =470.74(4), c =799.64(7) pm, wR 2 =0.0622, 469 F 2 values, 20 variables for SrPtSn, and CaCuGe type, Pnma , a =2341.4(3), b =481.80(5), c =826.7(1) pm, wR 2 =0.1368, 1136 F 2 values, 56 variables for SrAuSn. The platinum (gold) and tin atoms form two-dimensional layers of puckered Pt 3 Sn 3 and Au 3 Sn 3 hexagons with short PtSn (276 and 278 pm) and AuSn (279–286 pm) intralayer distances. These condensed two-dimensionally infinite nets are interconnected to each other via PtSn contacts (279 pm) in SrPtSn. In SrAuSn very weak interlayer AuSn (312 pm) and AuAu (340 pm) contacts occur, but stronger SnSn (304 pm) interactions. The SrAuSn structure is a superstructure of SrPtSn resulting from an isomorphic transition of index 3 from Pnma to Pnma . The KHg 2 type subcell of BaAuSn was determined from Guinier powder data: Imma , a =493.5(1), b =817.2(1), c =844.5(1) pm. 119 Sn Mossbauer spectra of TiNiSi type CaPdSn and CaPtSn show a single signal at 77 K at isomer shifts of δ =1.964(5) and 1.857(4) mm s −1 , respectively, subject to quadrupole splitting of ΔE Q =0.94(3) and 0.89(1) mm s −1 . SrAuSn shows two superimposed signals in a ratio of 2:1 at 77 K: δ 1 =2.03(5), δ 2 =2.12(5) mm s −1 , ΔE Q1 =0.9(1) and ΔE Q2 =0.6(2) mm s −1 .
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