锡
结晶学
四方晶系
钽
铂金
化学
微晶
衍射仪
晶体结构
分析化学(期刊)
材料科学
冶金
色谱法
生物化学
催化作用
作者
Steffen Klenner,Maximilian Kai Reimann,Stefan Seidel,Rainer Pöttgen
标识
DOI:10.1515/znb-2021-0080
摘要
Abstract Polycrystalline samples of the stannides Ca 1.692 Pt 2 Sn 3.308 , SrPtSn 2 and EuAuSn 2 were synthesized directly from the elements, using sealed tantalum ampoules as crucible material. The reactions were performed in muffle or induction furnaces. The phase purity of the samples was studied by X-ray powder diffraction (Guinier technique). The structures of Ca 1.692 Pt 2 Sn 3.308 and SrPtSn 2 were refined from single-crystal X-ray diffractometer data: NdRh 2 Sn 4 type, Pnma , a = 1887.22(13), b = 441.22(3), c = 742.89(4) pm, wR = 0.0626, 1325 F 2 values, 45 variables for Ca 1.692(8) Pt 2 Sn 3.308(8) and CeNiSi 2 type, Cmcm , a = 462.59(5), b = 1932.8(2), c = 458.00(5) pm, wR = 0.0549, 481 F 2 values, 18 variables for SrPtSn 2 . The calcium compound shows a homogeneity range Ca 1+ x Pt 2 Sn 4− x with substantial Sn4/Ca2 mixing on one of the 4 c Wyckoff positions. The [PtSn 2 ] network is characterized by Pt–Sn (269–281 pm) and Sn–Sn (306–336 pm) bonding interactions. SrPtSn 2 contains two different tin substructures: (i) Sn1–Sn1 zig-zag chains (282 pm) and (ii) orthorhombically distorted Sn2 squares (326 pm) with stronger and weaker Sn–Sn bonding. Together, the platinum and tin atoms build up a three-dimensional [PtSn 2 ] network in which the platinum atoms have a distorted square-pyramidal tin coordination with Pt–Sn distances ranging from 261–270 pm. EuAuSn 2 also crystallizes with the CeNiSi 2 -type structure with the lattice parameters a = 453.9(1), b = 2018.9(5) and c = 456.8(1) pm. Temperature dependent magnetic susceptibility studies indicate europium(II) with an experimental magnetic moment of 8.28(2) µ B per Eu atom. EuAuSn 2 is ordered antiferromagnetically at T N = 14.8(2) K. 151 Eu Mössbauer spectra confirm the oxidation state +2 for europium (isomer shift δ = −11.17(2) mm s −1 ) and the magnetic ordering at low temperature (21.8 T magnetic hyperfine field at 6 K).
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