The crystal structures and magnetic properties of YbMg0.75In1.25 and Yb6Mg6.41In5.59

Maximilian Kai Reimann, Rainer Pöttgen
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Abstract

The quasi-binary system YbMg2-YbIn2 was studied around the equiatomic composition. In contrast to the ordered rare earth (RE) phases REMgIn (ZrNiAl type), ytterbium forms phases with different structures and pronounced Mg/In mixing (M sites). The structures of YbMg0.75In1.25 (CaLiSn type, P3m1, a = 501.95(7), c = 1087.3(2) pm, wR2 = 0.0490, 790 F 2 values, 32 variables) and Yb6Mg6.41In5.59 (Yb6Ir5Ga7 type, P63/mcm, a = 1060.77(14), c = 970.27(16) pm, wR2 = 0.0484, 701 F 2 values, 26 variables) were refined from single-crystal X-ray diffractometer data. YbMg0.75In1.25 is an AlB2 superstructure with a tripling of the subcell. The magnesium and indium atoms form three differently puckered layers of M 6 hexagons. The Yb6Mg6.41In5.59 structure is derived from the hexagonal Laves phase YbMg2 (MgZn2 type, P63/mmc). A klassengleiche symmetry reduction leads to four crystallographically independent M sites for the rows of corner- and face-sharing tetrahedra which allow a composition close to the equiatomic one. The MM distances in both structures cover the broad range from 289 to 331 pm, comparable to the sums of the covalent radii. Temperature dependent magnetic susceptibility studies of the polycrystalline YbMg0.75In1.25 and Yb12Mg13In11 samples indicate Pauli paramagnetism with room temperature values of 2.8(1) × 10−3 emu mol−1 (YbMg0.75In1.25) and 5.2(1) × 10−3 emu mol−1 (Yb12Mg13In11).
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YbMg0.75In1.25 和 Yb6Mg6.41In5.59 的晶体结构和磁性能
围绕等原子成分对准二元体系 YbMg2-YbIn2 进行了研究。与有序稀土(RE)相 REMgIn(ZrNiAl 型)相反,镱形成的相具有不同的结构和明显的镁/铟混合(M 位点)。YbMg0.75In1.25 (CaLiSn 型,P3m1,a = 501.95(7),c = 1087.3(2) pm,wR2 = 0.0490,790 F 2 值,32 个变量)和 Yb6Mg6.41In5.59 (Yb6Ir5.59(Yb6Ir5Ga7 型,P63/mcm,a = 1060.77(14),c = 970.27(16) pm,wR2 = 0.0484,701 F 2 值,26 个变量)是根据单晶 X 射线衍射仪数据精制而成的。YbMg0.75In1.25 是一种 AlB2 超结构,其子单元增加了两倍。镁原子和铟原子形成三个不同的 M 6 六边形皱褶层。Yb6Mg6.41In5.59 结构源自六方拉维斯相 YbMg2(MgZn2 型,P63/mmc)。通过类对称性还原,在角和面共享四面体行中产生了四个晶体学上独立的 M 位点,从而使其成分接近于等原子。这两种结构中的 M-M 间距覆盖了从 289 到 331 pm 的宽广范围,与共价半径之和相当。对多晶 YbMg0.75In1.25 和 Yb12Mg13In11 样品进行的温度相关磁感应强度研究表明,它们具有保利顺磁性,室温值分别为 2.8(1) × 10-3 emu mol-1(YbMg0.75In1.25)和 5.2(1) × 10-3 emu mol-1(Yb12Mg13In11)。
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