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The crystal structures and magnetic properties of YbMg0.75In1.25 and Yb6Mg6.41In5.59
Zeitschrift für Naturforschung B ( IF 0.8 ) Pub Date : 2024-02-14 , DOI: 10.1515/znb-2023-0106 Maximilian Kai Reimann 1 , Rainer Pöttgen 1
Zeitschrift für Naturforschung B ( IF 0.8 ) Pub Date : 2024-02-14 , DOI: 10.1515/znb-2023-0106 Maximilian Kai Reimann 1 , Rainer Pöttgen 1
Affiliation
The quasi-binary system YbMg2 -YbIn2 was studied around the equiatomic composition. In contrast to the ordered rare earth (RE ) phases RE MgIn (ZrNiAl type), ytterbium forms phases with different structures and pronounced Mg/In mixing (M sites). The structures of YbMg0.75 In1.25 (CaLiSn type, P 3m 1, a = 501.95(7), c = 1087.3(2) pm, wR 2 = 0.0490, 790 F 2 values, 32 variables) and Yb6 Mg6.41 In5.59 (Yb6 Ir5 Ga7 type, P 63 /mcm , a = 1060.77(14), c = 970.27(16) pm, wR 2 = 0.0484, 701 F 2 values, 26 variables) were refined from single-crystal X-ray diffractometer data. YbMg0.75 In1.25 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 Yb6 Mg6.41 In5.59 structure is derived from the hexagonal Laves phase YbMg2 (MgZn2 type, P 63 /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 M –M 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 YbMg0.75 In1.25 and Yb12 Mg13 In11 samples indicate Pauli paramagnetism with room temperature values of 2.8(1) × 10−3 emu mol−1 (YbMg0.75 In1.25 ) and 5.2(1) × 10−3 emu mol−1 (Yb12 Mg13 In11 ).
中文翻译:
YbMg0.75In1.25和Yb6Mg6.41In5.59的晶体结构和磁性能
准二元系 YbMg2 -YbIn2 围绕等原子组成进行了研究。与有序稀土相比(关于 ) 阶段关于 MgIn(ZrNiAl 型),镱形成具有不同结构的相和明显的 Mg/In 混合(中号 站点)。 YbMg的结构0.75 在1.25 (钙锂锡型,磷 3米 1、A = 501.95(7),C = 1087.3(2) 下午,WR 2 = 0.0490, 790F 2 值,32 个变量)和 Yb6 镁6.41 在5.59 (镱6 红外线5 嘎7 类型,磷 63 /微厘米 ,A = 1060.77(14),C = 970.27(16) 下午,WR 2 = 0.0484, 701F 2 值,26 个变量)是根据单晶 X 射线衍射仪数据精炼的。镱镁0.75 在1.25 是一个AlB2 上层建筑的子单元增加了三倍。镁和铟原子形成三个不同的褶皱层中号 6 六边形。镱6 镁6.41 在5.59 结构源自六方拉夫斯相 YbMg2 (镁锌2 类型,磷 63 /MMC )。 A阶级 对称性降低导致四个晶体学独立中号 角和面共享四面体行的位点,允许接近等原子的组成。这中号 –中号 两个结构中的距离涵盖了从 289 到 331 pm 的广泛范围,与共价半径的总和相当。多晶 YbMg 的温度依赖性磁化率研究0.75 在1.25 和镱12 镁13 在11 样品表明泡利顺磁性,室温值为 2.8(1) × 10−3 鸸鹋摩尔−1 (镱镁0.75 在1.25 ) 和 5.2(1) × 10−3 鸸鹋摩尔−1 (镱12 镁13 在11 )。
更新日期:2024-02-14
中文翻译:
YbMg0.75In1.25和Yb6Mg6.41In5.59的晶体结构和磁性能
准二元系 YbMg