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(Ln = Tb - Yb), LnNiAs (Ln = La - Nd, Sm, Gd, Dy - Yb), and UNiAs

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Ternary Rare Earth and Uranium Nickel Arsenides Ln

2

NiAs

2

(Ln = Tb - Yb), LnNiAs (Ln = La - Nd, Sm, Gd, Dy - Yb), and UNiAs

Wolfgang Jeitschko, Ludger J. Terb¨uchte, and Ute Ch. Rodewald

Anorganisch-Chemisches Institut, Universit¨at M¨unster,

Wilhelm Klemm-Strasse 8, D-48149 M¨unster, Germany Reprint requests to W. Jeitschko. Fax: +49(0)251 8333 136.

Z. Naturforsch.56 b,1281–1288 (2001); received August 12, 2001 Rare Earth Compounds, Arsenides, Displacive Phase Transition

The new compounds Tm2NiAs2and Yb2NiAs2crystallize with a hexagonal structure similar to that reported for Zr2NiAs2. It was refined for Tm2NiAs2from single-crystal X-ray data in the polar space group P63mc: a = 408.4(1), c = 1374.2(3) pm, R = 0.044 for 176 structure factors and 16 variable parameters. The compounds Ln2NiAs2(Ln = Tb - Er) are confirmed to crystallize with an analogous structure from X-ray powder data. In contrast to the earlier structure refinement of Zr2NiAs2in the higher-symmetric space group P63/mmc, where the honeycomb layers of nickel and arsenic atoms are described as planar, these layers are puckered in Tm2NiAs2. These compounds are expected to undergo a displacive phase transition, with the centrosymmetric space group P63/mmc to be correct at high temperature. Since the room temperature structure is polar, these compounds might be classified as ferroelectric from a symmetry point of view. The equiatomic title compounds LnNiAs and UNiAs crystallize with a related hexagonal structure corresponding to a superstructure of the AlB2type with lattice constants varying between a = 416.2(1), c = 1636.1(4) pm for LaNiAs and a = 401.9(2), c = 1488.5(5) pm for YbNiAs. The crystal chemistry of these hexagonal structures is briefly discussed. Using oxidation numbers chemical bonding in the lanthanoid containing compounds may be rationalized with the formulas (Ln+3)2Ni(As 3)2 and Ln+3NiAs 3, thus suggesting semiconducting behavior.

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