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Crystal structure of ternary gallides NdCu5Ga6, GdCu6.87Ga4.13 and YbCu4.75Ga6.25
Authors: O.B. Mykhalichko, V.M. Mykhalichko, A.O. Fedorchuk, M.F. Fedyna
Number of views: 219
Crystal structures of the following ternary compounds were studied by X-ray powder method: NdCu5Ga6 (DRON-4.0 diffractometer, FeK-radiation, structure type (ST) BaCd11, Pearson symbol (PS) tI48, space group (SG) I41/amd, a=10.298(2) Å, c=6.625(2) Å, RB=0.0478, Rp=0.0454, 2=2.89), GdCu6.87Ga4.13 (DRON-4.0 diffractometer, FeK-radiation, ST BaCd11, PS tI48, SG I41/amd, a=10.2687(15) Å, c =6.60034(10) Å, RB=0.0414, Rp=0.0274, 2=1.86); and YbCu4.75Ga6.25 (STOE STADI P diffractometer, CuK1-radiation, ST BaCd11, PS tI48, SG I41/amd, a=10.3088(11) Å, c=6.6136(8) Å, RB=0.03854, Rp=0.0348, 2=3.46). The crystal structure of R(Cu,Ga)11 compounds is closely related to SmCu6.2Ga4.8 structure type according to the nearest coordination environment around the least electronegative atoms. The both structure types are realized at 8.33 at.% of R in the ternary systems R–Cu–Ga. The crystal structure of investigated compounds can be deduced from the structure of binary (RCu6, RGa6) and ternary (R2(Cu,Ga)17, R(Cu,Ga)12) phases. All structure types involve polyhedron in the form of a hexagonal prism with different number of additional atoms. The nearest coordination environment around R atoms transforms into the hexagonal antiprism with ten additional atoms in the structure of R(Cu,Ga)11 compounds.