Selcan TuncelBernard ChevalierSamir F. MatarRainer Pöttgen
Abstract The rare earth metal rich compounds RE 4 RuMg ( RE = La–Nd, Sm, Gd–Ho) were obtained by induction‐melting of the elements in sealed tantalum tubes in a water‐cooled sample chamber of a high‐frequency furnace. The RE 4 RuMg compounds were studied by powder X‐ray diffraction: Gd 4 RhIn type, $F {\rm {\bar 4}}{\rm 3}m$ , a = 1433.6(2) pm for La 4 RuMg, a = 1408.1(2) pm for Ce 4 RuMg, a = 1405.9(1) pm for Pr 4 RuMg, a = 1399.5(3) pm for Nd 4 RuMg, a = 1384.7(1) pm for Sm 4 RuMg, a = 1381.4(2) pm for Gd 4 RuMg, a = 1371.1(2) pm for Tb 4 RuMg, a = 1367.2(2) pm for Dy 4 RuMg, and a = 1361.4(5) pm for Ho 4 RuMg. The structures of RE 4 RuMg with RE = La, Pr, Nd, and Sm were refined from single crystal diffractometer data. The RE 4 RuMg structures consist of a three‐dimensional network of edge‐ and corner‐sharing Ru RE 6 trigonal prisms. In contrast to the isotypic series RE 4 CoMg and RE 4 RhMg, the ruthenium atoms displace from the centers of the prisms. The voids within the three‐dimensional network are filled by regular Mg 4 tetrahedra at a Mg–Mg distance of 316 pm in La 4 RuMg. The magnesium atoms have icosahedral coordination by three magnesium and nine rare earth metal atoms. The samarium based crystal revealed a small homogeneity range Sm 3−x Ru 1+y Mg 1+x−y leading to the refined composition Sm 3.92 Ru 1.16 Mg 0.92 . Chemical bonding in La 4 RuMg was studied in comparison with La 4 CoMg. The La1–Mg bonding is found to be dominating among the La–Mg interactions in both systems. Differences in chemical bonding due to a reduced valence electron concentration and different La2–Ru versus La3–Ru distances within RuLa2 3 La3 3 prisms are traced out.
Selcan TuncelBernard ChevalierSamir F. MatarRainer Poettgen
Svilen BobevTae‐Soo YouNian‐Tzu SuenShanta SahaR. L. GreeneJohnpierre Paglione
Vasyl‘ I. ZarembaUte Ch. RodewaldRainer Pöttgen
Nian‐Tzu SuenTae‐Soo YouSvilen Bobev
Ute Ch. RodewaldSelcan TuncelBernard ChevalierRainer Pöttgen