Several ternary rare-earth metals containing titanium aluminum intermetallics in the RE2TiAl3 series (RE = Y, Gd–Lu) have been synthesized from the elements using arc-melting techniques. All compounds crystallize in the trigonal crystal system with rhombohedral space group R3-m (Z = 3) and lattice parameters ranging between a = 582–570 and c = 1353–1358 pm. They adopt the Mg2Ni3Si-type structure, which is an ordered superstructure of the cubic Laves phase MgCu2 and has been observed for Al intermetallics for the first time. Tetrahedral [TiAl3] entities that are connected over all corners form a network where the empty [TiAl3] tetrahedra exhibit a full Ti/Al ordering based on the single crystal results. The Al atoms are arranged into 63 Kagomé nets, while the Ti atoms connect these nets over the triangular units. In the cavities of this three-dimensional arrangement, the RE cations can be found forming a distorted diamond-type substructure. Magnetic measurements revealed that Y2TiAl3 and Lu2TiAl3 are Pauli paramagnetic substances, in line with the metallic character. The other compounds exhibit paramagnetism with antiferromagnetic ordering at a maximum Néel temperature of TN = 26.1(1) K for Gd2TiAl3.

The stannide YbRhSn2 has been synthesized. An arc-melted Rh25Sn48 precursor sample was reacted with ytterbium in a sealed tantalum ampoule in an induction furnace. The structure of YbRhSn2 was refined from single-crystal X-ray diffractometer data: MgCuAl2 type, Cmcm, a = 433.10(3), b = 1076.63(8), c = 739.36(5) pm, wR2 = 0.0676, 444 F 2 values and 16 variables. The rhodium and tin atoms form a three-dimensional [RhSn2] δ− polyanionic network with short Rh–Sn (271–273 pm) and Sn–Sn (301–324 pm) distances. The tin substructure is an orthorhombically distorted lonsdaleite network. YbRhSn2 shows paramagnetic behavior with a reduced magnetic moment of 2.2(1) µB per ytterbium atom, classifying it as an intermediate-valent compound.

The stannides RE 3Rh2Sn4 (RE = Y, Gd–Tm, Lu) were synthesized from the elements by arc-melting and subsequent annealing (1220 K for RE = Y, Gd–Tm and 1170 K for RE = Lu) in sealed silica ampoules for 11 days. X-ray powder diffraction studies confirm the hexagonal Lu3Co2In4 type structure, space group P 6 ‾ $P\overline{6}$ . The structure of Gd3Rh2Sn4 was refined from single crystal X-ray diffractometer data for a twinned crystal: a = 744.04(6), c = 409.23(4) pm, wR2 = 0.0288, 567 F 2 values and 21 variables. The RE 3Rh2Sn4 stannides derive from the well-known equiatomic stannides RERhSn (≍RE 3Rh3Sn3) by Rh/Sn ordering within the RE 6 trigonal prisms. The striking structural motif is the trigonal planar tin coordination of the Sn2 atoms with 288 pm Sn2–Sn1 distances. The Sn2 atoms carry substantially more negative charge than the Sn1 atoms. This is underlined by 119Sn isomer shifts of δ = 1.86(1) mm s−1 for Sn1 and δ = 2.26(1) mm s−1 for Sn2 detected in the Mössbauer spectrum of Lu3Rh2Sn4. From atoms in molecules (AIM) analysis of the charge density obtained with calculation based on density functional theory (DFT) for Y3Rh2Sn4, the charge transfer proceeds from yttrium towards more electronegative rhodium. Little departure from neutrality is observed for tin whose itinerant s-like states are little involved with the bonding. The site projected density of states (DOS) and the crystal orbital overlap population (COOP) plots further illustrate these observations and reveal major Y–Rh and Rh–Sn bonding, while Y–Sn bonding is weaker.