AbstractEighteen new rare earth-rich intermetallic phasesRE10TCd3(RE=Y, Tb, Dy, Ho, Er, Tm, Lu;T=Rh, Pd, Ir, Pt) were obtained by induction melting of the elements in sealed niobium ampoules followed by annealing in muffle furnaces. All samples were characterized by X-ray powder diffraction. The structures of four representatives were refined from single-crystal X-ray diffractometer data: ordered Co2Al5type,P63/mmc,a=951.2(1),c=962.9(2) pm,wR=0.0460, 595F2values, 20 parameters for Er10RhCd3;a=945.17(4),c=943.33(4),wR=0.0395, 582F2values, 21 parameters for Lu9.89PdCd3.11;a=964.16(6),c=974.93(6) pm,wR=0.0463, 614F2values, 21 parameters for Y10Ir1.09Cd2.91;a=955.33(3),c=974.56(3) pm,wR=0.0508, 607F2values, 22 refined parameters for Dy9.92IrCd3.08. Refinements of the occupancy parameters revealed small homogeneity ranges resulting fromRE/Cd, respectivelyT/Cd mixing. The basic building units of theRE10TCd3phases are transition metal-centeredRE6trigonal prisms (TP) that are condensed with double-pairs of emptyRE6octahedra via common triangular faces. A second type of rods is formed by slightly distortedRE3@Cd6RE6icosahedra which are condensed via Cd3triangular faces. The shortest interatomic distances occur forRE–T, compatible with strong covalent bonding interactions. Temperature dependent magnetic susceptibility measurements were performed forRE10RhCd3(RE=Dy–Tm, Lu),RE10IrCd3(RE=Er, Tm, Lu) andRE10PtCd3(RE=Y, Lu). While Y10PtCd3and Lu10TCd3(T=Rh, Ir, Pt) show Pauli paramagnetic behavior, the compounds containing paramagnetic rare earth elements show Curie-Weiss behavior (the experimental magnetic moments indicate stable trivalentRE3+) and magnetic ordering at low temperatures:TC=80.5 K for Dy10RhCd3and Neél temperatures of 42.1, 23.3, 12.6, 5.9, 10.0 K for Ho10RhCd3, Er10RhCd3, Er10IrCd3, Tm10RhCd3, Tm10IrCd3, respectively.