The stannides CaErPt3Sn5 CaTmPt3Sn5, CaYbPt3Sn5, and CaLuPt3Sn5 were prepar
ed from the elements in glassy carbon crucibles under an argon atmosphere i
n a high-frequency furnace. Their Yb2Pt3Sn5 type structure (space group Pnm
a) was refined from single-crystal X-ray data: a = 736.4(1) pm, b = 444.11(
9) pm, c = 2639.9(4) pm, wR = 0.0905, 1403 F-2 values, 63 variables for the
erbium; a = 733.9(2) pm, b = 443.0(1) pm, 2634.8(5) pm, wR2 = 0.1430, 1372
F-2 values, 63 variables for the thulium; a = 733.9(1)pm, b = 443.3(1)pm,
2635.7(6) pm, wR2 = 0.0734, 2079 F-2 values, 64 variables for the ytterbium
; and a = 735.0(2)pm, b = 441.6(2)pm, 2634.1(7) pm, wR2 = 0.1202, 1344 F-2
values, 63 variables for the lutetium compound, The Yb2Pt3Sn5 structure is
built up from a complex threedimensional [Pt3Sn5] polyanion in which the yt
terbium atoms fill distorted hexagonal channels. The two crystallographical
ly different ytterbium sites have coordination numbers (CN) 20 and 18, resp
ectively. In the erbium, thulium, and lutetium compound, the CN 20 position
is occupied exclusively by calcium atoms, while a mixed calcium-rare-earth
occupancy is observed for the CN 18 position. In tbe ytterbium compound bo
th positions show mixed occupancy. The refinements resulted in the composit
ions Ca1.33Er0.67Pt3Sn5, Ca1.45Tm0.55Pt3Sn5, Ca1.28Yb0.72Pt3Sn5, and Ca1.63
Lu0.37Pt3Sn5 for the crystals investigated. These results were confirmed by
magnetic susceptibility measurements. The erbium and the thulium compound
show Curie-Weiss behavior with experimental effective magnetic moments of 9
.5(2) and 8.4(2) mu(B), respectively. At 4.8(1) K, the erbium compound orde
rs ferro- or ferrimagnetically, while antiferromagnetic ordering at T-N = 5
.0(1) K is observed for the thulium compound. CaYbPt3Sn5 shows Curie-Weiss
behavior above 100 K with an experimental magnetic moment of 2.8(2) mu(B) a
nd Theta = -71(5) K, indicating mixed-valent behavior. CaLuPt3Sn5 shows a d
iamagnetic signal of -7.8 x 10(-9) m(3)/mol. (C) 2000 Academic Press.