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Room-temperature single-crystal X-ray studies carried out on trivalent rare earth sulfate hydrates, Ln2(SO4)3. x H2O, crystallized at local ambience suggest the following arrays to be prevalent. For Ln = La, the nonahydrate is found, hexagonal P 63/ m , with conventional R on | F | 0·023 for N o 1159 ‘observed’ ( I >3s( I )) diffractometer reflections (redetermination). Although for Ln = Ce a similar structure has been previously recorded, we have obtained that adduct as the monoclinic C 2/ c , Z = 4, octahydrate, a phase also found for Ln = Lu and diverse representative intermediate lanthanoids: a ˜ 13·6, b ˜ 6·6, c ˜ 18·2 Å, ß ˜ 102°; for Ln = Ce (redetermination), Dy, Yb (redetermination), Lu, R was 0·022, 0·035, 0·031, 0·024 for N o 3279, 2127, 3008, 3325 respectively. The structures of two lower hydrates adventitiously obtained are also recorded: the pentahydrate for Ln = Ce, monoclinic C 2/ c , a 15·741(3), b 9·632(3), c 10·358(3) Å, ß 119·72(2)°, Z = 4, R 0·030 for N o 3372 (a redetermination), and the trihydrate for Ln = Lu, orthorhombic Cmc 21, a 13·527(5), b 18·415(5), c 9·242(7) Å, Z = 8, R 0·040 for N o 1743. All structures are infinite polymeric arrays, the lanthanoid atoms being bridged by sulfate ions. Studies are also recorded for the ammonium/trivalent rare earth double sulfate tetrahydrate salts, (NH4)Ln(SO4)2.4H2O, for the (hitherto) extremal members Ln = La, Tb, which are isomorphous with the previously studied Ln = Sm monoclinic P 21/c, Z = 4 array, a ˜ 6·6, b ˜ 19, c ˜ 8·8 Å, ß 97°; R 0·035, 0·037 for N o 3631, 3337. The array is a two-dimensional polymer, parallel to the ac plane.
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Kepert et al. (1999) studied this question.
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