Abstract

Compounds in the systems M 3+–O 2−–Cl −–Se 4+ are more than just quaternaries, for they can offer both oxygen that is bonded to selenium(IV) to form discrete [SeO 3] 2− ψ 1-tetrahedra ([SeO 3 E] 2− with E: non-bonding electron pair as pseudo-ligand) and oxygen that is only bonded to the trivalent lanthanoid (M = Ce–Lu) to form regular [OM 4] 10+ tetrahedra. The latter share edges and vertices in most cases to build up cationic chains ([OM 2] 4+ in Cl −-free Tb 2O[SeO 3] 2: a = 1064.57(7) pm, c = 521.56(4) pm, Z = 4, tetragonal, P4 2/ ncm), double strands ([O 2M 3] 5+ in Tb 3O 2Cl[SeO 3] 2: a = 535.16(4) pm, b = 1530.51(9) pm, c = 1081.72(7) pm, Z = 4, orthorhombic, Pnma; Er 3O 2Cl[SeO 3] 2: a = 1498.23(9) pm, b = 1102.04(7) pm, c = 547.95(4) pm, β = 105.515(6)°, Z = 4, monoclinic, C2/ c) or layers ([O 3M 4] 6+ in Yb 4O 3Cl 2[SeO 3] 2: a = 853.87(6) pm, b = 1145.92(8) pm, c = 1195.46(8) pm, α = 68.132(6)°, β = 78.113(6)°, γ = 85.748(6)°, Z = 2, triclinic, P 1 ¯ , [O 4M 5] 7+ in Tb 5O 4Cl 3[SeO 3] 2: a = 1229.13(8) pm, b = 546.17(4) pm, c = 978.79(6) pm, β = 90.485(6)°, Z = 2, monoclinic, C2/ m; [O 8M 9] 11+ in Gd 9O 8Cl 3[SeO 3] 4: a = 680.17(5) pm, b = 882.86(7) pm, c = 960.18(7) pm, α = 97.241(6)°, β = 95.539(6)°, γ = 96.265(6)°, Z = 1, triclinic, P 1 ¯ ; [O 3M 3] 3+ in CsEu 4O 3Cl 3[SeO 3] 2: a = 545.09(4) pm, b = 879.98(7) pm, c = 1597.45(9) pm, α = 81.036(6)°, β = 89.992(6)°, γ = 71.925(6)°, Z = 2, triclinic, P 1 ¯ ). On the other hand and much like in the pure lanthanoid(III) oxoselenates(IV) M 2[SeO 3] 3 themselves, segregation of the stereochemically active non-bonding electron pairs (one per Se 4+ cation) of the pyramidal [SeO 3] 2− units occurs, such that “lone-pair” channel or layer structures emerge. Sometimes even the “lone-pair” electrons of the chloride anions help to construct these structural features as also observed in the O 2−-free chloride oxoselenates(IV) MCl[SeO 3].

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