Nanoporous mixed-framework silicates are of particular interest because they show promising physico-chemical properties similar to zeolites. In the course of an ongoing project on new micro- and nanoporous M3+ silicates new di-, tri-and tetrasilicate compounds were synthesised. All syntheses were carried out using the flux-growth technique (MoO3–based flux mixtures in Pt crucibles in air; Tmax = 1150°C, cooling rate 2°C/h, Tmin = 900°C). The crystal structures of all compounds have been determined from single-crystal X-ray intensity data (Mo Kα X-radiation, CCD area detector, 293 K).
The three isotypic compounds BaKYSi2O7 (Kolitsch et al., 2007), BaKYbSi2O7 and BaKScSi2O7 crystallise as small colourless isometric crystals in space group P21/n. BaKREESi2O7 (REE = Y, Yb, Sc) represents a novel tetrahedral-octahedral framework structure type. The structure is based on isolated Si2O7 groups with octahedrally coordinated REE3+ cations and [9]-coordinated Ba atoms and [8]-coordinated K atoms. The isolated REEO6 octahedra share each of their apices with oxygen atoms of the Si2O7 groups. The connectivity results in a three-dimensional framework with Ba2+ and K1+ cations in channels running parallel to [10-1]. By comparison to other disilicates, the Si-O-Si angle in BaKREESi2O7 is unusually small (124.51(9), 124.9(2) and 128.2(1)°, respectively). No isoelectronic or other related silicates are known, although the monoclinic diphosphates M2SrP2O7 (M = K, Rb, Cs) (Trunov et al., 1991) have similar crystal structures.
A new dimorph of BaKYbSi2O7 crystallised together with P21/n-type BaKYbSi2O7 (see above); it is also monoclinic (space group Cc). Its crystal structure is closely related to the BaKREESi2O7 (REE = Y, Yb, Sc) type; the Si-O-Si angle is alsosimilar, 126.0(7)°.
The third new structure type based on disilicate groups is represented by BaNaScSi2O7 (Wierzbicka et al., 2007). It is also topologically similar to BaKREESi2O7. BaNaScSi2O7 crystallises as small colourless isometric crystals in P21/m. Its structure consists of ScO6 octahedra that share each of their apices with O atoms of the Si2O7 groups and [9]-coordinated Ba atoms and [4+4]-coordinated Na atoms (Na-O = 2.457 – 2.907 Å). The Si-O-Si angle in BaNaScSi2O7, 123.12(12)°, is the smallest of all the mentioned new disilicates. The three above structure types differ in localisation of Ba2+, K1+, and Na1+ atoms and direction of the linkages between REEO6 (REE = Y, Yb, Sc) and Si2O7 units.
In the trisilicate family, a large number of new compounds was obtained: BaREE2Si3O10 (REE = Gd, Y, Er, Yb, Sc) (Kolitsch et al., 2006), SrY2Si3O10 (Kolitsch et al., 2006) and BaRbScSi3O9 (Wierzbicka et al., 2007). All compounds formed small, colourless plates, with monoclinic or triclinic symmetry. BaREE2Si3O10 crystallises in P21/m. Its crystal structure is based on zigzag chains parallel to [010] of edge-sharing distorted REEO6-octahedra linked by horseshoe-shaped Si3O10 groups and [8]-coordinated Ba atoms, which occupy narrow channels extending parallel to [100]. The Si-Si-Si angle in Si3O10 units increase with decreasing REE3+ ionic radii (94.78(5), 96.12(4), 96.40(5), 97.09(5), 99.63(4)° for REE = Gd, Y, Er, Yb, Sc, respectively). The second trisilicate compound, SrY2Si3O10, crystallises in P-1 (no. 2). The structure of SrY2Si3O10 contains zigzag chains parallel to [100] of edge-sharing YO7 polyhedra sharing further edges with YO6 polyhedra. These decorated chains are linked by slightly curved Si3O10 groups (Si-Si-Si angle = 133.5°). It is noteworthy that one SiO4 tetrahedron shares an edge with the YO7 polyhedron. Voids in the resulting framework are occupied by Sr2+ cations in [8]-coordination (Kolitsch et al., 2006). BaRbScSi3O9 crystallises as small pseudohexagonal plates (drillings) in P1/c. The topology of BaRbScSi3O9 is based on Si3O9 rings connected to the isolated ScO6 octahedra. The [6-7]-coordinated Ba and approximately [7-8]-coordinated Rb atoms are both arranged along rows parallel to [010].
The single new tetrasilicate obtained, Ba2Gd2Si4O13, crystallises as colourless pseudotetragonal prisms in C2/c. The structure consists of finite Si4O13 chains connected with GdO7 polyhedra. Two such polyhedra share a common edge creating isolated Gd2O12 groups, which form the basis of a heteropolyhedral slab in the ab plane. [8]-coordinated Ba atoms are located in channels running parallel to the b-axis. This compound shows structural similarities to Na4Sc2Si4O13 (Maksimov et al., 1980) and Ba2Nd2Si4O13 (Tamazyan et al., 1985).
Financial support by the Austrian Science Foundation (FWF) (Grant P17623-N10) and the ICDD (Grant 90-03ET) is gratefully acknowledged.
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