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1.
Incorporation of Al3+ in Ir3O12 Octahedra-Triple in Ba4Ir2AlO10 Single crystals of Ba4Ir2AlO10 were prepared by solid state/flux reactions. It crystallizes with orthorhombic symmetry: space group D–Cmca; a = 5.778; b = 13.352; c = 13.084 Å; Z = 4. The structure is characterized by face connection of three IrO6- or Ir/AlO6-octahedra. X-ray investigations show an ordered occupation of the centric octahedron by Ir and a statistically distribution of Ir and Al in the adjacent octahedra. Calculations of the coulomb term of the lattice energy support a charge distribution in the manner Ir5+/Al3+? Ir4+? Ir5+/Al3+.  相似文献   

2.
Synthesis and Structure of Ba10[Ti4N12], a Ternary Nitride with Tetranuclear Cyclic Nitridotitanate Ions Ba10[Ti4N12] results from the reaction of Ba3N2, TiN, and N2 at 980°C. It crystallizes in the triclinic space group P1 with the lattice parameters a = 644.3(4); b = 942.9(7); c = 966.9(7) pm, α = 106.37(4)°; β = 102.22(4)°; γ = 108.56(4)°, Z = 1. The crystal structure is built up by Ba2+ cations and tetranuclear cyclic nitridotitanate(IV) anions. In the anions four TiN4 tetrahedra are each connected by two corners to form centrosymmetrical rings, which are stacked along [100] forming tubes. The Ti? N distances range from 192 to 199 pm.  相似文献   

3.
About Ba6La2Co4O15 Ba6La2Co4O15 were prepared and investigated by X-ray single crystal work. It crystallizes with hexagonal symmetry, space group C–P63mc; a = 11.8082; c = 7.0019 Å; Z = 2. Ba2+ show face connected BaO6-octahedra and larger polyhedra of C.N. = 10 and 12. Co3+ is surrounded by four and six (tetrahedra, octahedra) oxygen. The Ba2+ and La3+ ions occupy one point position statistically.  相似文献   

4.
Ba5[CrN4]N: The First Nitridochromate(V) Ba5[CrN4]N is prepared by reaction of mixtures of Li3N, Ba3N2 and CrN/Cr2N (1 : 1) (molar ratio Li : Ba : Cr = 3 : 5 : 1) in tantalum crucibles at 700°C with flowing nitrogen (1 atm) within a period of 48 h. After cooling down to room temperature (60°C/h) black-shining single crystals of the ternary phase with a platy habit are obtained (monoclinic, C2/m; a = 1054.0(2) pm, b = 1170.9(3) pm, c = 937.7(2) pm, b? = 110,79(2)°; Z = 4). The crystal structure contains isolated complex anions [CrVN4]7? which nearly satisfy the ideal tetrahedral symmetry (Cr? N [pm]: 2 × 175.3(4), 2 × 175.8(5); N? Cr? N [°]: 106.8(2), 109.5(2), 2 × 109.9(2), 2 × 110,3(2)). The coordination sphere for each of the terminal nitride functions of the complex anions is completed by five neighbouring Ba2+ ions (distorted CrBa5 octahedra). The octahedra are connected via common CrBa2 faces as well as CrBa edges thereby forming condensed tetrameric octahedral groups. The isolated nitride ions which are also present in the crystal structure of Ba5[CrN4]N are in an octahedral environment of Ba2+ ions. The presence of a d1-System (Cr(V)) is confirmed by magnetic susceptibility data.  相似文献   

5.
About Ba4Ir3O10 Single crystals of Ba4Ir3O10 were prepared by a flux technique. X-ray investigations show monoclinic symmetry, space group C2h5–P21/a; a = 5.788; b = 13.222; c = 7.242 Å; β = 112.98°; Z = 2. Ir3O12 tripel, built up by face-sharing of IrO6 octahedra, are edge-connected into wave-like twodimensional planes. Ba4Ir3O10 is related to Ba4(Ti, Pt)3O10.  相似文献   

6.
Preparation and Crystal Structure of Nd4Ti9O24 The compound Nd4Ti9O24 was prepared by heating mixtures of Nd2O3/TiO2 (1 : 4.5) at temperatures of T = 1 330°C in air (2× 1d). Single crystals of Nd4Ti9O24 were obtained by chemical transport reaction (T2→T1; T1 = 1000°C, T1 = 900°C, 14 d) using chlorine (p(Cl2, 298 K) = 1 atm) as transport agent with Nd4Ti9O24 as starting material. Nd4Ti9O24 crystallizes in the orthorhombic space group Fddd (No. 70) with a = 13.9926(11) Å, b = 35.2844(21) Å, c = 14.4676(17) Å (Z = 16). The structure was refined to give R = 4.0% and R, = 3.7%. Main building units are TiO6 octahedra, NdO6 distorted square antiprisms and NdO6 octahedra.  相似文献   

7.
Ordered Occupation of Octahedra in Ba6La2Al1,5Fe2,5O15 Ba6La2Al1.5Fe2.5O15 was prepared and investigated by X-ray single crystal technique. It crystallizes in the space group C – P63mc; a = 11.814, c = 7.1003 Å; Z = 2. The M3+O6 octahedra are occupied exclusively by Fe3+ ions, the M3+O4 tetrahedra in contrast are statistically filled by Fe3+ and Al3+ ions. Ba6La2Al1.5Fe2.5O15 is a partially ordered mixed crystal of the pure iron and aluminium compounds.  相似文献   

8.
Synthesis and Crystal Structure of Ba6ZnIn2Cl20 Colourless single crystals of Ba6ZnIn2Cl20 are obtained from a 6 : 3 : 2 molar mixture of BaCl2, ZnCl2 and InCl3 at 420 °C in a Pyrex ampoule. It crystallizes with the monoclinic space group P21/c (Z = 4) with a = 1957.8(2), b = 1014.69(8), c = 1778.7(2) pm, β = 110.94(1)°, in a new structure. Zn2+ is surrounded tetrahedrally and In3+ octahedrally by chloride ions. Half of the [InCl6] octahedra are isolated from each other, the other half shares common edges to form [In2Cl10] double octahedra. Ba2+ has coordination numbers of eight and nine. There are chloride ions that do not belong to Zn2+ or In3+ so that the formula may be written as Ba12Cl10[ZnCl4]2[InCl6]2[In2Cl10].  相似文献   

9.
On the Synthesis and Crystal Structure of Ba6Lu4Zn10O22 with [OBa6] Octahedra Single crystals of Ba6Lu4Zn10O22 have been prepared by high temperature reactions and investigated by X-ray techniques. This compound is isotypic to Ba3In2Zn5O11 and the first member of the Rare Earth elements. Ba6Lu4Zn10O22 crystallizes with cubic symmetry, space group T-F4 3m, a = 13.452(1) Å and Z = 4. Zn2+ shows a tetrahedral, Lu3+ an octahedral and Ba2+ a three-fold capped trigonal prismatic coordination by O2?. The ZnO4 tetrahedra and LuO6 octahedra are forming macro polyhedra of the type Zn10O20 and Lu4O16. A discussion is given for the Ba6O33 and Ba6O42 groups.  相似文献   

10.
On an Oxide Chloride of CoIII: Sr8Co6O15Cl4 Sr8Co6O15Cl4 was prepared for the first time by flux reaction. It crystallizes with tetragonal symmetry: space group D4h17–I4/mmm; a = 3.927; c = 31.429 Å; Z = 1. Co3+ has different coordinations. One point position show CoO6 octahedra, the other one has a CoO5Cl surrounding. An oxygen deficit exhibit partly distorted square pyramids. Sr8Co6O15Cl4 is strongly related to Ba8In6O17.5 or can be seen as Sr4Co3O7.5Cl2 as a variety of the Sr4Ti3O10 type.  相似文献   

11.
Ba4Cu2Al3F21 is orthorhombic : a = 5.299(1) Å, b = 7.318(1) Å, c = 41.529(7) Å, Z = 4. The crystal structure was solved in the space group P212121 (no19) from X-ray single crystal data using 5682 unique reflections (3698 with FO/σ(F) > 4). It consists in a succession along c of 8 layers of 2 different types of sheets. The first layer, formulated [Cu2AlF11]4− in which copper-fluorine octahedra are linked by edges to form infinite distorted chains connected together by aluminium-fluorine octahedra, is followed by two [Al2F10]4− layers of infinite cischains of aluminium-fluorine octahedra linked by two vertices and another [Cu2AlF11]4− layer. These 4 layers are doubled along c by one of the screw-axes 21. The barium ions, 12-coordinated, are inserted between the sheets.  相似文献   

12.
SmAlF5 — a New Samarium(II) Fluoroaluminate with Al2F10 Bioctahedra and [AlF2/2F4/1] Chains . SmAlF5 has been obtained as orange-red transparent single crystals while heating mixtures of SmF3, Sm-powder and AlF3 (2:1:3) in a niobium crucible under Ar after 7?10 d at about 750°C. SmAlF5 crystallises in I 4/m (Nr. 87) with a=1 414.4(4), c=722.2(3) pm and Z=8 (CAD4, 4 340 IO, Rw=1.7%). The crystal structure of SmAlF5 is isotypic to BaTiF5. Characteristic building units are linear chains of trans-corner sharing AlF6 octahedra, which are connected via corners to two further AlF6 octahedra. Isolated Al2F10 octahedra lie disordered between such chains. The Sm atoms connect the AlF6 octahedra to a three-dimensional network. Measurements of the magnetic susceptibility show the temperature dependence typically found for Sm2+. The Madelung part of the lattice energy has been calculated and is discussed.  相似文献   

13.
Ba3V2O4F8 is prepared by hydrothermal synthesis. The crystal structure is established from single crystal X-ray diffraction data: Space group Pnnm, Z = 4, a = 9.945(4) Å, b = 10.277(1) Å and c = 9.673(1) Å R = 0.0331, Rw = 0.0315 for 892 independent reflections and 86 parameters. The structure is related to that Ba3Al2F12 and is described in terms of isolated [V4(O,F)20]8? tetrameric groups of octahedra inserted in a tridimensional network of (FBa4) tetrahedra. Location of oxygen and fluorine atoms is discussed with the help of bond valence calculations.  相似文献   

14.
A Partial Statistically Incorporation of Ca2+ into the Ba6Nd2Al4O15-Type: Ba5CaLa2Fe4O15 Using high temperature reactions we succeeded in incorporating Ca2+ into the Ba6Nd2Al4O15 type. Single crystal X-ray methods reveal a partly ordered alkaline earth distribution. Ba2+ and Ca2+ occupy face connected MO6-octahedra as well as a further point position together with La3+ ions (space group C−P63mc; a = 11.770; c = 7.039 Å; Z = 2).  相似文献   

15.
Preparation of the Free 12-Tungstoaluminium Acid H5[AlO4W12O36] · 6 H2O by Means of the Cryogenic Method The title compound was first prepared in solid state from its aqueous solution by means of the cryogenic method and characterized by chemical and thermal analyses, IR and UV spectroscopy. From X-ray heating patterns the formation of a new cubic phase 1/2 Al2O3 · 12 WO3 (I) at 400°C was found, being stable till 830°C: a = 378 pm (600°C). High-resolution 27Al NMR (MAS-technique) was used to determine the tetrahedral coordination of aluminium in the title compound and the octahedral coordination in I. The degradation of the doped WO3-phase I into Al2(WO4)3 begins at 600°C. Above 830°C tetragonal WO3 and Al2(WO4)3 coexist.  相似文献   

16.
A Contribution on Ba3Pt4HgO11: The First Alkaline-Earth Oxoplatinate(II,V)/Oxomercurate Single crystals of Ba3Pt4HgO11 were prepared by oxygen high pressure technique (4 200–3 600 bar) and investigated by X-ray methods. It crystallizes with hexagonal symmetry, space group D? P6 2c, a = 6.021, c = 17.374 Å, Z = 2. Ba3Pt4HgO11 represents a new structure type, showing structural relationships to Ba2Hg3Pd7O14 and to the precious metal 6L-perovskites. The Hg2+ ions show dumb-bell like coordination, Pt2+ a square-planar surrounding and Pt5+ face shared double octahedra.  相似文献   

17.
On Hexagonal Perovskites with Cationic Vacancies. XXVII. Systems Ba4?xSrxBIIRe2□O12, Ba4B CaxRe2□O12, and Ba4?xLaxBIIRe2?xWx□O12 with BII = Co, Ni In the systems Ba4?xSrxBIIRe2□O12, Ba4BCaxRe2□O12 and Ba4?xLaxBIIRe2?xWx□O12 (BII = Co, Ni) hexagonal perovskites with a rhombohedral 12 L structure (general composition A4BM2□O12; sequence (hhcc)3; space group R&3macr;m) are observed. With the exception of Ba4NiRe2□O12 the octahedral net consists of BO6 single octahedra and M2□O12 face connected blocks (type 1). In type 2 (Ba4NiRe2□O12) the M ions are located in the single octahedra and in the center of the groups of three face connected octahedra. The two outer positions of the latter are occupied by B ions and vacancies in the ratio 1:1. The difference between type 1 and 2 are discussed by means of the vibrational and diffuse reflectance spectra.  相似文献   

18.
Single phase cubic spinel of the composition Mn1.5Al1.5O4 is synthesized. Its crystal structure refinement shows that 0.4Mn+0.6Al are in the octahedral sites and 0.7Mn+0.3Al are in the tetrahedral sites. High temperature X-ray diffraction is used to analyze Mn1.5Al1.5O4 behavior during heating and cooling in air. In a temperature range of 600°C to 700°C, initial spinel splits into layers, and the sample represents a twophase system: cubic spinel Mn0.4Al2.4O4 and a phase based on β-Mn3O4. Above 900°C the sample again turns into single phase cubic spinel. The role of oxidizing processes in the decomposition of Mn1.5Al1.5O4 caused by oxygenation and partial oxidation of Mn2+ to Mn3+ is shown. A scheme of structural transformations of manganese aluminum spinel during heating from room temperature and cooling from 950°C is proposed.  相似文献   

19.
On Oxotitanates of the Alkaline Metals: On Na4Ti5O12 Colourless single crystals of the new titanate Na4Ti5O12 (starting from mixtures Na2O/TiO2, 1000°C, 6 d, Au-crucible, open system) crystallize in the monoclinic system, space group C2/m, a = 26.544(9), b = 2.952(1), c = 6.322(3) Å, β = 95.79(3)°, Z = 2, d = 3.45 and dpyk = 3.38 g · cm?3 (four-cycle-diffractometer data, PW 1100, 2?-scan, MoKα). R = 5.09% and Rw = 4.87% for 1178 independent I0(hkl) with 3° ≤ 2? ≤ 34°. Corrugated layers of Ti5O12, held together by Na+, are stacked along [001]. Details about partially occupied positions of Na+, Effective Coordination Numbers (ECoN), the Madelung part of lattice energy (MAPLE), and the structural differences to Na2Ti3O7 are discussed.  相似文献   

20.
On the Structure of Ba2Wo3F4 and Ba2MoO3F4 Ba2[WO2/2O2F2]F2 has been prepared for the first time as colourless single crystals (from powder, Au-tube, 680°C, 90 d). It crystallizes in the monoclinic (C c) crystal system with a = 1151.1, b = 938.2, c = 718.8 pm, ß = 126.17°, Z = 4. dx = 6.17, dpyk = 6.13 g · cm?3. (Fourcirclediffractometer PW 1100, Fa. Philips, MoKα-, ω-2Θ-scan, 1832 I0(hkl) R = 8.3, Rw = 7.4%). Parameters see in the text. The isotypic Ba2MoO3F4 has been prepared as powder (a = 1147.5, b = 937.0, c = 725.1 pm, ß = 126.42°). The structure shows chains of (WO2/2O2F2) groups along [001]. To establish O2? and F? on the positions IR and Raman Spectra are employed. The Madelung Part of Lattice Energy, MAPLE, is calculated and discussed.  相似文献   

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