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1.
Powder material of ?‐Fe2O3 was obtained by thermal decomposition of the clay mineral nontronite and subsequent isolation of the ferric oxide by leaching the silicate phases. Additionally, crystals of ?‐Fe2O3 were grown as precipitates by internal oxidation of a Pd96Fe4 alloy. Analysis of the precipitate crystals by electron diffraction yields an orthorhombic crystal system and space group Pna21 ab initio. X‐ray diffraction data of the powder containing small amounts of Al substituting Fe were refined by the Rietveld method. The refinement yields lattice parameters a = 507.15 pm, b = 873.59 pm and c = 941.78 pm, and atom positions. ?‐Fe2O3 is isostructural with κ‐Al2O3, AlFeO3, and GaFeO3 having an anion stacking sequence /ABAC/, and 1/4 of the cations in tetrahedral co‐ordination. Some strongly distorted FeO6 octahedrons with one large Fe‐O distance, which may be considered as a 5+1 co‐ordination, appear to be characteristic for ?‐Fe2O3. The structure shows elements known from silicates and oxyhydroxides of iron, respectively.  相似文献   

2.
BaB2S4: The first non‐oxidic Chalcogenoborate with Boron in a trigonal‐planar and tetrahedral Coordination Hitherto we know boron in a trigonal‐planar and a tetrahedral coordination within one crystal structure from boron oxides in various compounds. With the novel bariummetathioborate BaB2S4 we now report a crystal structure containing BS3 and BS4 units in the ratio 1 : 1 forming infinite chains along [001]. BaB2S4 was synthesized in a solid state reaction at a temperature of 800 °C from barium sulfide, amorphous boron and sulfur and crystallizes in the monoclinic space group Cc (no. 9) with the following lattice parameters: a = 6.6465(5) Å, b = 15.699(1) Å, c = 6.0306(5) Å, β = 110.96(1)°, Z = 4.  相似文献   

3.
The First Compound of BaMLn2O5-Type Containing Mn2+: BaMnDy2O5 Single crystals of the hitherto unknown compound BaMnDy2O5 were prepared by CO2-Laser technique and H2 atmosphere. Four circle diffractometer measurements led to space group D162h-Pnma, a = 12.428; b = 5.766; c = 7.143 Å; Z = 4. It is isotypic to BaCuSm2O5 and shows Mn2+ in square pyramids of oxygen.  相似文献   

4.
5.
The structure of completely exchanged Mn2+—ß″—Al2O3(Mn0.77Al10.46Mg0.54O17) crystals has been investigated by single—crystal X—ray diffraction methods at room temperature (trigonal, R3¯, Z = 3, a = 560.65(7), c = 3329.3(9) pm). The manganese ions (Mn2+) are found to occupy Beevers‐Ross (56 %) and mid—oxygen positions (44 %) in nearly the same amounts. The crystal composition was confirmed by electron probe microanalyses on various crystals.  相似文献   

6.
The Mixed‐Valent Oxoferrate(II,III) K3[Fe2O4] – A Stuffed Variant of the K2[Fe2O4] Type of Structure K3[Fe2O4] has been obtained by tempering “Cs3K3CdO4” in sealed Fe containers (36 d at 450–480 °C) as dark red transparent single crystals of rectangular shape. The structure determination (IPDS diffractometer data, MoKα, 1891 collected reflections, 234 symmetry independent, R1 = 0.033, wR2 = 0.088) confirms the space group Fddd; a = 596.11(9), b = 1140.3(1), c = 1717.9(3) pm; Z = 8. K3[Fe2O4] exhibits a structure with [FeO4] tetrahedra connected via corners leading to a three‐dimensional network closely related to the KFeO2 type of structure. From the oxidation at 520 °C of iron metal with KO2 in the presence of Na2O black single crystal of K2[Fe2O4] have been obtained. K2[Fe2O4] crystallizes in the space group Pbca with Z = 8 and a = 559.18(7), b = 1122.1(1), c = 1592.8(2) pm (IPDS diffractometer data, MoKα, collected refelctions: 9543, 1213 symmetry independent, R1 = 0.043, wR2 = 0.102).  相似文献   

7.
Synthesis and Crystal Structure of Na10[M3O6][MO3] (M = Fe, Mn) with a Remark on the Magnetic Properties Single crystals of Na10[M3O6][MO3] (M = Mn, Fe) may be obtained via a redox reaction of CdO with the respective transition metal in the presence of Na2O and a flux as red single crystals, which are sensitive to moisture. The crystal structure (determined from IPDS data, , Z = 6) contains isolated trigonal aplanar [MO3] units and layers of [MO4] tetrahedra connected via corners to three‐membered rings, which share common edges resulting in the formation of twelve‐membered rings. The statistical occupancy of 21 out of 60 sodium atoms per unit cell is discussed and calculations of the Madelung Part of the Lattice Energy (MAPLE) are given. Furthermore, we report on the magnetic properties of Na10[Mn3O6][MnO3] in close relation to the structural entities.  相似文献   

8.
Crystal Structure of the Diacetone Alcohol Complex [Mn(DAA)3]2+[MnI4]2– · DAA The title compound has been prepared from MnI2 and excess diacetone alcohol (4‐hydroxy‐4‐methyl‐2‐pentanon) to give brown single crystals which were suitable for a crystal structure determination. Space group P21/c, Z = 4, lattice dimensions at 157 K: a = 1158.3(1), b = 1806.0(1), c = 1846.5(2) pm, β = 97.421(8)°, R1 = 0.0381. The structure consists of [Mn(DAA)3]2+ ions with distorted octahedral environment of the manganese atom, tetrahedral [MnI4]2– ions and a diacetone alcohol molecule which is connected by two hydrogen bridges with the complex cation.  相似文献   

9.
A Sodium Oxocobaltate(II) Sulfate: Na8[CoO3][SO4]2 Na8[CoO3][SO4]2 has been obtained from a redox reaction between cobalt metal and CdO in the presence of Na2SO4 and Na2O at 550 °C (15 d) as red single crystals. The structure has been determined from single crystal data (IPDS‐data, T = 170 K, Cmcm, Z = 4, a = 806.88(9) pm, b = 2232.1(3) pm, c = 705.97(9) pm, Rall = 0.047). Magnetic properties and spectroscopic investigations are reported and discussed within the Angular‐Overlap‐Model.  相似文献   

10.
Temperature-dependent crystallographic and magnetic studies on stoichiometric single crystals of LiCu2O2 are reported. The temperature dependence of the lattice parameters was extracted from X-ray powder diffractograms collected on crushed single crystals, from 12 K to 295 K. The magnetic properties are similar to earlier findings demonstrating antiferromagnetic ordering below 25 K. Evidence of magnetoelastic coupling is observed in the thermal expansion along the c-direction; not only at the low temperature antiferromagnetic transitions, but an anomalous behavior of the thermal expansion indicate magnetoelastic coupling also to the magnetic ordering related to a weak spontaneous magnetic moment appearing at 150 K. Ac-susceptibility measurements at different frequencies and superposed dc-fields are employed to further characterize this magnetic anomaly.  相似文献   

11.
Nd(S2O7)(HSO4): The First Disulfate of a Rare Earth Element Light violett single crystals of Nd(S2O7)(HSO4) have been obtained by the reaction of Nd2O3 and oleum (30% SO3) at 200 °C in sealed glass ampoules. The crystal structure (monoclinic, P21/n, Z = 4, a = 857.8(1), b = 1061.0(2), c = 972.4(1) pm, β = 99.33(2)°) contains Nd3+ in eightfold coordination of oxygen atoms which belong to three HSO4 ions and four S2O72– groups. One of the latter acts as bidentate ligand. Hydrogen bonding is observed between the H atom of the HSO4 ion and the non‐coordinating O atom of the S2O72– group.  相似文献   

12.
A Fluoride Phosphate of Manganese(III) with Unusual Layer Structure: Na7[Mn5F13(PO4)3(H2O)3] The title compound was crystallized from a solution of MnF3 · 3 H2O in aqueous HF by addition of NaH2PO4 · H2O in 2 M phosphoric acid. The crystal structure has been determined at 295 and 150 K on a trigonal crystal twinned by merohedry: Space group P3c1, Z = 4, a = 1055,0(1), c = 2314,0(1) pm (a = 1052,5(1), c = 2304,2(1) pm at 150 K), wR2 = 0.0651 (0.0651). The structure contains anionic layers formed by triangular moieties of three [MnF3O2(H2O)] octahedra sharing one common μ3-F atom and bridged by three phosphate groups. Three of those groups, respectively, are interconnected by two [MnF3O3] octahedra over six phosphate O-atoms to form a trigonal layer in the a,b plane. Stacking of these layers gives channels along the c axis in which most of the Na+ ions are located. The [MnF3O2(H2O)] octahedra show strong elongation along the μ3-F–Mn–OH2 axis mainly due to the Jahn-Teller effect whereas in the [MnF3O3] octahedra with C3 symmetry weak signs only of a dynamical Jahn-Teller-effect can be observed. The magnetic properties (μeff = 4.61 μB, 3-D ordering point TN = 3.3 K) were determined on powders and possible magnetic exchange pathways are discussed.  相似文献   

13.
CsMn2P2, a Manganese(II, III) Phosphide with BaZn2P2 Structure. With a Contribution to the BaAl4 Structure Type CsMn2P22is formed by the reaction of Cs4P6 with Mn and red phosphorus (Nb ampoule; 1073 K) as black platelets. The compound is paramagnetic following the Curie‐Weiss law above 110 K (μ = 4.81 B.M. / CsMn2P2; θ = —79 K) and orders antiferromagnetically below 110 K. The magnetic moment corresponds with the ratio MnII : MnIII = 1:1. CsMn2P2 is isotypic with BaZn2P2 (tI10; I4/mmm; a = 4.098(1) Å, c = 14.215(4) Å, d(Mn—P) = 2.387(1) Å (4×), d(Cs—P) = 3.718(2) Å (8×)), and shows, therefore, no P—P‐bonds. The different regions of the BaAl4 (ThCr2Si2) structure type are analysed and parameterized once more.  相似文献   

14.
The mixed‐valent oxotantalate Eu1.83Ta15O32 was prepared from a compressed mixture of Ta2O5 and the metals in a sealed Ta ampoule at 1400 °C. The crystal structure was determined by means of single crystal X‐ray diffraction: space group R3¯, a = 777.2(6) pm and c = 3523.5(3) pm, Z = 3, 984 symmetrically independent reflections, 83 variables, RF = 0.027 for I > 2σ (I). The structure is isotypic to Ba2Nb15O32. The salient feature is a [Ta(+8/3)6O12iO6a] cluster consisting of an octahedral Ta6 core bonded to 12 edge‐bridging inner and six outer oxygen atoms. The clusters are arranged to slabs which are sandwiched by layers of [Ta(+5)3O13] triple octahedra. Additional Ta(+5) and Eu(+2) atoms provide the cohesion of these structural units. Twelve‐fold coordinated Eu(+2) atoms are situated on a triply degenerate position 33 pm displaced from the threefold axis of symmetry. A depletion of the Eu(+2) site from 6 to 5.5 atoms per unit cell reduces the number of electrons available for Ta‐Ta bonding from 15 to 14.67 electrons per cluster. Between 125 and 320 K Eu1.83Ta15O32 is semi‐conducting with a band gap of 0.23 eV. The course of the magnetization is consistently described with the Brillouin function in terms of a Mmol/(NAμB) versus B/T plot in the temperature range 5 K — 320 K and at magnetic flux densities 0.1 T — 5 T. At moderate flux densities (< 1 T) the magnetic moment agrees fairly well with the expected value of 7.94 μB for free Eu (2+) ions with 4f7 configuration in 8S7/2 ground state. Below 5 K, anisotropic magnetization measurements at flux densities B < 1 T point to an onset of an antiferromagnetic ordering of Eu spins within the layers and an incipient ferromagnetic ordering perpendicular to the layers.  相似文献   

15.
Colorless platelets of Na2Lu3I3[TeO3]4 were obtained within five days at 775 °C by the reaction of Lu2O3 and TeO2 in a 3:8 molar ratio with NaI added in excess as both fluxing agent and reactant in evacuated silica ampoules. It crystallizes in the monoclinic space group P2/c with the lattice parameters a = 921.69(5), b = 552.71(3), c = 1664.37(9) pm, β = 90.218(4)° and Z = 2. The crystal structure of Na2Lu3I3[TeO3]4 exhibits two crystallographically different Lu3+ cations, both coordinated by eight O2– anions as square antiprisms. These polyhedra are interconnected through four common edges to build up {}^2_∞ {[LuO{}^e_8/2 ]5–} layers (e = edge‐linking) parallel to (100). Furthermore, the crystal structure includes a crystallographically unique Na+ cation surrounded by four O2– and four I anions also in the shape of a square antiprism. These polyhedra connect via common (I2)···(I2) edges in generating {}^1_∞ {[Na2O8I{}^e_4 ]18–} double‐strands that are further linked by (I1) vertices to result in the formation of {}^2_∞ {[Na2O8I3{}^e,v_3 ]17–} layers (v = vertex‐linking) spreading out parallel to (100) as well. Thus, the crystal structure contains two crystallographically distinct I anions, of which (I1) is coordinated nearly linear (? (Na–I1–Na) = 179.6°) by two Na+ cations, whereas (I2) has contact to three of them displaying a distance of 114 pm from the triangular (Na+)3 plane. The crystal structure of Na2Lu3I3[TeO3]4 is completed by two crystallographically independent Te4+ cations that show stereochemically active non‐bonding electron pairs (“lone pairs”) and are located above and below the {}^2_∞ {[LuO{}^e_8/2 ]5–} layers forming isolated ψ1‐tetrahedral [TeO3]2– anions (d(Te–O) = 188–190 pm) with all oxygen atoms.  相似文献   

16.
Dy3OF5S: The First Oxyfluoride Sulfide of the Lanthanides While trying to synthesize DyFS with the PbFCl‐type crystal structure by the reaction of DyF3 with dysprosium and sulfur in 1:2:3‐molar ratios at 850 °C in gas‐tight sealed tantalum ampoules, oxygen contaminated educts (e.g. DyOF‐containing DyF3) were also applied occasionally. Consequently a small quantity of almost colourless, rod‐shaped single crystals of Dy3OF5S, the first oxyfluoride sulfide of the lanthanides, were formed in small quantities on adding equimolar amounts of NaCl as flux. Almost phase‐pure samples are obtained under otherwise analogous reaction conditions according to 2 Dy + 5 DyF3 + Dy2O3 + 3 S = 3 Dy3OF5S by deliberate addition of Dy2O3. In the hexagonal crystal structure (space group: P63/m; a = 942.58(8), c = 368.12(4) pm; c/a = 0.391, Vm = 85.285 cm3/mol, Z = 2) Dy3+ resides in nine‐fold anionic coordination (tricapped trigonal prism comprising 1.333 O2—, 5.667 F and 2 S2—). The fractional numerical values for the “light anions” are due to two six‐fold point positions with the exclusive existence of F in trigonal non‐planar coordination (CN = 3, d(F1—Dy) = 232 (1×) and 241 pm, 2×) on the one hand, but F and O2— simultaneously in the ratio 2 : 1 in tetrahedral coordination of Dy3+ (CN = 4, d(F2/O—Dy) = 234 (2×), 236 and 241 pm, 1× each) on the other. Finally, a trigonal prismatic Dy3+ coordination (d(S—Dy) = 290 pm, 6×) is attributed to the S2— anions. From the data of the single crystal X‐ray structure analysis, no indication of an ordering of O2— and F is obtained, its true nature as an oxyfluoride sulfide, however, is unambiguously confirmed by electron‐beam microanalysis on Dy3OF5S.  相似文献   

17.
Contributions on the Bonding Behaviour of Oxygen in Inorganic Solids. III [1] Mn2P2O7, Mn2P4O12 und Mn2Si(P2O7)2 — Crystal Growth, Structure Refinements and Electronic Spectra of Manganese(II) Phosphates By chemical vapour transport reactions in a temperature gradient single crystals of Mn2P2O7 (1050 → 950 °C) and Mn2P4O12 (850 → 750 °C) have been obtained using P/I mixtures as transport agent. Mn2Si(P2O7)2 was crystallized by isothermal heating (850 °C, 8d; NH4Cl as mineralizer) of Mn2P4O12 und SiO2. In Mn2Si(P2O7)2 [C 2/c, a = 17.072(1)Å, b = 5.0450(4)Å, c = 12.3880(9)Å, β = 103.55(9)°, 1052 independent reflections, 97 variables, R1 = 0.023, wR2 = 0.061] the Mn2+ ions show compressed octahedral coordination (d¯Mn—O = 2.19Å). The mean distance d¯Mn—O = 2.18Å was found for the radially distorted octahedra [MnO6] in Mn2P4O12 [C 2/c, Z = 4, a = 12.065(1)Å, b = 8.468(1)Å, c = 10.170(1)Å, β = 119.29(1)°, 2811 independent reflections, 85 variables, R1 = 0.025, wR2 = 0.072]. Powder reflectance spectra of the three pink coloured manganese(II) phosphates have been measured. The spectra show clearly the influence of the low‐symmetry ligand fields around Mn2+. Observed d—d electronic transition energies and the results of calculations within the framework of the angular overlap model (AOM) are in good agreement. Bonding parameters for the manganese‐oxygen interaction in [Mn2+O6] chromophors as obtained from the AOM treatment (B, C, Trees correction α, eσ, eπ) are discussed.  相似文献   

18.
Structural and Magnetochemical Studies at the Ternary Phosphates Ba2MII(PO4)2 (MII = Mn, Co) and Refinement of the Crystal Structure of BaNi2(PO4)2 Single crystals of the following phosphates were grown by the floating zone technique using a mirror furnace and their crystal structures refined (0,02 < R1 < 0,04 and 0,04 < wR2 < 0,10, resp.): Ba2Mn(PO4)2 (a = 531.1(1), b = 896.8(1), c = 1625.6(3) pm, β = 90.26(1)°), Ba2Co(PO4)2 (a = 529.8(1), b = 884.4(1), c = 1614.4(3) pm, β = 90.68(2)°) and BaNi2(PO4)2 (a = 480.0(1), c = 2327.3(5) pm, Z = 3, space group R3). Both compounds Ba2MII(PO4)2 crystallize with Z = 4 in space group P21/n of the monoclinic Ba2Ni(PO4)2 type; BaNi2(PO4)2 has the hexagonal‐rhombohedral structure of the BaNi2(AsO4)2 type. Magnetic measurements of powders of Ba2Mn(PO4)2 and Ba2Co(PO4)2 yielded room temperature moments of μeff = 5,73 and 4,93 μB, resp., but only the manganese compound obeys the Curie‐Weiss law down to low temperatures. Weak antiferromagnetic interactions at both compounds only near TM ≈ 5 K lead to a reciprocal susceptibility minimum.  相似文献   

19.
Using hydrothermal methods, two manganese arsenates have been synthesized and characterized by single crystal X‐ray diffraction. The products Mn5(AsO4)2(HAsO4)2 ?4H2O ( 1 ) and Mn2AsO4(OH) ( 2 ), the Mn end‐members of the minerals villyaellenite and sarkinite, respectively, have been obtained (crystal data 1 : monoclinic, C2/c, a = 18.109(4), b = 9.332(2), c = 9.809(2) Å, β = 96.172(4)?, Z = 4; 2 : monoclinic, P21/c, a = 10.219(2), b = 13.613(2), c = 12.780(2) Å, β = 108.834(2)?, Z = 16). In both compounds a three‐dimensional framework of edge‐sharing MnO polyhedra is observed. Based on the availability of the all Mn2containing form of villyaellenite ( 1 ), the ordering scheme of the impurity cations of the natural samples could be confirmed. Magnetic susceptibility measurements of 1 indicate the presence of high‐spin Mn2+ ions. The comparison of the data on sarkinite ( 2 ) with the data obtained from the natural sample indicates that the mineral has either a very high Mn content, or an absence of impurity cation ordering.  相似文献   

20.
Two new two‐dimensional CuII and MnII coordination polymers of 5‐aminobenzene‐1,3‐dicarboxylic acid (abdc) ligand, [Cu(μ4‐abdc)(DMF)]n and {[Mn(μ4‐abdc)(H2O)]·H2O}n, have been synthesized and characterized by elemental analysis and IR‐ spectroscopy. The single crystal X‐ray analyses show that the coordination number in these complexes is six, CuO5Cu and MnO5N. The compounds are structurally diverse and the coordination polymer obtained from copper show significant copper–copper interaction while the manganese coordination polymer shows Mn–Namino bond.  相似文献   

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