Fe4Si2Sn7O16: Eine Kombination von FeSn6-Oktaedern mit Schichten von (Fe3Sn)O6-Oktaedern; Präparation,Eigenschaften und Kristallstruktur [1]

Fe₄Si₂Sn₇O₁₆: A Combination of FeSn₆-Octahedra with Layers of (Fe₃Sn)O₆-Octahedra; Preparation, Properties, and Crystal Structure Fe₄Si₂Sn₇O₁₆ has been prepared by a solid state reaction at 900 °C from a mixture of Fe₂O₃, SnO₂, Sn, and Si. The compound is a paramagnetic semiconductor. Results of Mössbauer and suszeptibility measurements as well as bond length-bond strength calculations lead to the possible ionic formulation Fe₄²⁺Si₂⁴⁺Sn₁²⁺Sn₁⁴⁺O₁₆^2–. The compound crystallizes in the trigonal space group P3m1 (no. 164), with one formula unit per cell. Lattice parameters obtained by powder measurements are: a = 6.8243(6) Å, c = 9.1404(6) Å, γ = 120°, V = 368.6(1) ų. The structure consists of layers of edge linked oxygen octehedra exactly centered by Sn and Fe in the ratio 1 : 3. Three plains of isolated SiO₄ tetrahedra, FeSn₆ octahedra and again SiO₄ terahedra are inserted between two such layers. The layers are stacked along [001] and linked three-dimensionally by oxygen.     

IR-spektroskopische Untersuchungen der Phasengleichgewichte im System Ru/Sn/O

Infrared Spectroscopic Investigations on Phase Equilibria in the System Ru/Sn/O Infrared spectroscopic investigations give evidence for the existence of new phases and their phase relations in the system Ru/Sn/O. The obtained results coincide well with X-ray diffraction investigation. The composition of two phases was found to correspond to the formula: RuSn₃O₄ and RuSn₅O₄. Evidence is given for the existence of a third phase, the composition should correspond to RuSn₉O₈.     

Iron-modified mesoporous SBA-15 silica: Preparation and characterization studies

Fe-SBA-15 materials with different Si/Fe ratios (Si/Fe = 100, 60, 15) have been synthesized by hydrothermal method and characterized by several spectroscopic techniques. Electron spin resonance and Mössbauer spectroscopy, along with electron microscopy and X-ray diffraction, allowed differentiation of several iron species. These species correspond to hematite particles, very small “isolated” or oligomeric Fe^III species possibly incorporated in the mesoporous silica wall, and Fe^III oxide clusters either isolated or agglomerated, forming “rafts” at the surface of the silica and exhibiting ferromagnetic ordering. Because of their agglomeration, these clusters appear with a two-peak size distribution, with one peak corresponding to the isolated clusters formed in the mesopores and still embedded in them and the other corresponding to the agglomerates spread on the surface of the mesoporous silica particles.     

An in‐situ Mössbauer Study of the Formation of Cementite,Fe3C

The formation of cementite, Fe₃C, from thin iron foils has been studied at 550 and 650 °C by means of in‐situ Mössbauer spectroscopy. At 550 °C, the kinetics of the reaction have been determined from time‐resolved experiments performed at different carbon activities. The product formation follows a two‐step process exhibiting two different kinetic regimes. The slow initial stages of the reaction as well as its rapid final part can be described by an Avrami‐type kinetics with a characteristic parameter of n = 3/2.     

Darstellung,Eigenschaften und Molekülstrukturen von Alkylaluminiumaminoalkoxidchloriden

Synthesis, Properties, and Molecular Structures of Alkylaluminium Aminoalkoxide Chlorides Alkylaluminium aminoalkoxide chlorides [R(Cl)AlOR*] 1 – 3 have been obtained from the reaction of dialkyl aluminium chlorides R₂AlCl with the respective aminoalkohol HOR* ( 1 : R = Et, OR* = dimethylamino‐1‐propanol; 2 : R = Me, OR* = (+);(–)‐dimethylamino‐2‐propanol; 3 : R = Me, OR* = (S)‐N‐methyl‐2‐pyrrolidinyl‐methanol). The reaction between dimethylaluminium chloride and (S)‐α, α‐diphenyl‐2‐pyrrolidinyl‐methanol (OR* = Dpm) yielded, by contrast, the ionic {[MeAl(OR*)₂AlMe₂]⁺ [MeAlCl₃]^–} complex ( 4 ). 1 – 4 have been characterised by ¹H, ¹³C and ²⁷Al‐NMR spectroscopy. Crystal structures of 1 and of the 1 : 1 solvate of 4 with Et₂O have been determined by X‐ray methods and the absolute structure of 4 was confirmed by refinement of the Flack‐parameter. The dimeric molecules of 1 are composed of two chelating rings linked via an almost planar Al₂O₂ unit and pentacoordination is observed about aluminium. In contrast, each of the two crystallographically independent cation molecules of 4 contains one four‐ and and one five‐coordinate metal centre.     

Fifty Years of Mössbauer Spectroscopy in Solid State Research – Remarkable Achievements,Future Perspectives

Mössbauer spectroscopy was founded more than fifty years ago based on an outstanding discovery by the young German physicist Rudolf Ludwig Mössbauer while working on his Ph.D. thesis. He discovered the recoilless nuclear resonance fluorescence of gamma radiation and was awarded the Nobel Prize in Physics in 1961 as one of the youngest recipients of this most prestigious award. His discovery led to the development of a new technique for measurements of hyperfine interactions between nuclear moments and electromagnetic fields. This method, with highest sharpness of tuning of 10^–13, yields information on valence state, symmetry, magnetic behavior, phase transition, lattice dynamics and other solid state properties.     

Vibrational Spectra and Magnetic Properties of Eu3[BN2]2 and LiEu4[BN2]3

Eu₃[BN₂]₂ and LiEu₄[BN₂]₃ were synthesized from a stoichiometric mixture of EuN, BN, europium metal and Li₃N, EuN and BN (ratio: 1:4:3) in sealed niobium ampoules at 1475 and 1275 K, respectively. Temperature dependent susceptibility measurements of Eu₃[BN₂]₂ and LiEu₄[BN₂]₃ show Curie‐Weiss behavior with experimental magnetic moments of 8.03(5) and 8.5(1) μ_B/Eu atom, respectively, compatible with divalent europium. Both nitridoborates order ferromagnetically at T_C = 32.0(5) K (Eu₃[BN₂]₂) and 22.0(5) K (LiEu₄[BN₂]₃). The saturation magnetizations of 5.73(5) μ_B/Eu atom at 5 K and 7 T for Eu₃[BN₂]₂ and 4.2 μ_B/Eu atom at 5 K and 2 T for LiEu₄(BN₂)₃ are smaller than the maximum value of 7 μ_B. ¹⁵¹Eu Mössbauer data of Eu₃[BN₂]₂ at 4.2 K show an isomer shift of —11.4(1) mm/s and an experimental line width of 3.1(2) mm/s. Full magnetic hyperfine field splitting with 26.2(3) T at the europium nuclei is detected. Vibrational spectra of Eu₃[BN₂]₂ are interpreted on the basis of discrete [BN₂]^3— units with symmetry D_∞h by taking into account the existence of two crystallographically independent [BN₂]^3— anions and their dynamic coupling in the unit cell (factor group splitting).     

Mössbauer Spectroscopic Studies of Supported α-Fe2O3 and Fe Catalysts I: Particle Size Determination and Support Effect

The chemical state of particles of 5wt% Fe in α-Fe₂O₃ and the subsequently reduced iron particles supported on different particle size (50–200 mesh) of silica (SiO₂), alumina (Al₂O₃), magnesium oxide (MgO) and carbon (C) was examined by Mössbauer spectroscopy at various stages of calcination and reduction. The particle size of the α-Fe₂O₃ supported on different mesh sizes (50, 100, 140, 200 mesh) of SiO₂ has been determined. The strength of metal-support interaction with respect to the kind of support was found to be MgO>SiO₂>Al₂O₃>C.     

Mössbauer Spectroscopic Studies of Supported α-Fe2O3 and Fe Catalysts II: The Effect of the Second Metal Addition

The effect of the addition of a second metals such as Zn and Ni on the calcinaton and reduction of alumina, magnesia and silicasupported iron catalysis with total iron loading of 5wt% is investigated by Mössbauer spectroscopy. It is shown that the reducibility of supported α-Fe₂O₃ is gradually increased by adding the second metal. The values of the magnetic hyperfine field obtained from Mössbauer spectra for the Zn or Ni-added α-Fe₂O₃ or Fe catalysts decreased with increasing second metal loading.     

Koexistenzbeziehungen,Darstellung und Eigenschaften ternärer Phasen im System Cu/Mo/O

Coexistence Relations, Preparation and Properties of Ternary Compounds in the System Cu/Mo/O The phase diagram of the ternary system Cu/Mo/O is presented at 773 K. The compounds CuMoO₄, Cu₃Mo₂O₉, Cu₄Mo₅O₁₇, Cu₆Mo₅O₁₈, Cu_4–xMo₃O₁₂, and Cu_xMoO₃ are found to be thermodynamical stable. The homogeneity range of Cu_4–xMo₃O₁₂ runs to x = 0.1–0.2. Single crystals of CuMoO₄ and Cu₃Mo₂O₉ were grown by chemical transport reactions with TeCl₄, Cl₂, HCl, and Br₂ as transport agent. The results were compared with thermochemical calculations. The decomposition of CuMoO₄ and Cu₃Mo₂O₉ was investigated with thermal analysis and decompositon pressure measurements.     

Zum System Zn/Mo/O. I. Phasenbestand und Eigenschaften der ternären Zinkmolybdate; Struktur von Zn3Mo2O9

On the System Zn/Mo/O. I. Phases and Properties of Ternary Zinc Molybdates; Crystal Structure of Zn₃Mo₂O₉ Several ternary compounds are known in the Zn/Mo/O-system. The phases ZnMoO₄, Zn₂Mo₃O₈ and Zn₃Mo₂O₉ are stable at 900°C. The coexistence ranges are shown in the ternary phase diagram. The structure of Zn₃Mo₂O₉ has been determined by single crystal X-ray diffraction. The compound crystallizes in the monoclinic space group P2₁/m (a = 7,757(1) Å, b = 7,132(1) Å, c = 8,370(2) Å, β = 117,40(1)º, Z = 2).     

Darstellung und Kristallstruktur von ANi10P3 (A: Zn,Ga, Sn,Sb)

Preparation and Crystal Structure of A Ni₁₀P₃ ( A : Zn, Ga, Sn, Sb) Four compounds ANi₁₀P₃ (A: Zn, Ga, Sn, Sb) were prepared by heating mixtures of the elements and investigated by means of X‐ray methods. Single crystal structure determinations of ZnNi₁₀P₃ (a = 7.665(1), c = 9.360(1) Å) and SnNi₁₀P₃ (a = 7.674(1), c = 9.621(1) Å) respectively showed, that they are isotypic and crystallize in a new structure (P3m1; Z = 3). This type is characterized by 3²⁰ and 3²⁴ cages of Ni atoms (Frank Kasper polyhedra), which are connected with each other. A atoms are located in the centres of these polyhedra and have no direct bonds to the P atoms.     

Eu3F4S2: Synthesis, crystal structure, and magnetic properties of the mixed-valent europium(II,III) fluoride sulfide EuF2·(EuFS)2

Using the method to synthesize rare-earth metal(III) fluoride sulfides MFS (M=Y, La, Ce–Lu), in some cases we were able to obtain mixed-valent compounds such as Yb₃F₄S₂ instead. With Eu₃F₄S₂ another isotypic representative has now been synthesized. Eu₃F₄S₂ (tetragonal, I4/mmm, a=400.34(2), c=1928.17(9) pm, Z=2) is obtained from the reaction of metallic europium, elemental sulfur, and europium trifluoride in a molar ratio of 5:6:4 within seven days at 850 °C in silica-jacketed gas-tightly sealed platinum ampoules. The single-phase product consists of black plate-shaped single crystals with a square cross section, which can be obtained from a flux using equimolar amounts of NaCl as fluxing agent. The crystal structure is best described as an intergrowth structure, in which one layer of CaF₂-type EuF₂ is followed by two layers of PbFCl-type EuFS when sheeted parallel to the (001) plane. Accordingly there are two chemically and crystallographically different europium cations present. One of them (Eu²⁺) is coordinated by eight fluoride anions in a cubic fashion, the other one (Eu³⁺) exhibits a monocapped square antiprismatic coordination sphere with four F⁻ and five S²⁻ anions. Although the structural ordering of the different charged europium cations is plausible, a certain amount of charge delocalization with some polaron activity has to take place, which is suggested by the black color of the title compound. Temperature dependent magnetic susceptibility measurements of Eu₃F₄S₂ show Curie–Weiss behavior with an experimental magnetic moment of 8.19(5) μ_B per formula unit and a paramagnetic Curie temperature of 0.3(2) K. No magnetic ordering is observed down to 4.2 K. In accordance with an ionic formula splitting like (Eu^II)(Eu^III)₂F₄S₂ only one third of the europium centers in Eu₃F₄S₂ carry permanent magnetic moments. ¹⁵¹Eu-Mössbauer spectroscopic experiments at 4.2 K show one signal at an isomer shift of −12.4(1) mm/s and a second one at 0.42(4) mm/s. These signals occur in a ratio of 1:2 and correspond to Eu²⁺ and Eu³⁺, respectively. The spectra at 78 and 298 K are similar, thus no change in the Eu²⁺/Eu³⁺ fraction can be detected.