Kristallstrukturuntersuchungen an Verbindungen des Typs A3(M,Nb)8O21 (A  Tl,Ba; M  Fe,Ni)

Crystal Structure Investigations of Compounds with the A₃(M, Nb)₈O₂₁-Type (A ? Tl, Ba; M ? Fe, Ni) Tl₃Fe_0,5Nb_7,5O₂₁ (A), a hitherto unknown phase of the A₃(M, Nb)₈O₂₁-type, and Ba₃Fe₂Nb₆O₂₁ (B), Ba₃Ni_1.33Nb_6,66O₂₁ (C) were prepared and investigated by single crystal X-ray technique. ((A): a = 9.145(1), c = 11.942(1) Å; (B): a = 9.118(2), c = 11.870(1) Å; (C) a = 9.173(3), c = 11.923(1) Å, space group D? P6₃/mcm, Z = 2). There is a statistic occupation of the M-positions by Nb⁵⁺ and Fe³⁺ or Nb⁵⁺ and Ni²⁺, respectively. An other compound Ba₃Fe₂Ta₆O₂₁ is partially ordered in respect to Ta⁵⁺ and Fe³⁺. Calculations of the Coulomb-part of lattice energy are discussed.     

Kristallstrukturverfeinerungen an Natriumtrifluorometallaten NaMF3 (M  Mg,Co, Ni,Zn): Oktaederkippung und Toleranzfaktor orthorhombischer Fluorperowskite

Crystal Structure Refinements of Sodium Trifluorometallates NaMF₃ (M ? Mg, Co, Ni, Zn): Tilting of Octahedra and Tolerance Factor of Orthorhombic Fluoroperovskites Based on newly measured X-ray single crystal data the crystal structures of the orthorhombic fluoroperovskites NaMF₃ (M ? Mg, Co, Ni, Zn) were refined in space group Pbnm (GdFeO₃ type, Z = 4). The octahedra are but slightly distorted; the average distances (and bridge angles M? F? M) are: Mg? F = 197.8 pm (150.9°), Co? F = 203.8 pm (146.1°), Ni? F = 200.3 pm (148.0°) and Zn? F = 202.3 pm (147.4°). With respect to the axes of the pseudocell (Z = 1) the octahedra are rotated by tilt angles which vary, including NaMnF₃ and NaFeF₃, between 14.6 and 18.8°. The tilting becomes the more pronounced, the smaller the tolerance factor of the compound, so as to yield uniformly average values of Na? F = 232 pm for the four shortest distances within the [NaF₈] coordination (distorted tetrahedron and bicapped trigonal prism, respectively). Measurements of magnetic powder susceptibilities show that tilting of octahedra is no sufficient cause to produce spin canting resulting in ferromagnetism: This property is confirmed only for NaNiF₃ (T_N = 150 K), whereas NaCoF₃ exhibits a sharp minimum in its χ^?l-T curve (T_N = 75 K) and remains uncanted antiferromagnetic then down to 4.2 K.     

Zur Kenntnis des RbNiCrF6-Typs: über CsCuMF6 (M  NiIII,TiIII), CsMgMF6 (M  Co,Fe, Ga) und CsZnMF6 (M  NiIII,CoIII, FeIII)

On the RbNiCrF₆ Type(¹): On CsCuMF₆ (M?Ni^III, Ti^III), CsMgMF₆ (M ?Co, Fe, Ga), and CsZnMF₆ (M?Ni^III, Co^III, Fe^III) New prepared are the cubic compounds CsCuNi^IIIF₆ (dark brown, a = 10.14 Å); CsZnNi^IIIF₆ (dark brown, a = 10.17 Å); CsCuTi^IIIF₆ (light grey, a = 10.39 Å); CsMgGaF₆ (colourless, a = 10.23 Å); CsMgFeF₆ (colourless, a = 10.53 Å); CsZnFeF₆ (colourless, a = 10.42 Å); CsMgCo^IIIF₅ (light blue, a = 10.27 Å) and CsZnCo^IIIF₆ (light blue, a = 10.34 Å), all RbNiCrF₆-type of structure. The Madelung part of lattice energy, MAPLE, is calculated and discussed.     

Alternativ-Liganden. XXVI [1]. M(CO)4L-Komplexe (M  Cr,Mo, W) der Chelatliganden Me2ESiMe2(CH2)2E′Me2 (Me  CH3; E  P,As; E′  N,P, As)

Alternative Ligands. XXVI. M(CO)₄ L-Complexes (M ? Cr, Mo, W) of the Chelating Ligands Me₂ESiMe₂(CH₂)₂E′ Me₂ (Me ? CH₃; E ? P, As; E′ ? N, P, As) The reaction of M(CO)₄NBD (NBD = norbornadiene; M ? Cr, Mo, W) with the ligands Me₂ESiMe₂(CH₂)₂E′ Me₂ yields the chelate complexes (CO)₄M[Me₂ESiMe₂]) for E,E′ ? P, As, but not for E and /or E′ ? N. The NSi group is not suited for coordination because of strong (p-d)π-interaction. In the case of the ligands with E ? P or As and E′ ? N chelate complexes can be detected in the reaction mixture, but isolable products are complexes with two ligands coordinated via the E donor group. The new compounds are characterized by analytical and spectroscopic (IR, NMR, MS) investigations. The spectroscopic data are also used to deduce the coordinating properties of the ligands. X-ray diffraction studies of the molybdenum complexes (CO)₄Mo[Me₂ESiMe₂(CH₂)₂AsMe ₂] (E ? P, As) in accord with the observed coordination effects show only small differences between SiE and CE donor functions. Attempts to use the ligands Me₂ESiMe₂(CH₂)₂AsMe₂ (E ? P, As) for the preparation of Fe(CO)₃L complexes result in the fission of the SiE bonds and the formation of the binuclear systems Fe₂(CO)₆(EMe₂)₂ (E ? P, As) together with the disilane derivative [Me₂Si(CH₂)₂AsMe₂]₂.     

Über Verbindungen vom Typ Ba3BIIMO9 mit BII  Mg,Ca, Sr,Ba und MV  Nb,Ta

Compounds of the Type Ba₃B^IIM O₉ with B^II ? Mg, Ca, Sr, Ba, and M^V ? Nb, Ta The hexagonal perovskites Ba₃B^IIMO₉ (M^V ? Nb, Ta) crystallize with B^II ? Mg Ca in a 3 L structure (sequence (c)₃) and B^II ?; Sr in the hexagonal BaTiO₃ type (6 L; sequence (hcc)₂) with an 1:2 order for the B and M ions. Intensity calculations for Ba₃SrNb₂O₉ and Ba₃SrTa₂O₉ gave in the space group P6₃/mmc a refined, intensity related R′ value of 8.4% (Nb) and 9.0% (Ta) respectively. For B^II ? Ba the perovskite Ba₃BaTa₂O₉ has an orthorhombic distorted 6 L structure and forms with Ba₃SrTa₂O₉ a continuous series of mixed crystals (Ba₃Sr_1?xBa_xTa₂O₉). In the system Ba₃Sr_1?xBa_xNb₂O₉ the range of existence of the hexagonal BaTiO₃ type is confined to the Sr richer end. The pure Ba compound possesses a proper structure type (5 L: Ba₅BaNb₃□O_13.5□_1.5).     

Darstellung und Eigenschaften der festen Lösungen (Ca,SE)F2,33 mit SE  Y,La, Ln und der korrespondierenden Ordnungsphasen Ca2SEF7 mit SE  Er – Lu und Y

Preparation and Characterization of the Solid Solutions (Ca,RE)F_2,33 with RE ? Y, La, Ln and the Corresponding Superstructure Phases Ca₂REF₇ with RE ? Er–Lu and Y Solid solutions of the composition (Ca,RE)F_2.33 with RE ? Y, La, Ln were prepared by annealing of 2:1 mixtures of CaF₂ and REF₃ at 950–1000°C. X-Ray powder investigations showed that samples quenched to room-temperature have a cubic, anion-excess fluorite structure. Annealing at 500°C, however, resulted in tetragonal superstructure phases Ca₂REF₇ in the case of RE ? Er? Lu and Y. Accurate lattice parameters of all phases are reported. The regions of stability were determined by thermal analysis for both, the solid solutions and the ordered phases. Corresponding data of (Ca, Pm)F_2.33, Ca₂DyF₇ and Ca₂HoF₇ were estimated.     

Über die Existenz von Verbindungen des Typs Hg2XA (X  Halogen,A  Anion ≠ Halogen) und Hg2XY (X und Y Halogen)

Existence of Hg₂XA (X ? Halide, A ? Anion ≠ Halide) and Hg₂XY Compounds (X and Y Halide) Investigations in molten mercuric bromide HgBr₂ [1, 2] and comparing considerations between mercuric and mercurous chemistry lead to the till now unknown or less investigated compounds Hg₂XA and Hg₂XY (X, Y halide; A anion ≠ halide). Using TGA and DTA measurements in order to improve the reaction conditions Hg₂XClO₄ salts could be synthesized, whereas the hydrogene sulfates Hg₂XHSO₄ are formed in concentrated sulfuric acid (crystalline, instable by solvent removing). Powder diagrams and spectrochemical investigations point our that the lattices of the isolated mixed halides Hg₂BrCl, Hg₂BrI, and Hg₂ClI contain not only the pure molecules Hg₂X₂ and Hg₂Y₂ but also the mixed molecules Hg₂XY. Final statements need X-ray investigations.     

Die Kristallstrukturen der Vanadium-Weberite Na2MIIVIIIF7 (MII  Mn,Ni, Cu) und von NaVF4

The Crystal Structures of the Vanadium Weberites Na₂M^IIV^IIIF₇ (M^II ? Mn, Ni, Cu) and of NaVF₄ At single crystals of the vanadium(III) compounds NaVF₄ (a = 790.1, b = 531.7, c = 754.0 pm, β = 101.7°; P2₁/c, Z = 4), Na₂NiVF₇ (a = 726.0, b = 1031.9, c = 744.6 pm; Imma, Z = 4) and Na₂CuVF₇ (a = 717.6, b = 1043.5, c = 754.6 pm; Pmnb, Z = 4) X-ray structure determinations were performed, at Na₂MnVF₇ (a = 746.7, c = 1821.6 pm; P3₂21, Z = 6) a new refinement. NaVF₄ crystallizes in the layer structure type of NaNbO₂F₂. The fluorides Na₂M^IIVF₇ represent new orthorhombic (M^II ? Ni; Cu) resp. trigonal (M^II ? Mn) weberites. The average distances within the [VF₆] octahedra of the four compounds are in good agreement with each other and with data of related fluorides (V? F: 193.3 pm). The differences between mean bond lengths of terminal and bridging F ligands are 5% in NaVF₄, but less than 1% in the weberites. Details and data for comparison are discussed.     

Synthese und Struktur von MII[AuF4]2 (MII  Cd,Hg)

Synthesis and Structure of M^II[AuF₄]₂ (M^II ? Cd, Hg) Cd[AuF₄]₂ and the isotypic compound Hg[AuF₄]₂, both are yellow, crystallize tetragonal in the space-group P4/mcc-D (No. 124) with a = 575.0/575.6 pm, c = 1034.8/1042.3 pm and Z = 2. The single-crystals were obtained by solid-state reactions in goldtubes.     

Neue Tetrapnictidotitanate(IV): Na3M3[TiX4] mit M  Na/Sr,Na/Eu und X  P,As

New Tetrapnictidotitanates(IV): Na₃M₃[TiX₄] with M ? Na/Sr, Na/Eu and X ? P, As The four novel tetrapnictidotitanates(IV) Na₄Sr₂TiP₄, Na₄Sr₂TiAs₄, Na_4.3Eu_1.7TiP₄ and Na_4.3Eu_1.7TiAs₄ were prepared from the binary pnictides NaX, M₃X, M′X (X ? P, As and M′ ? Sr, Eu) and elementary titanium in tantalum ampoules. The air and moisture sensitive transition metal compounds form dark red hexagonal crystals. They are semiconductors with E_g = 1.8eV (Sr) and E_g = 1.3eV (Eu), respectively. The compounds are isotypic with Na₆ZnO₄ (space group P6₃mc (no. 186); hP22; Z = 2; Na₄Sr₂TiP₄; a = 936.8(1) pm, c = 740.5(1) pm; Na₄Sr₂TiAs₄: a = 958.2(1) pm, c = 757.1(1) pm; Na_4.3Eu_1.7TiP₄: a = 929.9(2) pm, c = 732.0(2) pm; Na_4.3Eu_1.7TiAs₄: a = 953.9(1) pm, c = 749.5(1) pm). Main structural units are polar oriented [TiP₄]^8? and [TiAs₄]^8? tetrahedral anions with d (Ti? P) = 240.2(3) pm and d (Ti? As) = 248.6(3) pm.     

Disupersilylmetalle (tBu3Si)2M und Supersilylmetallhalogenide tBu3SiMX mit M  Zn,Cd, Hg: Synthesen,Strukturen, Eigenschaften

Disupersilylmetals (^tBu₃Si)₂M and Supersilylmetal Halides ^tBu₃SiMX with M ? Zn, Cd, Hg: Syntheses, Properties, Structures Disupersilylmetals (^tBu₃Si)₂Zn (colorless), (^tBu₃Si)₂Cd (light yellow), (^tBu₃Si)₂Hg (light yellow), and supersilylmetal halides ^tBu₃SiZnCl(THF) (colorless), ^tBu₃SiCdI (colorless), ^tBu₃SiHgCl (colorless) are obtained in THF by the action of ^tBu₃SiNa on ZnCl₂, CdI₂, HgCl₂ in the molar ratio 2:1 and 1 :1, respectively. THF can be exchanged by TMEDA under formation of ^tBu₃SiZnCl(TMEDA), and (^tBu₃Si)₂Zn transforms by the action of BiCl₃ or BBr₃ into ^tBu₃SiZnCl (colorless) and ^tBu₃SiZnBr (colorless), respectively. As to X-ray crystal structure analyses, the compounds (^tBu₃Si)₂M are monomeric with a linear SiMSi framework, whereas ^tBu₃SiZnBr and ^tBu₃SiHgCl are tetrameric, the former with a regular, the latter with a pronounced irregular cubic M₄X₄ framework. The compounds are thermal stable up to 200°C (exception (^tBu₃Si)₂Cd), photolabile, and comparatively inert for water and oxygen. The disupersilylmetals work as sources of supersilyl radicals ^tBu₃Si (on irradiation) and as mild supersilanidation agents (e.g. (^tBu₃Si)₂Zn/BBr₃ → ^tBu₃SiZnBr/^tBu₃SiBBr₂), the supersilylmetal halides as Lewis acids (formation of ^tBu₃SiMX · donor) and electrophiles (e.g. ^tBu₃SiHgCl/RLi → ^tBu₃SiHgR/LiCl).     

Polysulfonylamine. LXXXIV [1]. Zur Isotypie in den Dimesylamid-Komplexreihen [M(H2O)4{(CH3SO2)2N}2] (MMg,Ca, Ni,Cu, Zn,Cd) und [M(py)4{(CH3SO2)2N}2] (MNi,Cu, Zn,Cd)

Polysulfonylamines. LXXXIV. Isotypic Structures in the Dimesylamide Complex Series [M(H₂O)₄{(CH₃SO₂)₂N}₂] (M?Mg, Ca, Ni, Cu, Zn, Cd) and [M(py)₄{(CH₃SO₂)₂N}₂] (M?Ni, Cu, Zn, Cd) The crystal structures of the trans-octahedral complexes [M(H₂O)₄{(CH₃SO₂)₂N}₂] (M?Ca, Cd), in which the dimesylamide anion acts as a monodentate O-ligand and a tetrafunctional hydrogen bond acceptor, were determined by low-temperature X-ray diffraction. Both belong to an isotypic series (triclinic, space group P1 , Z = 1) that had previously been characterized for M?Mg, Ni, Cu and Zn (Z. Anorg. Allg. Chem. 1996 , 622, 1065). In this structure there exists an extended network of strong hydrogen bonds which is probably the underlying reason why the structure type surprisingly persists across the whole series. To support this explanation by indirect evidence from comparison with suitable structures devoid of strong hydrogen bonding, the analogous trans-octahedral complexes [M(py)₄{(CH₃SO₂)₂N}₂] (M?Mn, Co, Ni, Cu, Zn, Cd) were prepared by treating M[(CH₃SO₂)₂N]₂ with pyridine, and the crystal structures of the Ni, Cu, Zn and Cd compounds were studied by low-temperature X-ray crystallography. As anticipated, the four pyridine complexes do not form an isotypic series but instead two isotypic pairs consisting of the Ni and Zn compounds (monoclinic, space group P2₁/n, Z =2) and of the Cu and Cd complexes (triclinic, space group P1, Z = 1). All molecules of the aqua and the pyridine complexes display crystallographic centrosymmetry. In the hydrates, the mean M? OH₂ and the M? O(anion) distances are 232.6 and 232.7 pm for M ? Ca, 225.5 and 230.3 pm für M ? Cd. The mean M? N and the M? O(anion) bond lengths of the pyridine species amount to 211.8 and 213.1 pm for M ? Ni, 217.0 and 218.5 pm for M ? Zn, 232.8 and 234.4 pm for M ? Cd; the corresponding values for the severely Jahn-Teller distorted Cu complex are 203.6 and 254.5 pm. In the crystals of the pyridine complexes, each methyl group is connected through a weak C? H…?O bond to a sulfonyl oxygen atom of an adjacent molecule.     

Die Bedeutung der Gasmolekeln MGa2Cl8, MGaCl5 und MCl2 (M = Ca,Cr, Fe,Co, Ni,Cu, Pd) beim chemischen Transport von MCl2,f mit GaCl3/Ga2Cl6

The Meaning of the Gas Molecules MGa₂Cl₈, MGaCl₅, and MCl₂ (M = Ca, Cr, Fe, Co, Ni, Cu, Pd) in the Chemical Transport of MCl_2,f, with GaCl₃/Ga₂Cl₆ On the reaction of MCl_2,s with GaCl₃ the vapor pressures of MGa₂Cl₈, MGaCl₅. MCl₂, Ga₂Cl₆, and GaCl₃ are found to exist above the solid phase. The temperature dependence of λ(M) = ΣP(M)/ΣP(Ga) is essential for the chemical transport of MCl_2,s. On variation of T a maximum of P(MGa₂Cl₈) is observed which originates from the dissociation reaction Ga₂Cl₆ = 2 GaCl₃ and which may lead in uncomplicated cases to a maximum of λ/T curve. Further increase in T results in a minimum of the λ/T dependence; its position is governed by the value of P(MCl₂) + P(MGaCl₅). In the range between maximum and minimum of λ/T MCl_2,s is transported into th high temperature region. Reduced stability of MGa₂Cl₈ and/or increased stability of MGaCl₅ resp. MCl_2,g may lead to a λ/T dependence without extrema. No transport of MCl₂ to the high temperature region may take place under these conditions. Experimental and calculated data are given for the reactions under consideration.     

Neue Lithiumchlorid-Suzukiphasen: Li6MCl8(M = Fe,Co, Ni)

Novel Lithium Chloride Suzuki Phases, Li₆MCl₈ (M = Fe, Co, Ni) The hitherto unknown Suzuki phases Li₆FeCl₈, Li₆CoCl₈, and Li₆NiCl₈ ( cF 60) were prepared by fusing the binary chlorides. X-ray, DTA, and conductivity data as well as the infrared and Raman spectra are presented. The unit cell dimensions of the cubic (space group Fm3 m) halides are a = 1029.3, 1027.5, and 1023.5 pm, respectively. Li₆FeCl₈ and Li₆CoCl₈ undergo a reversible phase transition to disordered LiCl solid solutions at 275 and 355°C, respectively. The metastable nickel compound can only be prepared by quenching from about 560°C. The lithium chloride Suzuki phases are fast lithium ion conductors at elevated temperatures. The specific conductivities are 1.4 × 10^?1, 1.5 × 10^?1, and 6.9 × 10^?2Ω^?1 × cm^?1 at 500°C, respectively. Whereas the i.r. spectra of the Suzuki phases only reveal a broad band, the Raman spectra exhibit the four group theoretically allowed modes as sharp scattering peaks, which are discussed in terms of the vibrational modes of this structure.