Tl5SnF9 und Tl5TiF9: die ersten [Tl5F3]2+‐Schichten in neuartigen Thallium(I)‐fluoridfluorometallaten(IV)

Tl₅SnF₉ and Tl₅TiF₉: The First [Tl₅F₃]²⁺ Layers in Novel Thallium(I) Fluoridefluorometallates(IV) Tl₅TiF₉ and Tl₅SnF₉ were prepared via solid state reactions from mixed powders of the TlF and SnF₄ or TiF₄, respectively, in platinum crucibles under Ar (573 K). Both fluorides are colourless, transparent and extremely hygroscopic. The compounds Tl₅MF₉ (M = Sn, Ti) crystallize in a new structure type in Pbam (Nr. 55) with a = 1117.6 pm, b = 684.8 pm, c = 799.2 pm for Tl₅SnF₉ and a = 1111.4 pm, b = 674.7 pm, c = 783.2 pm for Tl₅TiF₉. Characteristic building units in the new Thallium(I) fluoridefluorometallates(IV) are [Tl₅F₃]²⁺ sheets found for the first time, which are connected via [MF₆]^2– octahedra (M = Ti, Sn) to a threedimensional network (d_Sn–F = 194–197 pm, d_Ti–F = 186–187 pm). The monovalent Tl are coordinated by 8 F with distances Tl–F between 264 and 334 pm. The chemical bonding is discussed on the basis of Extended‐Hückel band structure calculations.     

Thallium(I), Silver(I), and Mixed Thallium(I)/Copper(I) Clusters with Bridging {Me2Si(N‐C6H4‐2‐SPh)2}2– Ligands

The S‐functionalized aminosilane Me₂Si(NH‐C₆H₄‐2‐SPh)₂ (H₂L) ( 1 ) was prepared from dichlorodimethylsilane and lithiated 2‐(phenylthio)aniline. Treatment of compound 1 with two equivalents of n‐butyllithium led to the dilithium derivative Li₂L, which was used in subsequent reactions with MCl (M = Tl, Cu, Ag) to prepare the complexes [Tl₂L] ( 2 ), [Cu₂Tl₂L₂] · 2THF ( 3a ), [Cu₂Tl₂L₂(THF)₂] ( 3b ), and [Ag₄L₂(THT)₂] ( 4 ) (THT = tetrahydrothiophene). Compound 2 consists of two thallium atoms, which are connected by a L^2– ligand to give a puckered Tl₂N₂ ring with Tl–N distances of 255(1)–268(1) pm. Compounds 3a and 3b are heterobimetallic complexes, which are based on [Cu₂L₂]^2– cores featuring a Cu₂N₄Si₂ ring with linearly coordinated copper atoms [Cu–N: 190.7(3)–192.5(3) pm] and two peripherally attached Tl atoms [Tl–N: 272.7(3)–281.9(3) pm]. The molecular structure of the tetranuclear silver(I) complex 4 is closely related to the structure of compounds 3a and 3b by replacement of the Cu and Tl atoms with Ag atoms. The Ag–N distances are 217.5(3)–245.7(3) pm.     

Kristallstruktur des „supramolekularen”︁ Komplexes [Cs2(18-Krone-6)][HgI4] mit ungewöhnlich koordinierten Cs-Ionen

Crystal Structure of the “Supramolecular” Complex [Cs₂(18-crown-6)][HgI₄] with Unusually Coordinated Cs Ions The reaction of 18-crown-6, 1,4,7,10,13,16-hexaoxacyclooctadecane, with HgI₂/CsI in methanol yields crystals of [Cs₂(C₁₂H₂₄O₆)][HgI₄]. The compound crystallizes monoclinically, space group P2₁/c, Z = 4, a = 1574.8(3), b = 1067.0(3), c = 1693.2(6) pm, and β = 98.29(3)º. The structure consists of a network made up of two different types of [Cs-(18-crown-6)-Cs]²⁺ cations, interconnected by [HgI₄]^2? anions. The cations form an “anti-sandwich” structure with relatively short Cs ? Cs distances of 382 pm in the first type of cations and a longer distance of 480 pm in the second type of cations.     

Kristallstruktur von Tl4Fe(CN)6

Crystal Structure of Tl₄Fe(CN)₆ Single crystals of Tl₄Fe(CN)₆ have been prepared for the first time and its crystal structure was determined. The pale yellow compound crystallizes in the triclinic space group P1 (No. 2) with the lattice parameters a = 726.6(1) pm, b = 797.4(8) pm, c = 1 336.0(1) pm, α = 104.7(9)°, β = 90.0(8)°, γ = 97.6(7)°, Z = 2 in a new structure type.     

Syntheses and Crystal Structures of the Thallium(I) Iodobismuthates(III) Tl7Bi3I16 and Tl3BiI6

Dark grey (dark red with transmitting light) crystals of heptathallium(I) hexadecaiodo‐tribismuthate(III), Tl₇Bi₃I₁₆, were obtained by slow cooling of a melt from 800 K to ambient temperature and, with higher crystal quality via solvothermal synthesis in aqueous HI by slowly cooling from 428 to 363 K. The compound is diamagnetic and melts congruently at 630(5) K. X‐ray diffraction on single‐crystals revealed that Tl₇Bi₃I₁₆ crystallizes in the orthorhombic space group Cmcm with lattice parameters a = 2473.4(5), b = 1441.9(2), c = 3616.9(7) pm. The crystal structure can be interpreted as a layered intergrowth of fragments from the CsNiCl₃ and K₅Dy₃I₁₂ structure types with isolated [BiI₆]^3? octahedra and [Bi₂I₁₀]^4? double octahedra. Rotation and distortion of the complex anions establish coordination numbers (c.n.) between 7 and 9 for the Tl⁺ cations. Dark red crystals of trithallium(I) hexaiodo‐bismuthate(III), Tl₃BiI₆, are only accessible via hydrothermal synthesis in aqueous HI and slowly cooling from 428 to 363 K. Thermal analysis reveals a peritectoid decomposition at 540(5) K into the neighboring phases Tl₇Bi₃I₁₆ and TlI. Tl₃BiI₆ crystallizes in the monoclinic space group P2₁/c with lattice parameters a = 1352.6(3), b = 899.6(2), c = 1353.8(3) pm, and β = 104.18(3)°. In the crystal structure isolated [BiI₆]^3? octahedra are arranged according to the motif of a face‐centered pseudo‐cubic packing. Due to the tilted orientation of the [BiI₆]^3? groups the Tl⁺ cations have c.n. of 8 and 9. Although the crystal structure of Tl₃BiI₆ looks like a distorted variant of the elpasolith type, there is no symmetry relation according to a group subgroup formalism.     

The crystal structure of barium manganese(II) iron(III) fluoride BaMnFeF7

The crystal structure of the monoclinic compound BaMnFeF₇ has been determined: a = 553.2(1), b = 1098.0(2), c = 918.3(1) pm, β = 94.67(1)°, V = 555.9(3) × 10^?24 cm³, Z = 4. All atoms are in general positions of space group $\text{P2}{}_1\text{c}$, weighted R = 0.031, using 1771 independent single-crystal reflections with I > 2σ(I). The structure consists of edge-sharing dinuclear Mn₂F^6?₁₀ units (MnMn = 322.2 pm), linked via corners by intermediate FeF₆ octahedra, at which two cis ligands remain unbridged. The average distances in the distorted octahedra are MnF = 211.6 pm and FeF = 192.7 pm. The barium atoms are irregularly 12-coordinated with a mean distance BaF = 290.5 pm. The structure is discussed in relation to the trigonal weberite Na₂MnFeF₇ and others.     

Über Thallium(I)-chlorooxomolybdate: Synthese und Kristallstrukturen von Tl[MoOCl4(NCCH3)], Tl[Mo2O2Cl7] und Tl2[Mo4O4Cl14] und die Struktur von Tl2[MoCl6]

On Thallium(I)-oxochloromolybdates: Synthesis and Crystal Structures of Tl[MoOCl₄(NCCH₃)], Tl[Mo₂O₂Cl₇], and Tl₂[Mo₄O₄Cl₁₄] and the Structure of Tl₂[MoCl₆] Black crystals of Tl₂[MoCl₆] are formed in the reaction of TlCl with MoOCl₃ in a sealed evacuated glass ampoule at 350 °C. The crystal structure analysis shows that Tl₂[MoCl₆] (cubic, Fm 3¯m, a = 986.35(7) pm) adopts the K₂[PtCl₆] structure with a Mo–Cl bond length of 236.6 pm. Tl[MoOCl₄(NCCH₃)] was obtained by the reaction of TlCl with MoOCl₃ in acetonitrile in form of yellow, moisture sensitive crystals. The structure (orthorhombic, Cmcm, a = 746.0(1), b = 1463.8(3), c = 857.3(2) pm) is built of Tl⁺ cations and octahedral [MoOCl₄(NCCH₃)]^– anions in which the acetonitrile ligand is bound in trans position to the oxygen. The reaction of TlCl and MoOCl₃ in dichloromethane yields Tl[Mo₂O₂Cl₇] and Tl₂[Mo₄O₄Cl₁₄] as green moisture sensitive crystals. The structure of Tl[Mo₂O₂Cl₇] (orthorhombic, Pmmn, a = 694.3(1), b = 951.9(2), c = 904.7(1) pm) consists of Tl⁺ cations and dinuclear [Mo₂O₂Cl₇]^– anions, with two equidistant chlorine bridges of 248.2 and one longer chlorine bridge of 265.7 pm. The oxygen atoms are located in the trans positions of the longer chloro bridge. The structure of Tl₂[Mo₄O₄Cl₁₄] (triclinic, P1¯, a = 692.8(1), b = 919.6(1), c = 998.9(1) pm, α = 104.94(1)°, β = 90.31(1)°, γ = 108.14(1)°) is build of Tl⁺ cations and [Mo₄O₄Cl₁₄]^2– anions which form tetramers of distorted octahedral, edgesharing (MoOCl₅) units with chlorine atoms in the bridging positions. The oxygen atoms are located in the trans positions of the longest chlorine bridges.     

CuInOVO4 – Einkristalle eines Kupfer(II)‐indiumoxidvanadats durch Oxidation von Cu/In/V‐Legierungen

CuInOVO₄ – Single Crystals of a Copper(II) Indium Oxide Vanadate by Oxidation of Cu/In/V Alloys Red‐brown crystals of the new compound CuInOVO₄ (monoclinic, P2₁/c, a = 879.3(2) pm, b = 615.42(6) pm, c = 1526.2(2) pm, β = 106.69(2)?, Z = 4) were prepared by the reaction of Cu/In/V alloys with oxygen. The investigated crystals were twins by pseudo‐merohedry with a (001) twinning plane. The structure contains isolated Cu₄O₁₈‐groups consisting of trans edge sharing CuO₆‐octahedra. Interconnection of the groups by [In₄O₁₆]‐ribbons running along [010] which are built of edge‐ and corner‐sharing InO₆‐octahedra results in the formation of slabs perpendicular to the c‐axis. The slabs are linked to a threedimensional framework by VO₄^3– groups. The structure may be derived from a cubic closest packing of the oxygen atoms with copper and indium atoms in the octahedral and vanadium atoms in the tetrahedral vacancies.     

Neubestimmung der Kristallstruktur von NbOCl3

NbOCl₃ was obtained from a reaction of NbCl₅ and Nb₂O₅ at 260?C. Contrary to the literature data, NbOCl₃ crystallizes in the non‐centrosymmetric space group P&4macr;2₁m as determined by single‐crystal and powder X‐ray diffraction data (crystal: a = b = 1089.59(6) pm, c = 394.79(2) pm, Z = 4, R₁ = 0.0229, wR₂ = 0.0459, powder: a = b = 1086.36(6) pm, c = 393.65(2) pm). The niobium atoms are surrounded by distorted octahedra built of four chlorine atoms and two oxygen atoms in trans positions. Two such octahedra are edge‐bridged through shared chlorine atoms, forming dimers. These units are linked to each other by apical oxygen atoms forming one‐dimensional Nb₂Cl₆O₂ chains parallel [001]. Contrary to the literature data two different Nb‐O distances are obtained.     

Phase relations in the TlXTl2Se systems (X = Cl,Br, I) and the crystal structure of Tl5Se2I

Each of the quasibinary systems TlClTl₂Se, TlBrTl₂Se, and TlITl₂Se contains a region of solid solution up to 18 mole% Tl₂Se, which decomposes peritectically. The mixed crystals can be explained by a statistical substitution of Se by two I atoms on the fourfold sites of the Tl₂Se lattice. Compounds of the type Tl₅Se₂X were derived by complete substitution. Crystals of Tl₅Se₂I, suitable for a crystal structure determination, were grown by the Bridgman technique. Tl₅Se₂I is tetragonal, $\text{I4}\text{mcm}\text{; a = 866.3}\text{pm}\text{, c = 1346.3}\text{pm}\text{, Z = 4}$. The structure is an ordered variation of the In₅Bi₃ structure and isopuntal to the Cr₅B₃ type. The structure is formed basically by layers of Tl₂Se, in which strings of TlI are introduced. The compounds Tl₅Se₂Br (a = 861.1 pm, c = 1292.2 pm) and Tl₅Se₂Cl (a = 856.5 pm, c = 1273.3 pm) have probably very similar structures. A tendency for immiscibility in the TlXTl₂Se systems is shown by the existence of a miscibility gap in the system TlClTl₂Se and by the endothermic enthalpies of mixing in the system TlBrTl₂Se. In the TlITl₂Se system the compound Tl₆Se₄I system was encountered.     

Die Kristallstruktur von SrCaCrF7

The Crystal Structure of SrCaCrF₇ By solid state reaction of the component fluorides at elevated temperature single crystals of SrCaCrF₇ were obtained (a = 792.3(2), b = 724.7(2), c = 986.1(2) pm; space group Pnma, Z = 4). The X‐ray structure determination confirmed isotypism with the Ca₂AlF₇ type of structure: Isolated octahedra [CrF₆]^3— (mean Cr‐F: 189.7 pm) are opposed by infinitely netted planar cations [SrFCa_2/2]³⁺ which contain “independent” F atoms 3‐coordinated by alkaline earth atoms only. The Sr atoms prefer (at a level of 80%) the 8‐fold, the Ca atoms the 7‐fold coordinated positions between the octahedra.     

Tetrapropylammonium triiodomercurate(II). Structural and vibrational spectra

The crystals of the tetrapropylammonium triiodomercurate(II) are monoclinic, with a = 1775.5(11) pm, b = 1287.4(20) pm, c = 938.9(5) pm and β = 95.52(5)°, Z = 4, space group P2₁/n. The structure was solved by direct methods and refined by least-squares techniques to a conventional R 0.04 for 1520 independent reflections. The structure consists of dimeric HgI₃ units. Each mercury atom is tetrahedrally coordinated to four iodine atoms in such a way that both tetrahedra are linked by sharing an edge. The average mercury—iodine terminal bond distance is 268.7 pm, whereas the bridging distance is 293.2 pm. Far-IR and Raman spectra are also reported and tentatively assigned to D_2h symmetry.     

Crystal Structures of MBi2Br7 (M = Rb,Cs) – Filled Variants of AX7 Sphere Packing

The reinvestigation of the pseudo‐binary systems MBr–BiBr₃ (M = Rb, Cs) revealed two new phases with composition MBi₂Br₇. Both compounds are hygroscopic and show brilliant yellow color. The crystal structures were solved from X‐ray single crystal diffraction data. The isostructural compounds adopt a new structure type in the triclinic space group P$\bar{1}$ . The lattice parameters are a = 755.68(3) pm, b = 952.56(3) pm, c = 1044.00(4) pm, α = 76.400(2)°, β = 84.590(2)°, γ = 76.652(2)° for RbBi₂Br₇ and a = 758.71(5) pm, b = 958.23(7) pm, c = 1060.24(7) pm, α = 76.194(3)°, β = 83.844(4)°, γ = 76.338(3)° for CsBi₂Br₇. The crystal structures consist of M⁺ cations in anticuboctahedral coordination by bromide ions and bromidobismuthate(III) layers ²_∞[Bi₂Br₇]^–. The 2D layers comprise pairs of BiBr₆ octahedra sharing a common edge. The Bi₂Br₁₀ double octahedra are further connected by common vertices. The bismuth(III) atoms increase their mutual distance in the double octahedra by off‐centering so that the BiBr₆ octahedra are distorted. The CsBi₂Br₇ type can be interpreted as a common hexagonal close sphere packing of M and Br atoms, in which 1/4 of the octahedral voids are filled by Bi atoms. The structure type was systematically analyzed and compared with alternative types of common packings. The existence of a compound with the suggested composition CsBiBr₄ could not be verified experimentally.     

Synthese und Strukturuntersuchungen von Iodocupraten (I). XI. Die Kristallstruktur von Tl4Cu2I6

Syntheses and Structure Analyses of Iodocuprates (I). XI. Crystal Structure of Tl₄Cu₂I₆ Tl₄Cu₂I₆ was prepared by melting TlI and CuI or by hydrothermal synthesis in concentratet aqueous HI solution. The crystal structure analysis of Tl₄Cu₂I₆ (orthorhombic, Pnnm, a = 919.6(1), b = 955.2(2), c = 933.6(2) pm, Z = 2) shows that the compound contains dinuclear anions [Cu₂I₆]^4? which are built up by edge sharing CuI₄-tetrahedra. The coordination of Tl^I with I^? is analogous to the yellow TlI.     

Darstellung und Kristallstruktur von SnTl4Se3 mit einer Anmerkung zu TlSe

Preparation and Crystal Structure of SnTl₄Se₃ with a Note on TlSe We describe the preparation and crystal structure of SnTl₄Se₃. It crystallizes as a low symmetric distorted derivative with the In₅Bi₃ type of structure, which itself should be considered as a subfamily of the Cr₅B₃ type of structure: a = 852.2(2) pm, c = 1 272.2(6) pm, c/a = 1.49, Z = 4. Short Sn? Se distances of 311 pm, and 326 pm, respectively, are obtained in [SnSe_2/2] chains running along [001]. Furthermore, short Tl? Se distances are found in quasimolecular bent moieties Tl₂Se: 300 pm, 313 pm, and 347 pm, respectively. SnTl₄Se₃ is a semiconductor. The conductivity of some closely related phases are also reported. Finally, the structure of the well known compound TlSe has been refined for the first time, in order to get some more information about Tl¹⁺? Se distances for square-antiprismatic coordinated Tl¹⁺ ions.     

Polykationische Hg‐Pnictid‐Gerüste mit einer neuen Füllungsvariante in den Strukturen von Hg3As2TlCl3 und Hg3Sb2TlBr3

Polycationic Hg‐Pnictide Frameworks with a Novel Kind of Filling in the Structures of Hg₃As₂TlCl₃ and Hg₃Sb₂TlBr₃ Hg₃As₂TlCl₃ and Hg₃Sb₂TlBr₃ were prepared from mixtures of Hg₂X₂, HgX₂ (X = Cl, Br), As or Sb and Tl in sealed evacuated glass ampoules in temperature gradients 330 °C → 290 °C for Hg₃As₂TlCl₃ (red, transparent crystals) and 290 °C → 260 °C for Hg₃Sb₂TlBr₃ (black crystals). The structures of the diamagnetic compounds were determined based on single crystal X‐ray diffraction data. Both compounds crystallize isotypically in the orthorhombic space group Pbcm with Z = 4 and the lattice constants a = 629.2(5) pm, b = 1234.1(7) pm and c = 1224.8(9) pm for Hg₃As₂TlCl₃ and a = 661.0(4) pm, b = 1311.2(9) pm and c = 1307.1(2) pm for Hg₃Sb₂TlBr₃. The structures can be described either as a cubic closest packing of As₂/Sb₂ dumb‐bells and halide anions with all octahedral interstices filled with Hg²⁺ and Tl⁺, or as a polycationic framework (Hg₃Y₂)²⁺ (Y = As, Sb) consisting of pnictide‐pnictide dumbbells each connected by six Hg atoms to a three dimensional porous arrangement. The centers of the cavities are occupied by Tl⁺ ions which are coordinated by six halide ions in distorted octahedral form. These TlX₆ octahedra share corners in all directions in the motive of the ReO₃ structure type. This new structure type shows a close relationship to the cubic family of compounds of the general formula (Hg₆Y₄)[MX₆]X (Y = As, Sb; M = Mo, Ti, Bi, Sb; X = Cl, Br). The halide ions are connected to the Hg atoms of the polycationic network and to the Tl⁺ ions. Extended Hueckel calculations were used to explain the bonding character of the thallium–halide and mercury–halide bonds.     

Tl2S: Re-Determination of Crystal Structure and Stereochemical Discussion

The crystal structure of synthetic carlinite, Tl₂S, was re-determined by single crystal and powder X-ray diffraction methods. The cell parameters obtained from Rietveld refinement are a=12.150(2) Å, c=18.190(4) Å, V=2325.5(7) ų. A single crystal data refinement proved Tl₂S crystallizing in the trigonal space group R3 with M=440.8gmol⁻¹, Z=27, R=0.076, and wR=0.145. The atomic arrangement found is that of a strongly deformed anti-CdI₂ type, but the deformation is clearly different from that given by previous workers. In the five crystallographically different STl₆ octahedra the S-Tl distances vary between 2.82 and 3.09Å, the Tl-Tl edges between 3.52 and 4.58Å. The common features of these octahedra are (i) each one with a definitely smaller vs larger Tl₃ face in trans-position, both faces parallel or sub-parallel (00.1), and (ii) each three shorter and longer S-Tl distances to the atoms of the larger and smaller Tl₃ faces, respectively. The Tl-Tl contacts between different Tl₂S sheets are on the average definitely shorter than the ones within the sheet and they can be smaller than the Tl-Tl contacts in the small Tl₃ faces of the STl₆ octahedra. The atomic arrangement indicates that the single electron pairs of the monovalent Tl atoms are not arranged all parallel to the z-axis, as one would expect for Tl₂S with an ideal anti-CdI₂ structure. The surrounding of the S atoms resembles that of one-third of the Cl atoms in yellow InCl. The absorbance of Tl₂S is very low at wave numbers approximately <9000 cm⁻¹.     

Röntgenographische Einkristallstrukturbestimmungen an den Kalium-Kupfer(II)-Fluoriden K2CuF4 und K3Cu2F7

X-Ray Single Crystal Structure Determinations of the Potassium Copper(II) Fluorides K₂CuF₄ and K₃Cu₂F₇ With single crystals of the tetragonal compounds K₂CuF₄ (a = 414.7(2), c = 1273(3) pm) and K₃Cu₂F₇ (a = 415.6(3), c = 2052(3) pm), showing no superstructure reflections, crystal structure determinations were based on space group I4/mmm of the K₂NiF₄ and Sr₃Ti₂O₇ type, resp. The shape of F₀-Fourier maxima at the positions of linking fluorine atoms within the layers of octahedra suggested disorder of bridging ligands caused by multidomain structure, which could be refined assuming half occupation of higherfold positions. The results confirmed the Jahn-Teller-distortions of octahedra being elongated with a significant orthorhombic component: Cu? F = 190.9(7)/193.9(2)/223.8(7) pm in K₂CuF₄ (R_W = 0.020) and 190.0(7)/194.7/225.6(7) pm in K₃Cu₂F₇ (R_W = 0.023). In the acentric octahedra of the latter compound the intermediate distance is averaged from the splitted lengths 192.7(4)/196.8(1) pm of axes along the c direction.     

Ein neues Bleistrontiumferrat(III): Die Kristallstruktur der Phase Pb4Sr2Fe6O15

A New Lead Strontium Ferrate(III): The Crystal Structure of the Phase Pb₄Sr₂Fe₆O₁₅ At orthorhombic single crystals of Pb₄Sr₂Fe₆O₁₅ (a = 568.73(8), b = 392.03(4), c = 2107.5(3) pm; Z = 4/3, space group Pnma) a X-ray structure determination has been performed (R₁ = 0,036 for 488 ?observed”? resp. wR₂ = 0,073 for all 643 independent reflexions). It revealed a framework of polyhedra related to perovskite, in which chains of edgesharing pyramids [FeO₅] (average Fe1? O: 197 pm; Fe1? Fe1: 305.5 pm) are linked via apices with corner-sharing [FeO₆] octahedra (Fe2? O: 201 pm). 12–fold, strongly distorted cuboctahedrally coordinated ?perovskite positions”? show mixed occupancy by 2/3 Sr + 1/3 Pb (= Sr2; Sr2? O: 287 pm). More spacy channels, running parallel to the chains of pyramids along [010] of the structure, contain lead atoms only. The double occupancy of the corresponding cages results in short distances Pb1? Pb1 (355.9 pm) and Pb1? Fe2 (314.4 pm), as well as in a very asymmetric [PbO₆] coordination (Pb1? O: 253 pm), in the opposite hemisphere of which the lone electron pair s² is supposed to be located. Details are communicated and structural relations discussed.     

Die Reaktion von SeCl4 mit Übergangsmetalltetrachloriden. Synthese und Kristallstrukturen von (SeCl3)2MCl6 mit M = Zr,Hf, Mo,Re

The Reaction of SeCl₄ with Transition Metal Tetrachlorides. Synthesis and Crystal Structures of (SeCl₃)₂MCl₆ with M = Zr, Hf, Mo, Re The transition metal tetrachlorides ZrCl₄, HfCl₄ and MoCl₄ react with SeCl₄ in closed ampoules at temperatures of 140°C to (SeCl₃)₂MCl₆ (M = Zr, Hf, Mo) which are all isotypic and crystallize in the (SeCl₃)₂ReCl₆ structure type (orthorhombic, Fdd2, Z = 8, lattice constants for M = Zr: a = 1165.7(1)pm, b = 1287.2(2)pm, c = 2180.2(2)pm; for M = Hf: a = 1162.9(2)pm, b = 1285.0(2)pm, c = 2178.2(3)pm; for M = Mo: a = 1153.8(1)pm, b = 1267.7(1)pm, c = 2147.4(2)pm). The Cl^? ions form a hexagonal closest packing with one fourth of the octahedral holes filled by Se⁴⁺ and M⁴⁺ in an ordered way. The MCl₆ octahedra are regular, the SeCl₆ octahedra are distorted with 3 short and 3 long Se? Cl bonds (mean 215 pm and 287 pm). The structures can thus be regarded as built of SeCl₃⁺ and MCl₆^2? ions. Magnetic susceptibility measurements show for M = Zr the expected diamagnetic behavior, for M = Mo and Re paramagnetic behavior according to the Curie-Weiss law with magnetic moments of 2.5 B. M. for M = Mo and 3.7 B. M. for M = Re corresponding to 2 and 3 unpaired electrons respectivly.