Synthese und Kristallstruktur von [C(NMe2)3]2[(CO)4Fe(μ‐InCl2)2Fe(CO)4]

Synthesis and Crystal Structure of [C(NMe₂)₃]₂[(CO)₄Fe(μ‐InCl₂)₂Fe(CO)₄] Treatment of [C(NMe₂)₃]₂[(CO)₄FeInCl₃] ( 1 ) with hot water produces the dinuclear complex [C(NMe₂)₃]₂[(CO)₄Fe(μ‐InCl₂)₂Fe(CO)₄] ( 2 ) which could be crystallized from dichloromethane/pentane. 2 crystallizes in the monoclinic space group P2₁/n with a = 835.7(1), b = 1187.8(1), c = 1902.7(1) pm, β = 91.877(5)° and Z = 2. The anion contains a four‐membered Fe—In—Fe—In ring with octahedral environment at the iron atom and tetrahedral coordination at the In atom.     

Darstellung,Kristallstruktur und quantenchemische Berechnung von [C(NMe2)3]2[(CO)4FeInCl3]

Preparation, Structure, and Quantum Chemical Calculation of [C(NMe₂)₃]₂[(CO)₄FeInCl₃] The title compound ( 1 ) has been obtained as colorless crystals by reacting InCl₃ with [C(NMe₂)₃][(CO)₄FeC(O)NMe₂] in THF solution. The crystal structure determination (monoclinic, C2/c) shows the presence of separate ions with one disordered and one non disordered cation. In the dianion the CO groups of the trigonal bipyramidal coordinated iron atom and the Cl atoms of the tetrahedral coordinated indium atom form a staggered conformation with a relatively short In–Fe bond distance of 252 pm. Quantum Chemical DFT calculations of [CO)₄FeInCl₃]^2– show that the Fe–In bond has a strong ionic character and that it should be considered as an adduct of [Fe(CO)₄]^2– and InCl₃.     

Zur Kristallstruktur von CaFeF5

On the Crystal Structure of CaFeF₅ Single crystals of CaFeF₅ were obtained by heating a mixture of the component fluorides at 860°C for 12 d (a = 549.2(1), b = 1007.6(2), c = 759.9(2) pm, β = 110.02(3)°; space group P2₁/c, Z = 4). The X‐ray structure redetermination of a twinned specimen confirmed the chain structure of octahedra sharing trans corners already known. But the anomalies reported earlier were removed and less distorted [FeF₆] octahedra and [CaF₇] pentagonal bipyramids were found, the distances of which are split within the usual range around mean values of Fe—F: 192.4 and Ca—F: 233.1 pm.     

Synthese und Kristallstruktur von [{(tBu2P)2InCl}2]

Synthesis and Crystal Structure of [{(tBu₂P)₂InCl}₂] The reaction of InCl₃ with tBu₂PSiMe₃ leads to [{(tBu₂P)₂InCl}₂] ( 1 ). 1 crystallizes in the space group P2₁/c. The lattice constants (at 216 K) are: a = 945.9(5) pm, b = 1 604.1(9) pm, c = 1 636.8(8) pm, β = 100.55(4)°. 1 contains a planar In₂P₂ ring. Each In atom is coordinated by two bridging tBu₂P groups, a terminal tBu₂P group and a terminal Cl atom. The coordination geometry of the In atoms is roughly tetrahedral.     

Zur Kristallstruktur von MnF3 und MnPtF6

On the Crystal Structure of MnF₃ and MnPtF₆ Single crystal investigations of MnF₃ (rubyred) confirmed the crystal structure based on powder data [2]: monoclinic, space group C 2/c?C (No. 15) with a = 892.02 pm, b = 504.72 pm, c = 1 347.48 pm, β = 92.64° with Z = 12. The corresponding determination of the crystal structure of MnPtF₆, yellow, confirmed the unit cell [3] with a = 510.47 pm, c = 1 421.0 pm and γ = 120°, Z = 3 space group R 3 -C (No. 148). For both compounds detailed parameters respectively interatomic distances have been obtained.     

Synthese und Kristallstruktur von Ba6ZnIn2Cl20

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].     

Reindarstellung und Kristallstruktur von Lithiumnitridhydrid,Li4NH,Li4ND

Preparation and Crystal Structure of Lithium Nitride Hydride, Li₄NH, Li₄ND Single phase Li₄NH was prepared by the reaction of Li₃N and LiH at 490°C. Its structure has been solved from x-ray and time-of-flight neutron powder diffraction data. Li₄NH crystallizes in an ordered variant of the Li₂O structure. N and H occupy the sites of two interpenetrating “extended” diamond lattices. Li occupies all N₂H₂ tetrahedral voids and is found to be shifted into a N₂H tetrahedral face. As a result H is in compressed tetrahedral coordination by Li, while N is in bisdisphenoidal coordination by Li. Alternatively, the Li₄NH structure may be regarded as a [Li₄N]⁺threedimensional net, its voids being filled up with H^?. Li₄NH is a reactive solid, which decomposes to imide when in contact with N₂ or H₂ at some 400°C.     

Zur Kenntnis der Kristallstruktur von Melem C6N7(NH2)3

On the Crystal Structure of Melem C₆N₇(NH₂)₃ Single crystals of melem ( 1 ) were grown from both DMSO‐solutions and the gas phase. The structure of melem ( 1 ) was solved by single‐crystal X‐ray diffraction (P2₁/c, Z = 4, a = 741.66(15), b = 862.28(17), c = 1335.9(3) pm, β = 99.91(3)° R1 = 0.037 for 1098 reflections). The structure determination by X‐ray powder diffraction, which has been previously conducted, is in agreement with our data. The increased quality of the structural information allows for a more detailed understanding of the hydrogen bonding network.     

Die Kristallstruktur von [InI · C6D6][{(CH3)3Si}3C‐InI3]; ein Nebenprodukt der Umsetzung von InI3 mit basefreiem Li‐C(Si(CH3)3)3

The title compound is formed together with Li[Tsi‐InI₃] (the main product), (Tsi‐In(Me)I)₂ and (Tsi)₂InMe in very low yield in the reaction of InI₃ with Tsi‐Li (Tsi = ‐C(Si(CH₃)₃)₃)in toluene. According to the X‐ray structure determination this compound crystallizes in the triclinic space group P&1marc; and consists of slightly associated dimers of [Tsi‐InI₃]^‐ anions via weak In^I···I(‐In^III) contact‐bonds of 345.6(1) to 373.8(2) pm. Additionally the In^I atom is capped by a D₆‐benzene molecule.     

Zur Kenntnis von LiSi2N3: Synthese und Verfeinerung der Kristallstruktur

On LiSi₂N₃ – Synthesis and Crystal Structure Refinement Single-crystalline LiSi₂N₃ was obtained by the reaction of lithium and silicon diimide under N₂ atmosphere in a radio-frequency furnace at 1300 °C. LiSi₂N₃ is isotypic with Li₂SiO₃ and it crystallizes as an ordered variant of wurtzite. A single-crystal X-ray diffraction analysis (Cmc2₁, a = 922.15(9), b = 529.64(8), c = 477.98(5) pm, Z = 4, R1 = 0.0173, wR2 = 0.0382) confirms and improves the structural data which previously had been obtained from powder diffraction data.     

Zur Kristallstruktur von CuInMo2O8

On the Crystal Structure of CuInMo₂O₈ . Single crystals of CuInMo₂O₈ were prepared and investigated by X-ray work. It shows monoclinic symmetry, space group C—C2/c; a = 9.549 Å, b = 11.529 Å, c = 5.000 Å; β = 91.38(2)°, Z = 4. CuInMo₂O₈ represents a LiYbW₂O₈ related structure, characterised by zigzag-chains of MoO₆-octahedrons and octahedrons around copper and indium. With respect to LiFeW₂O₈ the single and three-valent ions are in opposite distribution. There are strong evidence for molybdenum in lowered oxidation state.     

Die Kristallstrukturen der Hydroxyhalogenide Li4(OH)3Br und Li4(OH)3I

The Crystal Structures of the Lithium Hydroxide Halides Li₄(OH)₃Br and Li₄(OH)₃I Using single crystal analysis and powder diffraction data the crystal structures of the lithium hydroxide halides Li₄(OH)₃Br and Li₄(OH)₃I were solved and refined. Li₄(OH)₃Br crystallises in the space group P2₁/m and is isotypic with the lighter homologue Li₄(OH)₃Cl. (Rietveld‐refinement; T = 293 K; a = 545, 41(1); b = 758, 13(1); c = 650, 20(1) pm; β = 93, 82(1)°; Z = 2; 300 unique reflections; R_p = 0, 106; R_wp = 0, 109; R_exp = 0, 081). Li₄(OH)₃I crystallises in the space group Pmmn in a variant of the LiOH structure in which 1/4 of the hydroxide anions are replaced by iodide anions. (Single crystal analysis; T = 100 K; a = 1029, 5(4); b = 525, 9(2); c = 573, 2(2) pm; Z = 2; 392 unique reflections; R₁ = 0, 0642).     

Die Kristallstruktur von cis‐ und trans‐N‐iso‐Propylamidodimethylindium, [(CH3)2In‐N(H)iC3H7]2

The Crystal Structure of cis‐ and trans‐N‐iso‐Propylamidodimethyl Indium, [(CH₃)₂In‐N(H)ⁱC₃H₇]₂ According to the X‐ray structure determination [(CH₃)₂In‐N(H)ⁱC₃H₇]₂ (prepared from InMe₃ (Me = CH₃) and H₂NⁱPr (ⁱPr = CH(CH₃)₂) crystallizes in the monoclinic space group P2₁/n with 3 dimeric trans as well as 3 dimeric cis isomers per unit cell. The centrosymmetric form has a planar In₂N₂ core with In—N bonds of 222.1(4) and 222.9(5) pm, respectively, the skeleton of the cis isomer with In—N bonds of 221.4(4) pm is slightly folded (13.7°). Some ¹H, ¹³C NMR, IR, and Raman data are reported.     

Die Kristallstruktur von Bortriiodid,BI3

Crystal Structure of Boron Triiodide, BI₃ Boron triiodide as a micro‐crystalline powder was obtained after sublimation of the reaction product of NaBH₄ and iodine. An X‐ray powder diagram of the temperature‐, air‐, and light‐sensitive compound was collected at –73 °C. According to the results of the Rietveld refinement, the crystal structure of BI₃ is isotypic to that of BCl₃ (space group P6₃/m, no. 176, a = 699.09(2), c = 736.42(3) pm). The B–I bond length was determined to be 211.2(8) pm.     

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.     

Zur Kristallstruktur von Li8PbO6 [1]

On the Structure of Li₈PbO₆ For the first time single crystals of Li₈PbO₆ have been prepared by heating of mixtures of Na₂PbO₃ and Li₂O [Ag-cylinders, 650°C, 150 d]. The structure [382 I₀(hkl), four circle diffractometer PW 1100, ω/2Θ-scan, MoKα, R = 3.07%, R_w = 3.00%, space group R3 ; a = 555.09(4), c = 1564.13(17) pm, D_x = 4.28 g · cm^?3, D_pyk = 4.24 g · cm^?3, Z = 3] is characterized by the motive of a hexagonal-closed O^2? packing. Half of the octahedral sites are occupied by Pb⁴⁺ and Li⁺ and half of the tetrahedral sites only by Li⁺. The Madelung Part of Lattice Energy, MAPLE, and the Effective Coordination Numbers, ECoN, these via Mean Fictive Ionic Radii, MEFIR, are calculated.     

Struktur und elektrochemische Untersuchung von Nb3Cl8

Structure and Electrochemical Study of Nb₃Cl₈ The compound Nb₃Cl₈ was synthesized from NbCl₅ and niobium metal in a sealed quartz ampoule at 700 °C. Single crystals, obtained from LiCl melt were used for X‐ray structure determination (space group P 3 m1, Z = 2, lattice parameters a = b = 672.95(7) pm, c = 1223.2(2) pm (at 100 K), R1 = 0.029, wR2 = 0.064 for all independent reflections). Electrical resistivity measurements are reported. Electrochemical intercalation of lithium into the structure of Nb₃Cl₈ was studied.     

Zur Kenntnis von Tripraseodym‐hexanitridotriborat Pr3B3N6: Neue Synthese und Verfeinerung der Kristallstruktur

On Tripraseodymium Hexanitridotriborate Pr₃B₃N₆: New Synthesis and Crystal Structure Refinement Single‐crystalline Pr₃B₃N₆ was obtained by the reaction of praseodymium and BN_x(NH)_y(NH₂)_z in a NaCl melt under N₂ atmosphere in a high‐frequency furnace at 1250 °C. Contrary to literature data, Pr₃B₃N₆ crystallizes in the centrosymmetric space group R 3 c as revealed by single‐crystal X‐ray diffraction (a = 1211.95(9), c = 701.53(7) pm, Z = 6, R1 = 0.0258, wR2 = 0.0658). In the solid, Pr₃B₃N₆ contains Pr³⁺ and planar cyclotrinitridoborate units B₃N₆^9–. The anions represent motifs from the structure of hexagonal boron nitride (h‐BN) and they are stacked analogously along [001]. Both the bond lengths B–N (average value 147.8 pm) and the interionic distances between the anions (350.8 pm) are comparable with the values in h‐BN.     

Zur Kristallstruktur von Ba2ZnO3

On the Crystal Structure of Ba₂ZnO₃ Single crystals of Ba₂ZnO₃ were prepared by solid state reaction. It crystallizes monoclinic: space group C ? C12/c1; a = 5.833; b = 11.376; c = 12.585 Å; β = 93.63°; Z = 8. The crystal structure is characterised by [ZnO₃] chains along [100]. They are connected by Ba²⁺ in seven fold oxygen coordination.