Syntheses and Crystal Structures of a New Niobium Polysulfide K6Nb4S22 and two New Dimorphic Tantalum Polysulfides K6Ta4S22

The new compounds K₆Nb₄S₂₂ and K₆Ta₄S₂₂ ( I ) have been synthesised by the reaction of NbS₂ or Ta metal in a K₂S₃ flux. Using TaS₂ as educt a second modification of K₆Ta₄S₂₂ ( II ) is obtained. K₆Nb₄S₂₂ and K₆Ta₄S₂₂ (form I ) crystallise in the monoclinic space group C2/c with a = 35.634 (2)Å, b = 7.8448 (4)Å, c = 12.1505 (5)Å, β = 100.853 (5)°, V = 3335.8 (3)ų, and Z = 4 for K₆Nb₄S₂₂ and a = 35.563 (7) Å, b = 7.836 (2)Å, c = 12.139 (2)Å, β = 100.56 (3)°, V = 3325.5 (2)ų, and Z = 4 for K₆Ta₄S₂₂ ( I ). The second modification K₆Ta₄S₂₂ (form II ) crystallises in the monoclinic space group P2₁/c with a = 7.5835 (6)Å, b = 8.7115 (5)Å, c = 24.421 (2)Å, β = 98.733 (9)°, V = 1594.6 (2)ų, and Z = 2. The structures consist of [M₄S₂₂]^6— anions composed of two M₂S₁₁ sub‐units which are linked into M₄S₂₂ units via terminal sulfur ligands. The anions are well separated by the K⁺ cations. Differences between the structures of the title compounds and those with the heavier alkali cations Rb⁺ and Cs⁺ are caused by the different arrangement of the [M₄S₂₂]^6— anions around the cations and the different S^2—/S₂^2— binding modes. The thermal behaviour of both modifications was investigated using differential scanning calorimetry (DSC). From these investigations there is no hint for a polymorphic transition between the two forms. After heating crystals of form II above the melting point and cooling the melt to room temperature a crystalline powder of form I can be isolated.     

Synthesis and Crystal Structure of Rb6Ta4S22: The First Tantalum Polysulfide Composed of the Dimeric Complex Anion [Ta4S22]6–

The reaction of Rb₂S₃, Ta and S in a 1.3 : 1 : 5.6 molar ratio at 400 °C yields red‐orange crystals of the new ternary compound Rb₆Ta₄S₂₂ being the first tantalum polysulfide containing the dimeric complex anion [Ta₄S₂₂]^6–. The polysulfide anions are composed of two Ta₂S₁₁ subunits which are linked to Ta₄S₂₂ units via terminal sulfur ligands. The Ta⁵⁺ centers are coordinated by S₂^2– and S^2– ligands according to [(Ta₂(μ₂‐η²,η¹‐S₂)₃(η²‐S₂)(S)₂)₂(μ₂‐η¹,η¹‐S₂)]^6–. Every Ta⁵⁺ ion is surrounded by seven sulfur ions forming a strongly distorted pentagonal bipyramid. In the crystal structure the discrete [Ta₄S₂₂]^6– anions are stacked parallel to the crystallographic b‐axis. The Rb⁺ cations are located between these stacks. Rb₆Ta₄S₂₂ crystallizes in the monoclinic space group P2₁/c (No. 14) with a = 11.8253(9) Å, b = 7.9665(4) Å, c = 19.174(2) Å, β = 104.215(9)°, V = 1751.0(2) ų, Z = 2.     

Crystal Structure of Cesium Dihydrotrifluoride,CsH2F3. Refinement of the Crystal Structures of NMe4HF2 and NMe4H2F3

Single crystals of (NMe₄)(HF₂) were obtained during attempted recrystallization of NMe₄F from fluoroolefin. X‐ray diffraction data show that (NMe₄)(HF₂) crystallizes in the orthorhombic space group Pmmn with unit cell dimensions a = 6.535(2), b = 8.688(3), and c = 5.333(2) Å. The symmetric and virtually linear HF₂ anions exhibit a short F···F distance of 2.256(2) Å. The both crystal structures of (NMe₄)(H₂F₃) (orthorhombic, Pbca, a = 8.509(1), b = 11.273(2), and c = 14.880(2) Å) and CsH₂F₃ (orthorhombic, P2₁2₁2₁, a = 7.345(3), b = 9.126(4), and c = 11.444(4) Å) contain dihydrogentrifluoride anions, H₂F₃^?, which have a bent shape and F···F distances of 2.30‐2.34Å.     

Mononuclear Imido Amido Complexes via Exhaustive Ammonolysis of Niobium and Tantalum Pentachloride with tert‐Butyl Amine

Reaction of MCl₅ (M = Nb, Ta) with excess of ^tBuNH₂ in the presence of pyridine leads to formation of mononuclear complexes [M(N^tBu)(NH^tBu)Cl₂Py₂],M = Nb ( 1 ), Ta ( 2 ). These new key compounds are characterized by ¹H, ¹³C NMR spectroscopy, mass spectrometry and elemental analyses. A single crystal structure analysis of [Ta(N^tBu)(NH^tBu)Cl₂Py₂] ( 2 ) reveals, that surprisingly chloro and not pyridine ligands are trans to the strongest π donor ligands [N^tBu]^2? and [NH^tBu]^?.     

Mixed‐Valent Europium in the Cubic Thiosilicate Li3Eu6[SiS4]4

In an attempt to synthesize LiEu₃S₃[SiS₄] utilizing elemental europium and sulfur as well as SiS₂ and an excess of LiCl as flux and lithium source, dark red, platelet‐shaped single crystals of Li₃Eu₆[SiS₄]₄ were obtained. This new compound crystallizes in the cubic space group I4 3d (a = 1369.22(5) pm) with four formula units per unit cell. Both the Li⁺ and the Si⁴⁺ cations are surrounded by four sulfide anions. The [SiS₄]^4– tetrahedra show merely a slight trigonal distortion, while the [LiS₄]^7– units are best described as flattened bisphenoids. The europium cations exhibit an eightfold, rather irregular coordination environment by eight S^2– anions and have to be regarded mixed‐valent with a +2:+3 charge‐ratio of 5:1 in order to gain electroneutrality. The lack of an inversion center is caused by the [SiS₄]^4– tetrahedra being stacked exclusively top up along [111] in this acentric crystal structure.     

X–ray Single Crystal Structure and Raman Spectrum of Ammonium Hexafluoroarsenate

The structure of ammonium hexafluoroarsenate, NH₄AsF₆, has been determined by X‐ray diffraction using a single crystal grown from saturated solution in anhydrous HF. NH₄AsF₆ crystallizes rhombohedral with the KOsF₆ structure type, with a = 7.459(3) Å, c = 7.543(3) Å (at 200 K), Z = 3, space group (No. 148). No phase transition was observed in the 100 K–296 K temperature range. The structure is dominated by regular AsF₆ octahedra and disordered NH₄⁺ cations. Raman spectrum of a single crystal of NH₄AsF₆ shows the bands at 372 cm^?1, 572 cm^?1, 687 cm^?1 (AsF₆^?) and at 3240 cm^?1 and 3360 cm^?1 (NH₄⁺).     

Synthesis and X‐ray Crystal Structure of Bis[oxamide dioximato‐κ2N,N′](oxamide dioxime‐κ2N,N′)cobalt(III) Perchlorate Hexahydrate

Co(OAc)₂ reacts with oxamide dioxime (H₂oxado) in water in the presence of ClO₄^– ions to produce [Co(Hoxado)₂(H₂oxado)]ClO₄ · 6H₂O ( 1 ), where Hoxado^– is the anion of H₂oxado, derived from the deprotonation of one of the two hydroximinic groups, and in which oxidation of Co^II to Co^III (in air) had occurred. 1 is the first example of a salt in which the cation, [Co(H₂oxado)₃]³⁺, is doubly deprotonated to generate the chiral cation, [Co(Hoxado)₂(H₂oxado)]⁺. The central cobalt cation is pseudo‐octahedrally coordinated by six nitrogen atoms. In the solid state, the complex cations form centro‐symmetric dimers via O–H ··· O bridges. The bulk structure is consolidated by an extended three‐dimensional network of O–H ··· O and N–H ··· O bridges that interconnect the ionic constituents and the water molecules.     

斯蒂芬酸氢铷的制备，晶体结构和热分解机理

A new compound,[RbHTNR]_∞[HTNR:C_6H(NO_2)_3(OH)O],was synthesized by the reaction of rubidium ni-trate and styphnic acid.The molecular structure was characterized using X-ray diffraction analysis,elementalanalysis and FTIR spectroscopy.The crystalline is monoclinic with space group P2_1/n and the empirical formulaC_6H_2N_3O_8Rb.The unit cell parameters are:a=0.4525 nm,b=1.0777 nm,c=1.9834 nm,β=90.47(2)°,V=0.96725 nm~3,Z=4,D_c=2.263 g/cm~3,Mr=329.58,F(000)=640,μ(Mo Kα)=5.165 mm~(-1).The thermal decompo-sition mechanism of the complex was studied by differential scanning calorimetry(DSC),thermogravimetry-derivative thermogravimetry(TG-DTG)and FTIR techniques.At the linear rate of 10 ℃/min,the thermaldecomposition of the complex showed three mass reducing processes between 60 and 500 ℃,and finally evolvedRbCN and some gaseous products.     

Synthesis and Modulated Crystal Structure of KBaNbS4

Single crystals of KBaNbS₄ have been prepared by the reaction of Nb with an in situ formed melt of K₂S₃, BaS, and S at 500 °C. Satellite reflections observed in X‐ray diffraction experiments of these crystals indicate the presence of a one‐dimensional lattice distortion. The modulated structure has been solved and refined from X‐ray data using the superspace group approach. KBaNbS₄ can be described in the (3 + 1)‐dimensional superspace group Pnma(α00)0s0 with lattice parameters a = 9.187(1), b = 7.001(1), and c = 12.494(1) Å and a modulation vector q = (0, 0.629(1), 0). In the structure the NbS₄ tetrahedra are stacked along the a axis and show a slight tilting against each other. The K⁺ and Ba²⁺ ions follow this tilting, both are slightly shifted from their positions in the average structure. The modulation does not lead to a significant change in the coordination spheres of the metal atoms. The small effects of the modulation correspond to the relatively weak intensities of the satellite reflections. Results of temperature dependent X‐ray investigations indicate that K⁺ librates at higher temperatures and the surrounding S^2? anions follow this motion. With decreasing temperature the libration of K⁺ is reduced and the coordination geometry freezes under formation of an incommensurate modulation. The heavier Ba and Nb atoms are also affected by positional modulation of the substructure and accommodate to their environment.     

Synthesis,Crystal Structure,and Thermal Properties of Na5[SnS4]Cl·13H2O

Reaction of Na₂S with SnCl₄ · 5H₂O in aqueous alkaline sodium hydroxide solution leads to the formation of Na₅[SnS₄]Cl · 13H₂O ( 1 ). The compound crystallizes monoclinic in space group P2₁/m with two formula units in the unit cell. In the crystal structure the Na⁺ cations are octahedrally coordinated and are linked into layers by bridging water molecules, μ₃ bridging Cl^– anions and μ_1,1 bridging S atoms of [SnS₄]^4– anions. Extended hydrogen bonding interactions generate a three‐dimensional network. Investigations using differential thermoanalysis, thermogravimetry, and differential scanning calorimetry shows that upon heating in open crucibles the water can be removed leading to the formation of the anhydrate that is stable at room temperature and does not transform back into compound 1 . Storage of the anhydrate in a desiccator over a water atmosphere leads first to formation of Na₄SnS₄ · 14H₂O followed by crystallization of the title compound. After longer storage times NaCl appears as a second crystalline phase. If the thermal measurements are performed in a self‐produced atmosphere, compound 1 transforms partly into Na₄SnS₄ · 14H₂O with an increasing amount of this phase with increasing temperature. Synthetic investigations reveal that crystallization of compound 1 sensitively depends on the water content of acetone, which is used for precipitation of 1 . Reacting Na₄SnS₄ · 14H₂O directly with NaCl afforded formation of complex mixtures.     

Cellular Synthesis and X‐ray Crystal Structure of a Designed Protein Heterocatenane

Herein, we report the biosynthesis of protein heterocatenanes using a programmed sequence of multiple post‐translational processing events including intramolecular chain entanglement, in situ backbone cleavage, and spontaneous cyclization. The approach is general, autonomous, and can obviate the need for any additional enzymes. The catenane topology was convincingly proven using a combination of SDS‐PAGE, LC‐MS, size exclusion chromatography, controlled proteolytic digestion, and protein crystallography. The X‐ray crystal structure clearly shows two mechanically interlocked protein rings with intact folded domains. It opens new avenues in the nascent field of protein‐topology engineering.     

Synthesis and Approximated Crystal and Electronic Structure of a Proposed New Tantalum Oxide Nitride Ta3O6N

In the quasibinary system Ta₂O₅/Ta₃N₅ we prepared a new oxide nitride phase, Ta₃O₆N, by the reaction of 1T–TaS₂ with water‐saturated ammonia gas. The determination of the unit cell metric and the crystal structure indicated that Ta₃O₆N is structurally related to the TiNb₂O₇‐type. Quantum‐chemical calculations on DFT level were used to rank the relative stabilities of possible N/O distributions and to provide a plausible structural model of the ground state with a minimum in the total energy. In agreement with Paulings 2nd rule, nitrogen ions prefer sites with high coordination numbers.     

Organometallic Niobium and Tantalum Complexes with Primary Phosphine Ligands: Syntheses and Molecular Structures of [Cp*MCl4(PH2R)] (M = Nb,Ta; Cp* = C5Me5;R = But,Ad, Cy,Ph, 2, 4, 6‐Me3C6H2 (Mes))

The reaction of [Cp*MCl₄] (M = Nb, Ta; Cp* = C₅Me₅) with PH₂R in toluene at room temperature gives the primary phosphine complexes [Cp*MCl₄(PH₂R)] [Cp* = C₅Me₅; M = Nb: R = Bu^t ( 1a ), Ad ( 2a ), Cy ( 3a ), Ph ( 4a ), 2, 4, 6‐Me₃C₆H₂ (Mes) ( 5a ); M = Ta: R = Bu^t ( 1b ), Ad ( 2b ), Cy ( 3b ), Ph ( 4b ), Mes ( 5b )] in high yield. 1—5 were characterized spectroscopically (NMR, IR, MS) and by crystal structure determinations. The starting material [Cp*TaCl₄] is monomeric in the solid state, as shown by crystal structure determination.     

Magnetic Anisotropy of Dichlorobis(η5‐cyclopentadienyl) Complexes of Vanadium,Niobium, and Tantalum

Abstract. The magnetic behavior of the mononuclear nd¹ systems MCp₂Cl₂ (M = V⁴⁺[3d¹], Nb⁴⁺[4d¹], Ta⁴⁺[5d¹], space group P2₁/c, pseudosymmetry of the molecules C_2v) deviates from pure single ion spin magnetism on account of ligand field effect (H_lf), spin‐orbit coupling (H_so), and intermolecular spin‐spin exchange interactions (H_ex). For both VCp₂Cl₂ and NbCp₂Cl₂ excellent adaptations to the measured susceptibility data were obtained (2 K ≤ T ≤ 300 K) on the basis of spectroscopic data (lf, so) and cooperative metal–metal interactions (ex) of antiferromagnetic nature [molecular field model (mf)]. For TaCp₂Cl₂ experimental term structure data are not available. Therefore, Jørgensen's spectroscopical series (g‐factor of the central ion) was applied to extrapolate the data set for TaCp₂Cl₂. H_lf, H_so, and H_ex (antiferromagnetic) increase in the order 3d¹ → 4d¹ → 5d¹ leading, with rising atomic number of the metals, to a distinct enhancement of the magnetic anisotropy. At 4 K the μ_eff components μ_eff,y (oriented perpendicular to the cg–M–cg plane; “cg” = center of gravity of the Cp ring), μ_eff,z (oriented along the twofold pseudoaxis), and μ_eff,x are 1.73, 1.69, 1.68 (V), 1.73, 1.62, 1.59 (Nb), and 1.71, 1.59, 1.49 (Ta). While μ_eff,y is independent of T, both μ_eff,z and μ_eff,x decrease with decreasing T.     

Preparation and Crystal Structure of Li4[TaN3]

The new lithium nitridotantalate(V), Li₄[TaN₃], was prepared by reaction of Li₁₅[CrN₄]₂N with the wall of a welded Ta ampoule in the presence of metallic Li at 1470 K. Li₄[TaN₃] forms colourless single crystals (platelets, space group Ibca, No. 73, a = 491.85(4) pm, b = 973.59(6) pm, c = 1415.0(1) pm, Z = 8, R1 = 0.0288). The crystal structure is described as Li₂O superstructure with ordered occupation of the tetrahedral sites by Li and Ta. The resulting arrangement leads to infinite chains [TaN₂N_2/2^4—] running along [100].     

Tantalum Clusters in Oxidic Matrices — Synthesis,Crystal Structure and Magnetic Properties of Eu1.83Ta15O32

The mixed‐valent oxotantalate Eu_1.83Ta₁₅O₃₂ 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, R_F = 0.027 for I > 2σ (I). The structure is isotypic to Ba₂Nb₁₅O₃₂. The salient feature is a [Ta(+8/3)₆O₁₂ⁱO₆^a] 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 Eu_1.83Ta₁₅O₃₂ 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 M_mol/(N_Aμ_B) 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 μ_B for free Eu (2+) ions with 4f⁷ configuration in ⁸S_7/2 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.     

Three Salts Containing the Fullerene Tetra‐Anion C604– – Synthesis,X‐Ray Single‐Crystal Structure Determination and EPR Investigation

A synthesis for four‐fold negatively charged fullerides in solution is presented. Three salts containing discrete C₆₀^4– anions were synthesized by the reduction of C₆₀ in solution using rubidium‐mercury amalgams and rubidium suboxide both in the presence of elemental mercury. The three new salts, [Rb₆DMF₁₄(C₆H₁₃N₂O₂)₂] · C₆₀ ( 1 ), [Rb(diaza‐18‐crown‐6)]₄ · C₆₀ · (en)_4.1 ( 2 ), and [Rb(benzo‐18‐crown‐6)]₄ · C₆₀ ( 3 ), were characterized by single‐crystal X‐ray diffraction. The results clearly indicate a charge of 4– for the fulleride anions. In 1 the fulleride units are ordered, and their distortion from I_h symmetry shows similarities to binary alkali metal fullerides that contain C₆₀^4– anions. In the crystal structures of 2 and 3 the C₆₀^4– anions show a rotational disorder. In all structures the 6:6 bond lengths within the fulleride are strongly enlarged compared to the ones in neutralC₆₀. EPR measurements reveal a singlet state for the C₆₀^4– anion.     

Crystal Structure,Characterization, and Luminescence Properties of Mn4+-Doped K3Nb2O4F5

In this paper, we present the high-pressure/high-temperature synthesis and characterization of the potassium fluoridooxidoniobate K₃Nb₂O₄F₅. Single-crystal analysis revealed that the phase crystallizes in the trigonal space group m (hR18) with a=5.799(2), c=21.371(4) Å, V=622.4(4) ų and Z=3 at T=299 K exhibiting a structure type closely related to that of Ba₂RbFe₂F₉. The assignment of the anion positions to oxygen and fluorine is based on crystallographic data and BLBS/CHARDI calculations. Further characterization via EDX spectroscopy was carried out, corroborating the ratio of K to Nb. Doping of the title compound with Mn⁴⁺ was achieved in a secondary step using a ball-mill, resulting in a red phosphor material, which was additionally analyzed by luminescence spectroscopy. The emission maximum is located at λ_max=630 nm.