Trichloroberyllat‐Komplexe von Dimethylcyanamid,Morpholin und 4,4′‐Bipyridin

Trichloroberyllate Complexes of Dimethyl Cyanamide, Morpholine, and 4,4′‐Bipyridine The trichloroberyllate complexes (Ph₄P)[BeCl₃(NCNMe₂)] ( 1 ), (Ph₄P)[BeCl₃{HN(CH₂)₄O}] ( 2 ), and (Ph₄P)₂[(BeCl₃)₂(4,4′‐bipy)] ( 3 ) were prepared by reactions of (Ph₄P)₂[Be₂Cl₆] with dimethyl cyanamide, trimethylsilylmorpholinate, and 4,4′‐bipyridine, respectively, in dichloromethane solutions. 1 ‐ 3 were characterized by X‐ray crystallography and by IR‐spectroscopy. 1 ·CH₂Cl₂: Space group P1, Z = 1, lattice dimensions at 173 K: a = 714.2(1), b = 919.5(2), c = 1233.4(2) pm, α = 94.97(1)°, β = 90.86(1)°, γ = 111.90(1)°, R₁ = 0.0310. In the complex anion [BeCl₃(NCNMe₂)]^? the dimethyl cyanamide ligand is coordinated via a linear Be–N≡C‐NMe₂ arrangement, the CH₂Cl₂ molecules forming linear chains by hydrogen bridges ···HCH···Cl··· with the chlorine atoms of the {BeCl₃^?} groups. 2 : Space group , Z = 2, lattice dimensions at 173 K: a = 1050.9(1), b = 1099.7(1), c = 1308.3(2) pm, α = 87.57(1)°, β = 70.97(1)°, γ = 74.58(1)°, R₁ = 0.0397. The complex anions are dimerized by centrosymmetric puckered eight‐membered [Be–N–H···Cl]₂ rings. 3 ·2CH₂Cl₂: Space group , Z = 2, lattice dimensions at 173 K: a = 1095.4(1), b = 1559.6(2), c = 1869.8(3) pm, α = 79.12(1)°, β = 73.83(1)°, γ = 78.76(1)°, R₁ = 0.0548. The complex contains dianions [Cl₃Be(μ‐bipy)BeCl₃]^2? with Be–N distances of 177.0(6) and 178.5(6) pm. Both {BeCl₃}^? groups form C–H···Cl hydrogen bridges with the dichloromethane molecules.     

Chloroberyllate mit Stickstoff‐Donorliganden. Die Kristallstrukturen von (Ph4P)[BeCl3(Py)], (Ph4P)2[(BeCl3)2(TMEDA)], (Ph4P)[BeCl2{(Me3SiN)2CPh}] und (Ph4P)2[BeCl4] · 2CH2Cl2

Chloroberyllates with Nitrogen Donor Ligands. Crystal Structures of (Ph₄P)[BeCl₃(py)], (Ph₄P)₂[(BeCl₃)₂(tmeda)], (Ph₄P)[BeCl₂{(Me₃SiN)₂CPh}], and (Ph₄P)₂[BeCl₄] · 2CH₂Cl₂ The title compounds were obtained as colourless, moisture sensitive crystals by reactions of (Ph₄P)₂[Be₂Cl₆] with pyridine, tmeda (N, N′‐tetramethylethylendiamine), or with the silylated benzamidine PhC—[N(SiMe₃)₂(NSiMe₃)], whereas the tetrachloro beryllate was isolated as a by‐product from a solution in dichloromethane in the presence of the silylated phosphaneimine Me₃SiNP(tol)₃. All compounds were characterized by crystal structure determinations and by IR spectroscopy. (Ph₄P)[BeCl₃(Py)] ( 1 ): Space group Pbcm, Z = 4, lattice dimensions at 193 K: a = 756.2(1), b = 1739.2(2), c = 2016.3(2) pm, R₁ = 0.0626. The complex anion contains tetrahedrally coordinated beryllium atom with a Be—N distance of 176.5 pm. (Ph₄P)₂[(BeCl₃)₂(tmeda)]·2CH₂Cl₂ ( 2 ·2CH₂Cl₂). Space group P1¯, Z = 1, lattice dimensions at 193 K: a = 1072.7(1), b = 1132.6(1), c = 1248.9(1) pm, α = 95.34(1)°, β = 92.80(1)°, γ = 90.81(1)°, R₁ = 0.0344. Both nitrogen atoms of the tmeda molecule coordinate with BeCl₃^— units forming the centrosymmetric complex anion with Be—N distances of 181.3 pm. (PPh₄)[BeCl₂{(Me₃SiN)₂CPh}] ( 3 ). Space group C2, Z = 2, lattice dimensions at 193 K: a = 1255.4(2), b = 1401.9(2), c = 1085.2(2) pm, R₁ = 0.0288. In the complex anion the benzamidinato ligand {(Me₃SiN)₂CPh}^— acts as chelate with Be—N distances of 174.9 pm. (Ph₄P)₂[BeCl₄]·2CH₂Cl₂ ( 4 ·2CH₂Cl₂). Space group P2/c, Z = 4, lattice dimensions at 193 K: a = 2295.4(1), b = 982.5(1), c = 2197.2(2) pm, β = 99.19(1)°, R₁ = 0.0586. 4 ·2CH₂Cl₂ contains nearly ideal tetrahedral [BeCl₄]^2— ions, like the previously described 4 ·2, 5CH₂Cl₂, which crystallizes in the space group P1¯, with Be—Cl distances of 203.4 pm on average.     

Über Reaktionen von Hexachlorodiberyllat mit Trimethylsilyl‐N‐dimethylamid. Die Kristallstrukturen von (Ph4P)3[Be2Cl5(OSiMe3)][BeCl3(Me2NSiMe3)], (Ph4P)[BeCl3(HNMe2)] und (Ph4P)(H2NMe2)[BeCl4]

On Reactions of Hexachlorodiberyllate with Trimethylsilyl‐N‐dimethylamide. Crystal Structures of (Ph₄P)₃[Be₂Cl₅(OSiMe₃)][BeCl₃(Me₂NSiMe₃)], (Ph₄P)[BeCl₃(HNMe₂)], and (Ph₄P)(H₂NMe₂)[BeCl₄] Reactions of bis‐tetraphenylphosphonium hexachlorodiberyllate, (Ph₄P)₂[Be₂Cl₆], with trimethylsilyl‐N‐dimethylamide under different conditions lead to the novel chloroberyllate derivatives (Ph₄P)₃[Be₂Cl₅(OSiMe₃)][BeCl₃(Me₂NSiMe₃)] ( 1 ), (Ph₄P)[BeCl₃(HNMe₂)] ( 2 ), and (Ph₄P)(H₂NMe₂)[BeCl₄] ( 3 ). 1 ‐ 3 were characterized by IR spectroscopy and crystal structure determinations. 1· 4CH₂Cl₂: Space group P1¯, Z = 2, lattice dimensions at 193 K: a = 1115.6(1), b = 2110.7(2), c = 2145.0(3) pm, α = 71.38(1)°, β = 85.66(1)°, γ = 85.24(1)°, R₁ = 0.0732. The [Be₂Cl₅(OSiMe₃)]^2— ion in the structure of 1 is derived from the [Be₂Cl₆]^2— ion by substitution of a μ‐Cl ligand by the oxygen atom of the (OSiMe₃)^— group. The second anion, [BeCl₃(Me₂NSiMe₃)]^—, can be described as donor acceptor complex with a short Be—N bond of 179(1) pm. 2 : Space group P1¯, Z = 2, lattice dimensions at 193 K: a = 1063.1(1), b = 1072.0(1), c = 1238.3(1) pm, α = 87.55(1)°, β = 74.86(1)°, γ = 69.73(1)°, R₁ = 0.0299. The anion of 2 forms a centrosymmetric dimer [BeCl₃(HNMe₂)]₂^2— via N—H···Cl bridges of the two donor acceptor complex units with Be—N separations of 175.2(2) pm. 3 : Space group Pbca, Z = 8, lattice dimensions at 193 K: a = 926.9(1), b = 2164.7(1), c = 2732.7(1) pm, R₁ = 0.0495. The structure of 3 contains centrosymmetric ion quadrupoles [(Me₂NH₂)(BeCl₄)]₂^2— forming by N—H···Cl bridges between (Me₂NH₂)⁺ and [BeCl₄]^2— ions.     

[Be(OH2)4]Cl2 – Herstellung,IR‐Spektrum und Kristallstruktur

[Be(OH₂)₄]Cl₂ – Preparation, IR spectrum, and Crystal Structure Single crystals of [Be(OH₂)₄]Cl₂ were prepared by the reaction of thionyl chloride at 20 °C with samples which result from evaporated, HCl containing, aqueous solutions of BeCl₂. With excess of boiling thionyl chloride BeCl₂ is formed. [Be(OH₂)₄]Cl₂ is characterized by IR spectroscopy and by X‐ray crystal structure determination: Space group P2₁/c, Z = 4, lattice dimensions at 193 K: a = 653.53(5), b = 1298.15(14), c = 789.52(6) pm, β = 103.005(9)°, R1 = 0.027. The structure consists of slightly distorted tetrahedral [Be(OH₂)₂]²⁺ ions, which are connected with the chloride ions via nearly linear O–H···Cl hydrogen bonds to give a 3D network.     

Phosphanimin‐ und Phosphaniminato‐Komplexe von Beryllium. Kristallstrukturen von [BeCl2(HNPPh3)2], [BeCl(HNPPh3)2(Py)]Cl und [Be3Cl2(NPPh3)4]

Phosphanimine and Phosphoraneiminato Complexes of Beryllium. Crystal Structures of [BeCl₂(HNPPh₃)₂], [BeCl(HNPPh₃)₂(Py)]Cl, and [Be₃Cl₂(NPPh₃)₄] Tetraphenylphosphonium hexachlorodiberyllate, (Ph₄P)₂[Be₂Cl₆], reacts with lithium phosphoraneiminate, [LiNPPh₃]₆, in dichloromethane to give the three‐nuclear beryllium phosphoraneiminate [Be₃Cl₂(NPPh₃)₄] ( 3 ). As a by‐product the phosphaneimine complex [BeCl₂(HNPPh₃)₂] ( 1 ) can be isolated, which reacts with pyridine to give the ionic complex [BeCl(HNPPh₃)₂(Py)]Cl ( 2 ). On the other hand, the silylated phosphanimine Me₃SiNP(p‐tolyl)₃ ( 5 ) does not react with BeCl₂ or (Ph₄P)₂[Be₂Cl₆] forming the expected phosphoraneiminates. From CH₂Cl₂ solutions only the amino‐phosphonium salt [(C₇H₇)₃PNH₂]Cl ( 4 ) can be obtained. The compounds 1 ‐ 5 are characterized by single X‐ray analyses and by IR spectroscopy. 1 ·C₇H₈: Space group C2/c, Z = 4, lattice dimensions at 193 K: a = 1408.9(2), b = 1750.9(2), c = 1633.2(2) pm, β = 106.50(1)°; R₁ = 0.0385. 1 forms a molecular structure with short Be—N distances of 169.8(3) pm. 2 ·Py: Space group P1¯, Z = 4, lattice dimensions at 193 K: a = 969.5(1), b = 2077.1(2), c = 2266.4(2) pm, α = 72.24(1)°, β = 87.16(1)°, γ = 77.42(2)°, R₁ = 0.0776. 2 forms ion pairs in which the NH atoms of the phosphaneimine ligands act as hydrogen bridges with the chloride ion. The HNPPh₃ ligand realizes short Be—N bonds of 169.0(6) pm, the Be—N distance of the pyridine molecule is 182.5(6) pm. 3 ·3CH₂Cl₂: Space group P1¯, Z = 2, lattice dimensions at 193 K: a = 1333.2(2), b = 1370.2(2), c = 2151.8(3) pm, α = 107.14(1)°, β = 91.39(1)°, γ = 105.15(1)°, R₁ = 0.0917. The structure of the three‐nuclear molecule 3 corresponds with a Be²⁺ ion which is tetrahedrally coordinated by the nitrogen atoms of two {ClBe(NPPh₃)₂}^— chelates. 4 ·CH₂Cl₂: Space group P2₁/c, Z = 4, lattice dimensions at 193 K: a = 1206.6(2), b = 1798.0(2), c = 1096.2(1) pm, β = 97.65(1)°, R₁ = 0.0535. 4 forms dimeric units in which the NH₂ groups of the [(C₇H₇)₃PNH₂]⁺ cations act as hydrogen bridges with the chloride ions to give centrosymmetric eight‐membered rings. 5 : Space group P2₁/n, Z = 4, lattice dimensions at 193 K: a = 1074.3(2), b = 2132.2(3), c = 1075.5(2) pm, β = 110.68(1)°, R₁ = 0.0664. 5 forms molecules with distances PN of 154.6(3), SiN of 168.8(3) pm, and bond angle SiNP of 134.4(2)°.     

Polymere,bandförmige Tellurkationen in den Strukturen des Chloroberyllats Te7[Be2Cl6] und des Chlorobismutats (Te4)(Te10)[Bi4Cl16]

Polymeric, Band Shaped Tellurium Cations in the Structures of the Chloroberyllate Te₇[Be₂Cl₆] and the Chlorobismutate (Te₄)(Te₁₀)[Bi₄Cl₁₆] Te₇[Be₂Cl₆] is obtained at 250 °C in an eutectic Na₂[BeCl₄] / BeCl₂ melt from Te, TeCl₄ und BeCl₂ in form of black crystals, which are sensitive towards hydrolysis in moist air. (Te₄) (Te₁₀)[Bi₄Cl₁₆] is prepared from Te, TeCl₄ und BiCl₃ by chemical vapour transport in sealed evacuated glass ampoules in a temperature gradient 150 ° → 90 °Cin form of needle shaped crystals with a silver lustre. The structures of both compounds were determined based on single crystal X‐ray diffraction data (Te₇[Be₂Cl₆]: orthorhombic, Pnnm, Z = 2, a = 541.60(3), b = 974.79(6), c = 1664.4(1) pm; (Te₄)(Te₁₀)[Bi₄Cl₁₆]: triclinic, P1¯, Z = 2, a = 547.2(3), b = 1321.1(7), c = 1490(1) pm, α = 102.09(5)°, β = 95.05(5)°, γ = 96.69(4)°). The structure of Te₇[Be₂Cl₆] consists of one‐dimensional polymeric cations (Te₇²⁺)_n which form folded bands and of discrete [Be₂Cl₆]^2— anions which form double tetrahedraconnected by a common edge. By a different way of folding compared with the cations present in the structures of Te₇[MOX₄]X (M = Nb, W; X = Cl, Br) the (Te₇²⁺)_n cation in Te₇[Be₂Cl₆]represents a new, isomeric form. The structure of (Te₄)(Te₁₀)[Bi₄Cl₁₆] contains two different polymeric cations. (Te₁₀²⁺)_n consists of planar Te₁₀ groups in the form of three corner‐sharing Te₄ rings connected to folded bands. (Te₄²⁺)_n forms in contrast to the so far notoriously observed discrete, square‐planar E₄²⁺ ions a chain of rectangular planar Te₄ rings (Te—Te 274 and 281 pm) connected by Te‐Te bonds of 297 pm. [Bi₄Cl₁₆]^4— has a complex one‐dimensional structure of edge‐ and corner‐sharing BiCl₇ units.     

Phosphanimin‐Komplexe des Berylliums und Phosphaniminato‐Komplexe mit Heterokubanstruktur

Phosphaneimine Complexes of Beryllium and Phosphoraneiminato Complexes with Heterocubane Structure Beryllium dichloride reacts with the silylated phosphaneimine Me₃SiNPEt₃ in dichloromethane solution to give the monomeric donor‐acceptor complex [BeCl₂(Me₃SiNPEt₃)] ( 1 ). Under cleavage of trimethylchlorosilane the thermolysis of 1 at 160 °C leads to the formation of the phosphoraneiminato complex [BeCl(μ₃‐NPEt₃)]₄ ( 2 ) with heterocubane structure. In the presence of BeCl₂ 1 reacts in the melt to give the phosphoraneiminato complex [Be₄Cl₄(μ₃‐Cl)(μ₃‐NPEt₃)₃] ( 3 ), the structure of which corresponds with the structure of 2 by substitution of a ligand (μ₃‐NPEt₃)^— by a μ₃‐chloro ligand. As a by‐product from the synthesis of 2 in dichloromethane solution the phosphaneimine complex [BeCl₂(μ‐HNPEt₃)]₂·CH₂Cl₂ ( 4 ·CH₂Cl₂) can be obtained. Its dimeric units form dimers [{BeCl₂(μ‐HNPEt₃)}₂]₂ with symmetry D₂ via Cl···H‐N hydrogen bridges. The compounds 1 — 4 ·CH₂Cl₂ are characterized by X‐ray structure determinations, 1 — 3 additionally by IR spectroscopy. 1 : Space group C2/c, Z = 8, lattice dimensions at 193 K: a = 1502.5(1), b = 801.8(1), c = 2609.6(2) pm, β = 96.15(1)°, R₁ = 0.0523. 2 : Space group C2/c, Z = 4, lattice dimensions at 193 K: a = 1992.2(2), b = 1054.8(1), c = 1950.6(2) pm, β = 114.82(1)°, R₁ = 0.0275. 3 : Space group P2₁2₁2₁, Z = 4, lattice dimensions at 193 K: a = 1159.5(1), b = 1199.0(1), c = 2251.1(2) pm, R₁ = 0.0399. 4 ·CH₂Cl₂: Space group Ccca, Z = 8, lattice dimensions at 193 K: a = 1454.6(1), b = 2795.7(3), c = 1235.6(1) pm, R₁ = 0.0349.     

Untersuchungen an Natriumtrifluormethylsulfonat – Kristallstruktur und Phasenumwandlung des Monohydrats und Natriumionenleitfähigkeit des wasserfreien Salzes

Studies on Sodium Trifluormethanesulfonate – Crystal Structure and Phase Transition of Sodium Trifluormethanesulfonate Monohydrate and Sodium Ion Conductivity of Anhydrous Sodium Trifluormethanesulfonate According to the results of temperature dependent powder diffractometry (Guinier-Simon-technique) sodium trifluormethanesulfonate monohydrate is dimorphous. The phase transition occurs at ?35°C. The room-temperature modification crystallizes monoclinic in space group P2₁/c with the lattice parameters a = 941.6(5) pm, b = 654.3(2) pm, c = 1062.4(5) pm and β = 107.73(2)°. The crystal structure consists of double layers of trifluormethanesulfonate anions, the lipophilic CF₃-groups pointing at each other. Sodium is coordinated by four oxygen atoms from four different anions and by two molecules of crystal water. The resulting polyhedron may be addressed as a distorted octahedron. The low-temperature modification crystallizes orthorhombic in space group Pnma with the lattice parameters a = 645.31(9) pm, b = 538.03(9) pm, c = 1745.3(3) pm. The loss of crystal water occurs at 136°C. Anhydrous sodium trifluormethanesulfonate shows a phase transition at 252°C. The high-temperature modification is a good sodium ionic conductor (σ = 4.1 · 10^?1 Ω^?1 cm^?1 at 250°C).     

Chloro‐N′,N′‐dimethylformamidinium‐(dimethylcyanamid)trichloroberyllat, [Me2NC(Cl)NH2]+[BeCl3(NCNMe2)]−

Chloro‐N′,N′‐dimethylformamidinium‐(dimethylcyanamide)trichloroberyllate, [Me₂NC(Cl)NH₂]⁺[BeCl₃(NCNMe₂)]^? Chloro‐N′,N′‐dimethylformamidinium‐(dimethylcyanamide)trichloroberyllate, [Me₂NC(Cl)NH₂]⁺[BeCl₃(NCNMe₂)]^? was prepared from BeCl₂ with two equivalents of dimethylcyanamide in CH₂Cl₂ suspension. The compound was characterized by X‐ray crystallography and by IR spectroscopy. Space group , Z = 2, lattice dimensions at 193 K: a = 620.7(1), b = 744.9(2), c = 1520.3(3) pm, α = 96.87(2)°, β = 100.41(2)°, γ = 100.17(2)°, R₁ = 0.0443. Cations and anions form N–H…Cl hydrogen bridges along [010].     

Ca3Cl2CBN,eine Verbindung mit dem neuen Anion CBN4−

Ca₃Cl₂CBN, a Compound with the New CBN^4? Unit The new compound Ca₃Cl₂CBN was obtained from the reaction of Ca and CaCl₂ with CaCN₂, B and C or with BN and C, in sealed tantalum containers at 900°C. The crystal structure is related with the structure of Ca₃Cl₂C₃ whereas the C₃^4? units (C_2v symmetry) are substituted by isoelectronic CBN^4? anions (C_s symmetry): Ca₃Cl₂CBN, Pnma, a = 1 386.7(9) pm, b = 384.7(3) pm, c = 1 124.7(6) pm, Z = 4; R = 0.055, R_w = 0.036 for 380 independent intensities. The CBN^4? units are located between layers of Ca²⁺ that are interconnected by Cl^?. The bond angle (C? B? N) is 176° and bond distances are d_{C? B} = 144 pm and d_{B? N} = 138 pm, respectively.     

(PPh4)2[V2Cl9][VCl5] · CH2Cl2 Synthese,IR-Spektrum und Kristallstruktur

(PPh₄)₂[V₂Cl₉][VCl₅] · CH₂Cl₂. Synthesis, I.R. Spectrum, and Crystal Structure The title compound was obtained by addition of CCl₄ to a solution of PPh₄Cl and excess VCl₄ in CH₂Cl₂. It forms black crystals which are light and moisture sensitive. The i.r. spectrum is reported. The crystal structure was determined by X-ray diffraction (3044 independent reflexions, R = 0.063). Crystal data: triclinic, space group P1 , Z = 2, a = 1186, b 1325, c = 1995 pm, α 97.5, β 105.6°, γ 93.4°. The structure consists of PPh₄⁺ cations, V₂Cl₉? and VCl₅? anions and CH₂Cl₂ molecules. The V₂Cl₉? ions consist of face-sharing octahedra with a long V…?V distance of 333 pm; the VCl₅? ions form nearly ideal trigonal bipyramids with V? Cl bonds of 228 pm (axial) and 218 pm (equatorial). Both anions deviate only marginally from D_3h symmetry. Half of the cations is arranged to (PPh₄⁺)₂ pairs about inversion centers.     

LiTiCl3: Synthesis and thermal behaviour

LiTiCl₃ is obtained as one example within an ample solid solution, Li_24–2nTi_nCl₂₄ (?4?n?10), by synpropotionation of TiCl₃ and Ti in the presence of LiCl (2:1:3 molar ratio) in sealed tantalum tubes at 750°C. It crystallizes with the inverse spinel-type structure according to (Li_0.67)^[4](Li_0.67Ti_1.33)^[4]Cl₄ with, at 25°C, a = 1048.62(4) pm, space group Fd3m. Thermal expansion is linear with α = 4.85 × 10^?5K^?1 up to about 300°C and thereafter, when the migration of Li⁺ from tetrahedral to octahedral interstices becomes increasingly important, it exhibits a relative decrease resulting, finally, in the phase transition to a NaCl-type structure that is observed for the first time at about 575°C.     

Darstellung der Dichlormethyleniminium-Salze Cl2CNClH+ MF6− und Cl2CNClCH3+ MF6− (M = As,Sb) und Kristallstruktur von Dichlormethyleniminiumhexachloroantimonat Cl2CNH2+SbCl6−

Synthesis of the Dichloromethyleneiminium Salts Cl₂C?NClH⁺MF₆^? and Cl₂C?NClCH₃⁺ MF₆^? (M = As, Sb) and Crystal Structure of Dichloromethyleneiminium-hyxachloroantimonate Cl₂C?NH₂⁺SbCl₆^? The N-chloro-dichloromethyleneiminium salts Cl₂C=NCIH⁺MF₆^? (M = As, Sb) are prepared by protonationof trichloromethyleneimine in the superacide system HF/MF5 at 195 K. The synthesis of the N-chloro-N-methyl-dichloromethyleneiminium salts Cl₂C?NClCH₃⁺MF₆^? (M = As, Sb) is proceeded by methylation of perchloromethylenimine by CH₃OSO⁺MF₆^? in SO₂ also at low temperature. All salts are characterized by vibrational and NMR spectra. The dichloromethyleneiminiumhexachloroantimonate crystallizes in the space group P2₁/c with a = 971.3(4)pm, b = 1134.0(4)pm, c = 2154.2(7)pm β = 102.04(3)° and Z = 8.     

(NH4)3[M2NCl10] (M = Nb,Ta): Synthese,Kristallstruktur und Phasenumwandlung

(NH₄)₃[M₂NCl₁₀] (M = Nb, Ta): Synthesis, Crystal Structure, and Phase Transition The nitrido complexes (NH₄)₃[Nb₂NCl₁₀], and (NH₄)₃[Ta₂NCl₁₀] are obtained in form of moisture-sensitive, tetragonal crystals by the reaction of the corresponding pentachlorides with NH₄Cl at 400 °C in sealed glass ampoules. Both compounds crystallize isotypically in two modifications, a low temperature form with the space group P4/mnc and a high temperature form with space group I4/mmm. In case of (NH₄)₃[Ta₂NCl₁₀] a continuous phase transition occurs between –70 °C and +60 °C. For the niobium compound this phase transition is not yet fully completed at 90 °C. The structure of (NH₄)₃[Nb₂NCl₁₀] was determined at several temperatures between –65 °C und +90 °C to carefully follow the continuous phase transition. For (NH₄)₃[Ta₂NCl₁₀] the structure of the low temperature form was determined at –70 °C, and of the high temperature form at +60 °C. The closely related crystal structures of the two modifications contain NH₄⁺ cations and [M₂NCl₁₀]^3– anions. The anions with the symmetry D_4h are characterized by a symmetrical nitrido bridge M=N=M with distances Nb–N = 184.5(1) pm at –65 °C or 183.8(2) pm at 90 °C, and Ta–N = 184.86(5) pm at –70 °C or 184.57(5) pm at 60 °C.     

Darstellung und Kristallstruktur eines Calciumcarbidchlorides mit einer C34−-Einheit,Ca3Cl2C3

Synthesis and Crystal Structure of a Calciumcarbide Chloride Containing a C₃^4? Unit, Ca₃Cl₂C₃ Ca₃Cl₂C₃ was prepared from calcium, CaCl₂ and graphite in sealed tantalum capsules. Red, transparent crystals were obtained from heating the mixture to 900°C (for one day) and annealing afterwards at 780°C for three days. The compound forms a layered structure (Cmcm, Z = 4, a = 384.24(9) pm, b = 1340.7(3) pm, c = 1152.6(3) pm, R = R_W = 0.036 for 481 independent intensities) with alternating stacks of double layers of Ca²⁺ and monolayers of Cl^?. The double layers of calcium contain allylenide ions, C₃^4?. The latter exhibit C_2v symmetry, a bond angle (C? C? C) of 169.0(6)° and a C? C separation of 134.6(4) pm.     

Die Reaktion von UV- und UVI-Verbindungen mit SOCl2

Reaction of U^V and U^VI Compounds with SOCl₂ UO₃, UO₂Cl₂, UCl₆, and UCl₅ reacted with OSCl₂ yield always UCl₅ · SCl₂, [SCl₃]⁺ [UCl₆]^? or a mixture of these compounds, but not an adduct UCl₅ · OSCl₂. An X-ray study was carried out with single crystals of [SCl₃]⁺[UCl₆]^?. It crystallizes in the orthorhombic space group P2₁2₁2₁ with the lattice constants a = 1066.8, b = 1071.2, c = 1133.3 pm and with Z = 4, containing isolated pyramidal SCl₃⁺ (r_SCl = 196.2 ± 1.1 pm ?SCl₂ = 102.34 ± 1.13°) and octahedral UCl₆^? ions (r_UCl = 251.1 ± 2.6 pm).     

Komplexe von Osmium (VIII) und Rhenium (VII) mit fünffach koordiniertem Metallatom Kristallstruktur von PPh4[OsO4Cl] · CH2Cl2

Five-coordinated Complexes of Osmium (VIII) and Rhenium (VII). Crystal Structure of PPh₄[OsO₄Cl] · CH₂Cl₂ The five-coordinated anionic complexes [OsO₄Cl]^?, [OsO₄N₃]^?, and [ReO₃Cl₂]^? were isolated as tetraphenylphosphonium salts from reactions of OsO₄ and ReO₃Cl with PPh₄Cl and PPh₄N₃, respectively, in dichloromethane solution. The compounds which are characterized by their i.r. spectra, are thermally sensitive and form crystalline powders with colours ranging from orange to violet. The crystal structure of PPh₄[OsO₄Cl] · CH₂Cl₂ was determined and refined with X-ray diffraction data. (4212 independent, observed reflexions, R = 0.032). It crystallizes in the monoclinic space group P2/b with four formula units per unit cell. The cell dimensions are at ?110°C a = 1754, b = 2184 pm, c = 692 and γ = 106.7°. The structure consists of tetraphenylphosphonium cations and anions [OsO₄Cl]^? with five-coordinated Os atoms in a trigonal bipyramidal geometry with the chlorine ligand in an axial position. The anion can also be regarded as a OsO₄ tetrahedron, monocapped by a chloride ion. Each chloride ion is linked with two CH₂Cl₂ molecules via hydrogen bridges, forming chains in the direction c. The Os? Cl bond length (276 pm) is very long; the average OsO distance (172 pm) corresponds to that in the OsO₄ molecule (170 pm).     

Rb6LiPr11Cl16[SeO3]12: Ein chloridisch derivatisiertes Rubidium‐Lithium‐Praseodym(III)‐Oxoselenat(IV)

Rb₆LiPr₁₁Cl₁₆[SeO₃]₁₂: A Chloride‐Derivatized Rubidium Lithium Praseodymium(III) Oxoselenate(IV) Transparent green square platelets with often truncated edges and corners of Rb₆LiPr₁₁Cl₁₆[SeO₃]₁₂ were obtained by the reaction of elemental praseodymium, praseodymium(III,IV) oxide and selenium dioxide with an eutectic LiCl–RbCl flux at 500 °C in evacuated silica ampoules. A single crystal of the moisture and air insensitive compound was characterized by X‐ray diffraction single‐crystal structure analysis. Rb₆LiPr₁₁Cl₁₆[SeO₃]₁₂ crystallizes tetragonally in the space group I4/mcm (no. 140; a = 1590.58(6) pm, c = 2478.97(9) pm, c/a = 1.559; Z = 4). The crystal structure is characterized by two types of layers parallel to the (001) plane following the sequence 121′2′1. Cl^? anions form cubes around the Rb⁺ cations (Rb1 and Rb2; CN = 8; d(Rb⁺?Cl^?) = 331 – 366 pm) within the first layer. One quarter of the possible places for Rb⁺ cations within this CsCl‐type kind of arrangement is not occupied, however the Cl^? anions of these vacancies are connected to Pr³⁺ cations (Pr4) above and below instead, forming square antiprisms of [(Pr4)O₄Cl₄]^9? units (d(Pr4?O) = 247–249 pm; d(Pr4?Cl) = 284–297 pm) that work as links between layer 1 and 2. Central cations of the second layer consist of Li⁺ and Pr³⁺. While the Li⁺ cations are surrounded by eight O^2? anions (d(Li?O5) = 251 pm) in the shape of cubes again, the Pr³⁺ cations are likewisely coordinated by eight O^2? anions as square antiprisms (for Pr1, d(Pr1?O2) = 242 pm) and by ten O^2? anions (for Pr2 and Pr3), respectively. The latter form tetracapped trigonal antiprisms (Pr2, d(Pr2?O) = 251–253 pm and 4 × 262 pm) or bicapped distorted cubes (Pr3, d(Pr3?O) = 245–259 pm and 2 × 279 pm). The non‐binding electron pairs (“lone pairs”) at the two crystallographically different Ψ¹‐tetrahedral [SeO₃]^2? anions (d(Se⁴⁺?O^2?) = 169–173 pm) are directing towards the empty cavities between the layer‐connecting [(Pr4)O₄Cl₄]^9? units.     

Synthese und Kristallstruktur von [Se3N2Cl]+ GaCl4−

Synthesis and Crystal Structure of [Se₃N₂Cl]⁺GaCl₄^? [Se₃N₂Cl]⁺GaCl₄^? has been prepared by the reduction of [Se₂NCl₂]⁺GaC1₄^? with SbPh₃ in CH₂Cl₂ solution, forming red crystals, which were characterized by an X-ray structure determination. Space group P2₁/n, Z = 4, 1640 observed unique reflections, R = 0.050. Lattice dimensions at ? 80 °C: a = 929.4(1), b= 1078.8(1), c = 1135.7(1) pm, β = 92.026(9)°. The cations from nearly planar Se₃N₂ five membered rings with Se? N bond lengths from 170 to 176pm and a Se? Se bond of 242.2 pm. One of the selenium atoms is bonded to the chlorine atom.     

Zur Kenntnis des quasi-binären Systems InCl?SnCl2 und eine Anmerkung zum System KCl?SnCl2

On the Quasi-binary System InCl? SnCl₂ and a Remark on the System KCl? SnCl₂ We report the phase diagrams of the quasi-binary systems InCl/SnCl₂ and KCl/SnCl₂ derived from DTA and X-ray investigations. In both systems we find a nonstoichiometric phase having the formula A_2?2xSn_5+xC₁₂ (with 0 ? x ? 0.15 for A = In and 0 ? x ? 0.14 for A ? K), a peritectic ASn₂Cl₅ compound and a dystectic 1:1 phase. The nonstoichiometric phases are both isotypic with Th₇S₁₂. KSn₂Cl₅ crystallizes with a tetragonal NH₄Pb₂Br₅-type structure (sp. gr. 14/mcm; a = 803.55(3), c = 1387.5(5) pm) and InSn₂Cl₅ with a monoclinic NH₄Pb₂Cl₅-type arrangement (sp. gr. P2₁/c; a = 891.7(3), b = 800.2(3), c = 1251.0(4) pm, β = 89.55(5)°). The lattice constants for InSnCl₃ (a = 1680(3), b = 799.2(9), c = 845.4(10) pm, β = 90.8(1)°) were derived by indexing the X-ray powder diagram. In addition the InCl? SnCl₂ system contains a peritectic In₄SnCl₆ phase (sp. gr. Pmma; a = 1270(2), b = 2515(3), c = 1456 (1) pm, (single crystal data)) and a dystectic In₉SnCl₁₁ compound (tetragonal primitive; a = 864.6(2), c = 1219.3(6) pm (derived from indexed powder data)).