Phthalocyaninate und Tetraphenylporphyrinate von hochkoordiniertem ZrIV/HfIV mit Hydroxo‐, Chloro‐, (Di)Phenolato‐, (Hydrogen)Carbonato‐ sowie (Amino)Carboxylato‐Liganden

Phthalocyaninates and Tetraphenylporphyrinates of High Co‐ordinated Zr^IV/Hf^IV with Hydroxo, Chloro, (Di)Phenolato, (Hydrogen)Carbonato, and (Amino)Carboxylato Ligands Crystals of tetra(n‐butyl)ammonium cis‐tri(phenolato)phthalocyaninato(2‐)zirconate(IV) ( 2 ) and ‐hafnate(IV) ( 1 ), di(tetra(n‐butyl)ammonium) cis‐di(tetrachlorocatecholato(O, O')phthalocyaninato(2‐)zirconate(IV) ( 3 ), and cis‐(di(μ‐alaninato(O, O')di(μ‐hydroxo))di(phthalocyaninato(2‐)zirconium(IV)) ( 12 ) have been isolated from tetra(n‐butyl)ammonium hydroxide solutions of cis‐di(chloro)phthalocyaninato(2‐)zirconium(IV) and ‐hafnium(IV), respectively, and the corresponding acid in polar organic solvents. Similarly, with cis‐di(chloro)tetraphenylporphyrinato(2‐)zirconium(IV), ^cis[Zr(Cl)₂tpp] as precursor crystalline tetra(n‐butyl)ammoniumcis‐tetrachlorocatecholato(O, O')hydrogentetrachlorocatecholato(O)tetraphenylporphyrinato(2‐)zirconate(IV) ( 4 ), cis‐hydrogencarbonato(O, O')phenolatotetraphenylporphyrinato(2‐)zirconium(IV) ( 6 ), cis‐di(benzoato(O, O'))tetraphenylporphyrinato(2‐)zirconium(IV) ( 11 ), and cis‐tetra(μ‐hydroxo)di(tetraphenylporphyrinato(2‐)zirconium(IV)) ( 13 ) with a cis‐arrangement of the symmetry equivalent μ‐hydroxo ligands, and from di(acetato)tetraphenylporphyrinato(2‐)zirconium(IV) the corresponding trans‐isomer ( 14 ) have been prepared. The endothermic dehydration at 215 °C of 13/14 yields μ‐oxodi(μ‐hydroxo)di(tetraphenylporphyrinato(2‐)zirconium(IV)) ( 15 ). 15 also precipitates on dilution of a solution of ^cis[Zr(X)₂tpp] (X = Cl, OAc) in dmf/(ⁿBu₄N)OH with water, while on prolonged standing of this solution on air tri(tetra(n‐butyl)ammonium) cis‐(^nido〈di(carbonato(O, O'))undecaaquamethoxide〉tetraphenylporphyrinato(2‐)zirconate(IV) ( 7 ) crystallizes, in which Zr^IV coordinates a supramolecular nestlike ^nido〈(O₂CO)₂(H₂O)₁₁OCH₃〉^5— cluster anion stabilised by hydrogen bonding in a nanocage of surrounding (ⁿBu₄N)⁺ cations. On the other hand, ^cis[Zr(Cl)₂pc] forms with (Et₄N)₂CO₃ in dichloromethane di(tetraethylammonium) cis‐di(carbonato(O, O')phthalocyaninato(2‐)zirconate(IV) ( 5 ). ^cis[Zr(Cl)₂tpp] dissolves in various O‐donor solvents, from which cis‐di(chloro)dimethylformamidetetraphenylporphyrinato(2‐)zirconium(IV) ( 8 ), cis‐di(chloro)dimethylsulfoxidetetraphenylporphyrinato(2‐)zirconium(IV) ( 9 ), and a 1:1 mixture ( 10 ) of cis‐di(chloro)dimethylsulfoxidetetraphenylporphyrinato(2‐)zirconium(IV) ( 10a ) and cis‐chlorodi(dimethylsulfoxide)tetraphenylporphyrinato(2‐)zirconium(IV) chloride ( 10b ) crystallize. All complexes contain solvate molecules in the solid state, except 3 . Zr^IV/Hf^IV is directed by ∼1Å out of the plane of the tetrapyrrolic ligand (pc, tpp) towards the mutually cis‐coordinated axial ligands. In the more concavely distorted phthalocyaninates, Zr^IV is mainly eight‐coordinated and in the tetraphenylporphyrinates seven‐coordinated. The octa‐coordinated Zr atom is in a distorted quadratic antiprism, and the hepta‐coordinated one is in a square‐base‐trigonal‐cap cooordination polyhedron. In most tpp complexes, the Zr atom is displaced by up to 0.3Å out of the centre of the coordination polyhedron towards the tetrapyrrolic ligand. In 13/14 , both antiprisms are face shared by an O₄ plane, and in 12 they are shared by an O₂ edge and the O atoms of the bridging aminocarboxylates, the dihedral angle between the O₄ planes of both antiprisms being 50.1(1)°. The mean Zr‐N_p distance is 0.05Å longer in the pc complexes than in the tpp complexes (d(Zr‐N_p)_pc = 2.31Å). In the monophenolato complexes, the mean Zr‐O distance (∼2.00Å) is shorter than in the complexes with other O‐donor ligands (d(Zr‐O)_pc = 2.18Å; d(Zr‐O)_tpp = 2.21Å); the Zr‐Cl distances vary between 2.473(1) and 2.559(2)Å (d(Zr‐Cl)_tpp = 2.51Å). d(C‐O_exo) = 1.494(4)Å in the bidentate hydrogencarbonato ligand in 6 is 0.26Å longer than in the bidentate carbonato ligands in 5 and 7 . 9 and 10a are rotamers slightly differing by the orientation of the axial ligands with respect to the tpp ligand. In 1—4, 6 , and 11 the phenolato, catecholato, and benzoato ligands, respectively, are in syn‐ and/or anti‐conformations with respect to the plane of the macrocycle. π‐Dimers with modest overlap of the neighbouring macrocyclic rings are observed in 5, 6, 8, 9, 10b, 12 , and 14 . The common UV/Vis spectroscopical and vibrational properties of the new phthalocyaninates and tetraphenylporphyrinates scarcely reflect their rich structural diversity.     

Studies on Properties of Tetra‐p‐nitro‐tetra‐O‐alkylcalix[4]arenes

Ibis paper reports the properties of the novel tetra‐p‐nitro‐tetra‐O‐alkyl‐calix[4]arenes (alkyl= n‐C₄H₉, 1; n‐C₈H₁₇ 2; n‐C₁₂H₂₅, 3; n‐C₁₆H₃₃, 4). X‐ray crystallographic analysis and ¹H NMR revealed that they exist as pinched‐cone conformation in crystal or cone conformation in solution. EFISH experiments at 1064 nm in CHCl₃, indicated that tetra‐p‐nitro‐tetra‐O‐butyl‐calix[4]arene (1) has higher hyperpolarizability β, values than the corresponding reference compound p‐nitro‐phenyl butyl ether, without red shift of the charge transfer band. Compounds 2, 3 and 4 with longer alkyl chains can form monolayer at the air/water.     

Darstellung,Kristallstrukturen, Schwingungsspektren und Normalkoordinatenanalysen der Tetrahalogeno‐bis‐Pyridin‐Osmium(III)‐Komplexe cis‐(n‐Bu4N)[OsCl4Py2] und trans‐(n‐Bu4N)[OsX4Py2], X = Cl,Br

Synthesis, Crystal Structures, Vibrational Spectra, and Normal Coordinate Analyses of the Tetrahalogeno‐bis‐Pyridine‐Osmium(III) Complexes cis ‐( n ‐Bu₄N)[OsCl₄Py₂] and trans ‐( n ‐Bu₄N)[OsX₄Py₂], X = Cl, Br By reaction of (n‐Bu₄N)₂[OsX₆], X = Cl, Br, with pyridine and (n‐Bu₄N)[BH₄] tetrahalogeno‐bis‐pyridine‐osmium(III) complexes are formed and purified by chromatography. X‐ray structure determinations on single crystals have been performed of cis‐(n‐Bu₄N)[OsCl₄Py₂] ( 1 ) (triclinic, space group P1, a = 9.4047(9), b = 10.8424(18), c = 17.007(2) Å, α = 71.833(2), β = 81.249(10), γ = 67.209(12)°, Z = 2), trans‐(n‐Bu₄N)[OsCl₄Py₂] ( 2 ) (orthorhombic, space group P2₁2₁2₁, a = 8.7709(12), b = 20.551(4), c = 17.174(4) Å, Z = 4) and trans‐(n‐Bu₄N)[OsBr₄Py₂] ( 3 ) (triclinic, space group P1, a = 9.132(3), b = 12.053(3), c = 15.398(2) Å, α = 95.551(18), β = 94.12(2), γ = 106.529(19)°, Z = 2). Based on the molecular parameters of the X‐ray structure determinations and assuming C₂ point symmetry for the anion of 1 and D_2h point symmetry for the anions of 2 and 3 the IR and Raman spectra are assigned by normal coordinate analysis. The valence force constants of 1 are in the Cl–Os–Cl axis f_d(OsCl) = 1.58, in the asymmetrically coordinated N′–Os–Cl ^· axes f_d(OsCl ^· ) = 1.45, f_d(OsN′) = 2.48, of 2 f_d(OsCl) = 1.62, f_d(OsN) = 2.42 and of 3 f_d(OsBr) = 1.39 and f_d(OsN) = 2.34 mdyn/Å.     

Crystal Structure of the [(C5H4BMe2)2Fe]‐4,4′‐bipyridine Polymer from High Resolution X‐Ray Powder Diffraction

The crystal structure of [(C₅H₄BMe₂)₂Fe]‐4,4′‐bipyridine [ 2 · bipy]_n has been determined by the method of simulated annealing from high resolution X‐ray powder diffraction at room temperature. The compound is of interest, because it proves that highly ordered organometallic macromolecules can be formed in the solid state via the self‐assembly of N–B‐donor‐acceptor bonds. [ 2 · bipy]_n crystallizes in the triclinic space group, P 1, Z = 2, with unit cell parameters of a = 8.3366(2) Å, b = 11.4378(3) Å, c = 12.6740(5) Å, α = 112.065(2)°, β = 108.979(1)°, γ = 90.551(2)°, and V = 1047.06(6) ų. For the structure solution of [ 2 · bipy]_n 11 degrees of freedom (3 translational, 3 orientational, 5 torsion angles) were determined within several hours, demonstrating that the crystal packing and the molecular conformation of medium sized (< 50 non‐hydrogen atoms) coordination compounds can nowadays be solved routinely from high resolution powder diffraction data.     

Synthese und Eigenschaften von Bis(tetra(n-butyl)ammonium)-μ-carbidodi(halogenophthalocyaninato(2–)ferraten(IV)); Kristallstruktur von Bis(tetra(n-butyl)ammonium)-μ-carbidodi(fluorophthalocyaninato(2–)ferrat(IV))-Trihydrat

Synthesis and Properties of Bis(tetra(n-butyl)ammonium)μ-Carbido-di(halophthalocyaninato(2–)ferrates(IV)); Crystal Structure of Bis(tetra(n-butyl)ammonium) μ-Carbido-di(fluorophthalocyaninato(2–)ferrate(IV)) Trihydrate μ-Carbido-di(pyridinephthalocyaninato(2–)iron(IV)) reacts with tetra(n-butyl)ammonium halide (ⁿBu₄N)X) in solution (X = F) or in a melt (X = Cl, Br) to yield bis(tetra(n-butyl)ammonium μ-carbido-di(halophthalo-cyaninato(2–)ferrat(IV)). The fluoro-complex salt crystallizes as a trihydrate monoclinically in the space group P12₁/n1 with the following cell parameters: a = 15.814(1) Å; b = 22.690(5) Å; c = 25.127(3) Å; β = 98.27(1)°, Z = 4. The Fe atoms are almost in the centre (Ct) of the (N_iso)₄ planes (N_iso: isoindoline-N atom) with a Fe–Ct distance of 0.053(1) Å. The average Fe–N_iso distance is 1.939(4) Å, the Fe–(μ-C) distance 1.687(4) Å and the Fe–F distance 2.033(2) Å. The Fe–(μ-C)–Fe core is linear (179.5(3)°). The pc²-ligands are staggered (φ = 42(1)°) with a convex distortion. The asymmetric Fe–(μ-C)–Fe stretch (in cm^–1) is observed in the IR spectra at 917 (X = F), 918 (Cl) and 920 (Br) and the symmetric Fe–(μ-C)–Fe stretch at 476 cm^–1 in the resonance Raman spectra. The IR active asymmetric Fe–X stretch (in cm^–1) absorbs at 336 (X = F), 203 (Cl), 182 (Br), respectively.     

Kristallstrukturen,Schwingungsspektren und Normalkoordinatenanalyse von (n‐Bu4N)2[Os(NCS)6] und (n‐Bu4N)3[Os(NCS)6]

Crystal Structure, Vibrational Spectra, and Normal Coordinate Analysis of ( n ‐Bu₄N)₂[Os(NCS)₆] and ( n ‐Bu₄N)₃[Os(NCS)₆] By tempering the solid mixture of the linkage isomers (n‐Bu₄N)₃[Os(NCS)_n(SCN)_6–n] n = 0–5 for a longer time at temperatures increasing from 60 to 140 °C the homoleptic (n‐Bu₄N)₃[Os(NCS)₆] is formed, which on oxidation with (NH₄)₂[Ce(NO₃)₆] in acetone yields the corresponding Os^IV complex (n‐Bu₄N)₂[Os(NCS)₆]. X‐ray structure determinations on single crystals of (n‐Bu₄N)₂[Os(NCS)₆] (1) (triclinic, space group P 1, a = 12.596(5), b = 12.666(5), c = 16.026(5) Å, α = 88.063(5), β = 80.439(5), γ = 88.637(5)°, Z = 2) and (n‐Bu₄N)₃[Os(NCS)₆] ( 2 ) (cubic, space group Pa 3, a = 24.349(4) Å, Z = 8) have been performed. The nearly linear thiocyanate groups are coordinated with Os–N–C angles of 172.3–177.7°. Based on the molecular parameters of the X‐ray determinations the IR and Raman spectra are assigned by normal coordinate analysis. The valence force constant f_d(OsN) is 2.3 ( 1 ) and 2.10 mdyn/Å ( 2 ).     

ReV‐Phthalocyaninate und ReV‐Tetraphenylporphyrinate mit Oxo‐Liganden: Synthese,Eigenschaften und Kristallstruktur

Re^V‐Phthalocyaninates and Re^V‐Tetraphenylporphyrinates: Synthesis, Properties, and Crystal Structure Hexa‐coordinated Re^V phthalocyaninates (pc) and Re^V tetraphenylporphyrinates (tpp) of the type [Re(O)(X)p] (p: pc, tpp) with X = OCH₃, ReO₄, Cl/pc, F/pc, OH/tpp, [{Re(O)p}₂(μ‐O)] and (cat)^trans[Re(O)₂p] (cat: ⁿBu₄N, Et₄N/tpp) have been isolated and characterised by their UV‐Vis‐NIR, IR and resonance Raman (RR) spectra. In the RR spectra, the intensity of the (Re=O) and (Re–X) stretching vibrations (ν(Re=O/–X)) in [Re(O)(X)p] and [{Re(O)p}₂(μ‐O)] is selectively enhanced with excitation in coincidence with O → Re–CT between ca 19000 and 22000 cm^–1. In accordance to selection rules, data of ν(Re=O/–X) compare well with those of the complementary IR spectra. Because of the trans influence ν(Re=O) depends on the axial ligand X, ranging from 940 to 1010 cm^–1. The crystallographic characterization of [Re(O)(ReO₄)tpp] · CHCl₃ ( 1 ), [{Re(O)tpp}₂(μ‐O)] · py ( 2 ), (ⁿBu₄N)^trans[Re(O)₂tpp] ( 3 ), and (Et₄N)^trans[Re(O)₂tpp] · 2 H₂O ( 4 ) is described. The tpp centered Re atom is in a distorted octahedron of four N atoms of the porphyrinate and two axial O atoms in a mutual trans position. Average Re–N distances are 2.062 Å in 1 , 2.086 Å in 2 , 2.089 Å in 3 , and 2.082/2.086 Å in 4 . The Re–O distance of the terminal rhenyl group varies from 1.64(1) Å ( 1 ), 1.73(1)/1.70(1) Å ( 2 ) to 1.80(1) Å ( 4 ), that of the monodentate rhenate(VII) from 1.70(1) to 1.75(1) Å. The Re–O distances in the bridge of the linear O=Re–O–Re=O skeleton in 2 are 1.95(1)/1.89(1) Å. In 1 , with a bent O=Re–O^ ReO₃ moiety (∢(Re–O^ReO₃) = 143(1)°) and a mostly ionic coordinated rhenate(VII), these distances differ significantly (2.20(1) Å vs 1.75(1) Å). The porphyrinate in 1 is saucer‐shaped with a distal rhenate(VII), and the tpp centered Re atom is displaced by 0.31 Å out of the (N)₄ plane towards the rhenyl‐O atom. The distorted porphyrinates in 2 are rotated by 30.4(4)°, and the Re atoms are 0.1 Å out of their (N)₄ planes towards the terminal O atoms. In 3 and 4 the porphyrinates are almost planar with the Re atom in their centre.     

Kristallstrukturen,spektroskopische Charakterisierung und Normalkoordinatenanalyse von (n‐Bu4N)2[M(ECN)4] (M = Pd,Pt; E = S,Se)

Crystal Structures, Spectroscopic Analysis, and Normal Coordinate Analysis of ( n ‐Bu₄N)₂[M(ECN)₄] (M = Pd, Pt; E = S, Se) The reaction of (NH₄)₂[PdCl₄] or K₂[PtCl₄] with KSCN or KSeCN in aqueous solutions yields the complex anions [Pd(SCN)₄]^2–, [Pt(SCN)₄]^2– and [Pt(SeCN)₄]^2–, which are converted into (n‐Bu₄N) salts with (n‐Bu₄N)HSO₄. (n‐Bu₄N)₂[Pd(SeCN)₄] is formed by treatment of (n‐Bu₄N)₂[PdCl₄] with (n‐Bu₄N)SeCN in acetone. X‐ray structure determinations on single crystals of (n‐Bu₄N)₂[Pd(SCN)₄] (monoclinic, space group P2₁/n, a = 13.088(3), b = 12.481(2), c = 13.574(3) Å, β = 91.494(15)°, Z = 2), (n‐Bu₄N)₂[Pd(SeCN)₄] (monoclinic, space group P2₁/n, a = 13.171(2), b = 12.644(2), c = 13.560(2) Å, β = 91.430(11)°, Z = 2) and (n‐Bu₄N)₂[Pt(SeCN)₄] (monoclinic, space group P2₁/n, a = 13.167(2), b = 12.641(1), c = 13.563(2) Å, β = 91.516(18)°, Z = 2) reveal, that the compounds crystallize isotypically and the complex anions are centrosymmetric and approximate planar. In the Raman spectra the metal ligand stretching modes of (n‐Bu₄N)₂[Pd(SCN)₄] ( 1 ) and (n‐Bu₄N)₂[Pt(SCN)₄] ( 3 ) are observed in the range of 260–303 cm^–1 and of (n‐Bu₄N)₂[Pd(SeCN)₄] ( 2 ) and (n‐Bu₄N)₂[Pt(SeCN)₄] ( 4 ) in the range of 171–195 cm^–1. The IR and Raman spectra are assigned by normal coordinate analysis using the molecular parameters of the X‐ray determination. The valence force constants are f_d(PdS) = 1.17, f_d(PdSe) = 1.17, f_d(PtS) = 1.44 and f_d(PtSe) = 1.42 mdyn/Å. The ⁷⁷Se NMR resonances are 23 for 2 , –3 for 4 and the ¹⁹⁵Pt NMR resonances 549 for 3 and 130 ppm for 4 .     

Synthesis,Properties, and Structures of Salts with the Reineckate Anion, [CrIII(NCS)4(NH3)2]–, and Large Organic Cations

A series of 9 new Reineckate salts, A[Cr^III(NCS)₄(NH₃)₂] with various large organic cations A = tetraalkylammonium, [R₄N]⁺, R = n‐butyl, n‐dodecyl; 1‐alkyl‐3‐methylimidazolium, (RMIm)⁺: R = methyl, ethyl, iso‐propyl, n‐butyl, and n‐hexyl; A = 1,3‐dimethyl‐2,4,5‐triphenylimidazolium and A = 1,2,3,4,5‐pentamethylimidazolium was synthesized. The melting point of each compound was measured to see if any belongs to the group of metal‐containing Ionic Liquids with low melting points. Each compound was further characterized by elemental analysis, NMR, IR, and UV/Vis spectroscopy. From NMR investigations information about the magnetic behavior was derivedusing the Evans method. It has been found that every compound is paramagnetic with effective magnetic moments of spin‐only Cr^III. The structures of the Reineckates with A = tetra‐n‐butyl‐ammonium, tetra‐n‐dodecyl‐ammonium, 1‐ethyl‐3‐methylimidazolium, and 1,2,3,4,5‐pentamethylimidazolium were determined by single‐crystal X‐ray diffraction measurements: (nBu₄N)[Cr(NCS)₄(NH₃)₂]: monoclinic, C2/c (no. 15), a = 12.0818(8), b = 10.2425(8), c = 24.222(2) Å, β = 98.324(3)°, Z = 4, R1(F)/wR2(F²) = 0.0332/0.0871; {(C₁₂H₂₅)₄N}[Cr(NCS)₄(NH₃)₂]·0.85H₂O: triclinic, P$\bar{1}$ (no. 2), a = 8.4049(1), b = 20.1525(4), c = 20.7908(4) Å, α = 67.487(1)°, β = 81.328(1)°, γ = 78.040(1)°, Z = 2, R1(F)/wR2(F²) = 0.0533/0.1343; (EMIm)[Cr(NCS)₄(NH₃)₂]: orthorhombic, Pbcm (no. 57), a = 8.765(2), b = 15.888(3), c = 14.191(3) Å, Z = 4, R1(F)/wR2(F²) = 0.0466/0.1271; (PeMIm)[Cr(NCS)₄(NH₃)₂]: monoclinic, P2₁/n (no. 14), a = 6.0817(2), b =13.9811(5), c = 25.2902(9) Å, β = 90.075(2)°, Z = 4, R1(F)/wR2(F²) = 0.0405/0.1111.     

Darstellung,Kristallstrukturen, Schwingungsspektren und Normalkoordinatenanalyse von cis‐ und trans‐(n‐Bu4N)2[PtF2(ox)2] und (n‐Bu4N)2[PtF4(ox)]

Synthesis, Crystal Structure, Vibrational Spectra, and Normal Coordinate Analysis of cis‐ and trans‐(n‐Bu₄N)₂[PtF₂(ox)₂] and (n‐Bu₄N)₂[PtF₄(ox)] By treatment of trans‐(n‐Bu₄N)₂[PtCl₂(ox)₂] and (n‐Bu₄N)₂[PtCl₄(ox)] with XeF₂ in propylene carbonate cis‐ and trans‐(n‐Bu₄N)₂[PtF₂(ox)₂] ( 1 , 2 ) and (n‐Bu₄N)₂[PtF₄(ox)] ( 3 ) are formed which have been isolated by ion exchange chromatography on diethylaminoethyl cellulose. The crystal structure of trans(n‐Bu₄N)₂[PtF₂(ox)₂] ( 2 ) (tetragonal, space group P4₂/n, a = 15.5489(9), b = 15.5489(9), c = 17.835(1)Å, Z = 4) und Cs₂[PtF₄(ox)] ( 3 ) (monoclinic, space group C2/m, a = 14.5261(7), b = 6.2719(4), c = 9.6966(9)Å, β = 90.216(8)°, Z = 4) reveal complex anions with nearly D_2h and C_2v point symmetry. The average bond lengths in the symmetrical coordinated axes are Pt—F = 1.93 ( 2 , 3 ) and Pt—O = 1.987 ( 2 ) and in the F^•—Pt—O′‐axes Pt—F^• = 1.957 and Pt—O′ = 1.977Å ( 3 ). The oxalato ligands are nearly planar with a maximum displacement of the ring atoms of 0.05 ( 2 ) und 0.01Å ( 3 ) to the calculated best planes. In the vibrational spectra the symmetric and antisymmetric PtF stretching vibrations are observed at 583 and 586 ( 2 ) and 576 and 568 cm^—1 ( 3 ). The PtF^• modes appear at 565 and 562 ( 1 ) and 560 cm^—1 ( 3 ). The PtO and PtO′ stretching vibrations are coupled with internal modes of the oxalato ligands and appear in the range of 400—800 cm^—1. Based on the molecular parameters of the X‐ray determinations ( 2 , 3 ) and estimated data ( 1 ) the IR and Raman spectra are assigned by normal coordinate analysis. The valence force constants are f_d(PtF) = 3.55 ( 2 ) and 3.38 ( 3 ), f_d(PtF^•) = 3.23 ( 1 ) and 3.20 ( 3 ), f_d(PtO) = 2.65 ( 1 ) and 2.84 ( 2 ) and f_d(PtO′) = 2.97 ( 1 ) and 3.00 mdyn/Å ( 3 ). Taking into account increments of the trans influence a good agreement between observed and calculated frequencies is achieved. The NMR shifts are δ(¹⁹⁵Pt) = 8485 ( 1 ), 8597 ( 2 ) and 10048 ppm ( 3 ), δ(¹⁹F) = —350 ( 2 ) and —352 ( 3 ) and δ(¹⁹F^•) = —323 ( 1 ) and —326 ppm ( 3 ) with the coupling constants ¹J(PtF) = 1784 ( 2 ) and 1864 ( 3 ) and ¹J(PtF^•) = 1525 ( 1 ) and 1638 Hz ( 3 ).     

Three Ternary Rare Earth(III) Complexes Based on 3‐[(4,6‐Dimethyl‐2‐pyrimidinyl)thio]‐propanoic Acid and 1,10‐Phenanthroline: Synthesis,Crystal Structure and Antioxidant Activity

Three ternary rare earth [Nd^III ( 1 ), Sm^III ( 2 ) and Y^III ( 3 )] complexes based on 3‐[(4,6‐dimethyl‐2‐pyrimidinyl)thio]‐propanoic acid (HL) and 1,10‐phenanthroline (Phen) were synthesized and characterized by IR and UV/Vis spectroscopy, TGA, and single‐crystal X‐ray diffraction. The crystal structures showed that complexes 1 – 3 contain dinuclear rare earth units bridged by four propionate groups and are of general formula [REL₃(Phen)]₂ · nH₂O (for 1 and 2 : n = 2; for 3 : n = 0). All rare earth ions are nine‐coordinate with distorted mono‐capped square antiprismatic coordination polyhedra. Complex 1 crystallizes in the monoclinic system, space group P2₁/c with a = 16.241(7) Å, b = 16.095(7) Å, c = 19.169(6) Å, β = 121.48(2)°. Complex 2 crystallizes in the monoclinic system, space group P2₁/c with a = 16.187(5) Å, b = 16.045(4) Å, c = 19.001(4) Å, β = 120.956(18)°. Complex 3 crystallizes in the triclinic system, space group P1 with a = 11.390(6) Å, b = 13.636(6) Å, c = 15.958(7) Å, α = 72.310(17)°, β = 77.548(15)°, γ = 78.288(16)°. The antioxidant activity test shows that all complexes own higher antioxidant activity than free ligands.     

Mononitrosyl‐ und trans‐Dinitrosyl‐Komplexe von Phthalocyaninaten des Mangans und Rheniums

Mononitrosyl and trans ‐Dinitrosyl Complexes of Phthalocyaninates of Manganese and Rhenium Tetra(n‐butyl)ammonium or di(triphenylphosphane)iminium nitrosylacidophthalocyaninato(2–)manganate, (cat)[Mn(NO)(X)pc^2–] (X = ONO, NCO, N₃; cat = ⁿBu₄N, PNP) is prepared from acidophthalocyaninato(2–)manganese, [Mn(X)pc^2–], (cat)NO₂ and (ⁿBu₄N)BH₄ in CH₂Cl₂ or from nitrosylphthalocyaninato(2–)manganese, [Mn(NO)pc^2–] and (ⁿBu₄N)X (X = ONO, NCO, N₃, NCS) at T < 120 °C, respectively. [Mn(NO)(X)pc^2–]^– dissociates in methanol, and [Mn(NO)pc^2–] precipitates. Nitrito(O)phthalocyaninato(2–)manganese, (cat)NO₂ and hydrogensulfide yield trans‐di(nitrosyl)phthalocyaninato(2–)manganate, ^trans[Mn(NO)₂pc^2–]^–, isolated as red violet (PNP) and (ⁿBu₄N) complex salt. Nitrosyl(triphenylphosphane oxide)phthalocyaninato(2–)manganese, [Mn(NO)(OPPh₃)pc^2–] is obtained by addition of OPPh₃ to [Mn(NO)pc^2–] at 200 °C. Di(triphenylphosphane)phthalocyaninato(2–)rhenium(II) and (PNP)NO₂ in CH₂Cl₂ or in molten (PNP)NO₂ and PPh₃ at 100 °C yields green blue l‐di(triphenylphosphane)iminium nitrosylnitrito(O)phthalocyaninato(2–)rhenate, ^l(PNP)[Re(NO)(ONO)pc^2–]. Similarly, but with (ⁿBu₄N)NO₂ red plates of tetra‐(n‐butyl)ammonium trans‐di(nitrosyl)phthalocyaninato(2–)rhenate, (ⁿBu₄N)^trans[Re(NO)₂pc^2–] is isolated. Addition of (PNP)Br or (PNP)PF₆ to a concentrated solution of (ⁿBu₄N)^trans[Re(NO)₂pc^2–] in pyridine precipitates ^l(PNP)^trans[Re(NO)₂pc^2–]. (ⁿBu₄N)^trans[Re(NO)₂pc^2–] and PPh₃ at 300 °C yield blue green nitrosyl(triphenylphosphane oxide)phthalocyaninato(2–)‐ rhenium, [Re(NO)(OPPh₃)pc^2–], that is oxidised with iodine precipitating nitrosyl(triphenylphosphane oxide)phthalocyaninato(2–)rhenium triiodide, [Re(NO)(OPPh₃)pc^2–]I₃. The crystal structures of ^l(PNP)[Mn(NO)(ONO)pc^2–] ( 1 ), ^l(PNP)‐ [Mn(NO)(NCO)pc^2–] ( 2 ), ^l(PNP)^trans[Mn(NO)₂pc^2–] ( 3 ), ^l(PNP)^trans[Re(NO)₂pc^2–] ( 4 ) [Mn(NO)(OPPh₃)pc^2–] ( 5 ), [Re(NO)(OPPh₃)pc^2–] ( 6 ), and [Re(NO)(OPPh₃)pc^2–]I₃ · CH₂Cl₂ ( 7 ) have been determined. The M–N(NO) distance varies between 1.623(12) Å in 5 and 1.846(3) Å in 3 . The M–N–O moiety is almost linear. The UV‐Vis spectra with the B band at ca. 14500 cm^–1and the Q band at 30400 cm^–1 do not dependent significantly on the axial ligand and the metal atom and its oxidation state. N–O stretching vibrations are observed in the IR spectra between 1701 cm^–1 in 3 and 1753 cm^–1 in [Mn(NO)pc^2–] or for the Re series between 1571 cm^–1 in 4 and 1724 cm^–1 in 7 . M–N(NO) stretching and M–N–O deformation vibrations are assigned in the IR spectra and resonance Raman spectra between 486 cm^–1 in 4 and 620 cm^–1 in 1 .     

C–H-Aktivierung: Synthese und Eigenschaften von Acetonato(C)acidophthalocyaninato(2–)metallaten(III) von Rhodium und Iridium; Kristallstruktur von Tetra(n-butyl)ammoniumacetonato(C)-azidophthalocyaninato(2–)iridat(III)

C–H-Activation: Syntheses and Properties of Acetonato( C )-acidophthalocyaninato(2–)metallates(III) of Rhodium and Iridium; Crystal Structure of Tetra(n-butyl)ammonium Acetonato( C )azidophthalocyaninato(2–)iridate(III) Phthalocyaninato(2–)metallate(I) of rhodium and iridium reacts with carbonyl substrates like acetone or acetylacetone and halides or pseudohalides forming acetonato(C)- or acetylacetonato(C)acidophthalocyaninato(2–)metallates(III), that are isolated as tetra(n-butyl)ammonium complex salts (ⁿBu₄N)[M(R)(X)pc^2–] (M = Rh, Ir; R = aC, acaC; X = Cl, I, N₃, SCN/NCS). (ⁿBu₄N)[Ir(aC)(N₃)pc^2–] · 0,25(C₂H₅)₂O · 0,5 CH₂Cl₂ crystallizes in the triclinic space group P1 with cell parameters a = 16.267(8) Å, b = 17.938(3) Å, c = 18.335(4) Å, α = 74.77(2)°, β = 73.73(3)°, γ = 84.25(3)°, V = 4954(3) ų, Z = 4. There are two crystallographically independent anions, differing by the orientation of the azido ligand either towards an isoindole group or a N_aza bridge of the phthalocyaninate, while the σ-C bonded acetonate is always oriented towards an isoindole group (gauche and ecliptical configuration). The Ir–C distances are 2.12(1) and 2.14(1) Å. Due to the trans influence of the acetonate-C atom the Ir-azide-N distances of 2.22(1)/2.24(1) Å are longer than expected. The electrochemical properties and the optical, vibrational, and ¹H-NMR spectra are discussed.     

Darstellung,Kristallstrukturen und Schwingungsspektren von trans‐[Pt(N3)4(ECN)2]2–, E = S,Se

Synthesis, Crystal Structures, and Vibrational Spectra of trans ‐[Pt(N₃)₄(ECN)₂]^2–, E = S, Se By oxidative addition to (n‐Bu₄N)₂[Pt(N₃)₄] with dirhodane in dichloromethane trans‐(n‐Bu₄N)₂[Pt(N₃)₄(SCN)₂] and by ligand exchange of trans(n‐Bu₄N)₂[Pt(N₃)₄I₂] with Pb(SeCN)₂ trans‐(n‐Bu₄N)₂[Pt(N₃)₄(SeCN)₂] are formed. X‐ray structure determinations on single crystals of trans‐(Ph₄P)₂[Pt(N₃)₄(SCN)₂] (triclinic, space group P 1, a = 10.309(3), b = 11.228(2), c = 11.967(2) Å, α = 87.267(13), β = 75.809(16), γ = 65.312(17)°, Z = 1) and trans‐(Ph₄P)₂[Pt(N₃)₄(SeCN)₂] (triclinic, space group P 1, a = 9.1620(10), b = 10.8520(10), c = 12.455(2) Å, α = 90.817(10), β = 102.172(10), γ = 92.994(9)°, Z = 1) reveal, that the compounds crystallize isotypically with octahedral centrosymmetric complex anions. The bond lengths are Pt–S = 2.337, Pt–Se = 2.490 and Pt–N = 2.083 (S), 2.053 Å (Se). The approximate linear Azidoligands with N^α–N^β–N^γ‐angles = 172,1–175,0° are bonded with Pt–N^α–N^β‐angles = 116,7–120,5°. In the vibrational spectra the platinum chalcogen stretching vibrations of trans‐(n‐Bu₄N)₂[Pt(N₃)₄(ECN)₂] are observed at 296 (E = S) and in the range of 186–203 cm^–1 (Se). The platinum azide stretching modes of the complex salts are in the range of 402–425 cm^–1. Based on the molecular parameters of the X‐ray determinations the IR and Raman spectra are assigned by normal coordinate analysis. The valence force constants are f_d(PtS) = 1.64, f_d(PtSe) = 1.36, f_d(PtN^α) = 2.33 (S), 2.40 (Se) and f_d(N^αN^β, N^βN^γ) = 12.43 (S), 12.40 mdyn/Å (Se).     

Synthesis and Crystal Structure of Octahydro‐5H,12H‐4,11‐methano‐1H,7H‐bis[1,2,5]oxadiazolo[3,4‐d:3′,4′‐j][1,7,3,9]dioxadiazacyclododecine

The unusual 12‐membered ring compound, octahydro‐5H,12H‐4,11‐methano‐1H,7H‐bis[1,2,5]oxadiazolo[3,4‐d:3′,4′‐j][1,7,3,9]dioxadiazacyclododecine is obtained from the acid catalyzed reaction of 3‐amino‐4‐hydroxymethylfurazan with formaldehyde instead of the expected methylene‐bridged compound, 4,4′‐methylenebis[4,5‐dihydro‐7H‐[1,2,5]oxadiazolo[3,4‐d][1,3]oxazine]. The compound crystallizes in Tetragonal, P4₃2₁2, a = 6.4141(4) Å, b = 6.4141(4) Å, c = 26.525(3) Å, α = 90°, β = 90°, γ = 90°, V = 1091.27(16) ų, Z = 4, dcalc = 1.614 Mg/m³.     

Synthese und Eigenschaften von cis-Diacidophthalocyaninato(2–)thallaten(III); Kristallstruktur von Tetra(n-butyl)ammonium-cisdinitrito(O,O′)- und -cis-dichlorophthalocyaninato(2–)thallat(III)

Syntheses and Properties of cis -Diacidophthalocyaninato(2–)thallates(III); Crystal Structure of Tetra(n-butyl)ammonium cis -dinitrito(O,O ′)- and cis -dichlorophthalocyaninato(2–)thallate(III) Blue green cis-diacidophthalocyaninato(2–)thallate(III), ^cis[Tl(X)₂pc^2–]^– (X = Cl, ONO′, NCO) is prepared from iodophthalocyaninato(2–)thallium(III) and the corresponding tetra(n-butyl)ammonium salt, (ⁿBu₄N)X in dichloromethane, and isolated as (ⁿBu₄N)^cis[Tl(X)₂pc^2–]. (ⁿBu₄N)^cis[Tl(ONO′)₂pc^2–] ( 1 ) and (ⁿBu₄N)^cis[Tl(X)₂pc^2–] · 0,5 (C₂H₅)₂O ( 2 ) crystallize in the monoclinic space group P2₁/n with cell parameters for 1: a = 14.496(2) Å, b = 17.293(5) Å, c = 18.293(2) Å, β = 98.76(1)° resp. for 2 : a = 13.146(1) Å, b = 14.204(5) Å, c = 24.900(3) Å, β = 93.88(1)°; Z = 4. In 1 , the octa-coordinated Tl atom is surrounded by four isoindole-N atoms (N_iso) and four O atoms of the bidental nitrito(O,O′) ligands in a distorted antiprism. The Tl–N_iso distances vary between 2.257(3) and 2.312(3) Å, the Tl–O distances between 2.408(3) and 2.562(3) Å. In 2 , the hexa-coordinated Tl atom ligates four N_iso atoms and two Cl atoms in a typical cis-arrangement. The average Tl–N_iso distance is 2.276 Å, the average Tl–Cl distance is 2.550 Å. In 1 and 2 , the Tl atom is directed out of the centre of the (N_iso)₄ plane (Ct_N) towards the acido ligands (d(Tl–Ct_N) = 1.144(1) Å in 1 , 1.116(2) Å in 2 ), and the phthalocyaninato ligand is concavely distorted. The vertical displacements of the periphereal C atoms amounts up to 0.82 Å. The optical and vibrational spectra as well as the electrochemical properties are discussed.     

Darstellung und Eigenschaften von (Acido)(pyridin)phthalocyaninato(2–)ruthenaten(II); Kristallstruktur von Tetra(n-butyl)ammonium(cyano)(pyridin)phthalocyaninato(2–)ruthenat(II)

Syntheses and Properties of (Acido)(pyridine)phthalocyaninato(2–)ruthenates(II); Crystal Structure of Tetra(n-butyl)ammonium (Cyano)(pyridine)phthalocyaninato(2–)ruthenate(II) Bis(tetra(n-butyl)ammonium bis(acido)phthalocyaninato(2–)ruthenate(II) reacts in boiling pyridine to yield blue purple, diamagnetic tetra(n-butyl)ammonium (acido)(pyridine)phthalocyaninato(2–)ruthenate(II), (ⁿBu₄N)[Ru(X)(py)pc^2–] (X = CN, N₃, NCS, NCO, NO₂). (ⁿBu₄N)[Ru(CN)(py)pc^2–] crystallizes in the orthorhombic space group Pca2₁ (no. 29) with cell parameters a = 28.319(5) Å, b = 29.850(3) Å, c = 24.566(7) Å, Z = 16, with four crystallographically independent complex anions present in the unit cell. Each Ru atom is located outside the centre (Ct) of the corresponding (N_iso)₄ plane (N_iso: isoindoline N atom) and coordinates axially pyridine and cyanide in a mutual trans position. The largest vertical displacement of the Ru atom from the (N_iso)₄ plane towards cyanide (d(Ru–Ct)) is 0.020 Å. The Ru–N_iso distance varies from 1.947(2) to 1.992(2) Å. The average Ru–C and Ru–N_py distance is 2.00 Å and 2.19 Å, respectively. The pc^2– ligand ist slightly distorted towards the cyanide. The cyclic and differential pulse voltammograms of (ⁿBu₄N)[Ru(X)(py)pc^2–] exhibit the first quasi-reversible one electron process (in V) at 0.46 (X = CN), 0.34 (N₃), 0.40 (NCO), 0.47 (NO₂), 0.50 V (NCS) and the second, independent of X, at approximately 1.05 V. The first process is metal directed, the second ring directed. The electronic absorption spectra and the vibrational spectra of (ⁿBu₄N)[Ru(X)(py)pc^2–] are discussed.     

Mesityl‐phenolato‐vanadium(III)‐Komplexe: Synthese,Struktur und Verhalten

Mesityl‐vanadium(III)‐phenolate Complexes: Synthesis, Structure, and Reactivity Protolysis reactions of [VMes₃(THF)] with ortho‐substituted phenols (2‐iso‐propyl‐(H–IPP), 2‐tert‐butyl(H–TBP), 2,4,6‐trimethylphenol (HOMes) and 2,2′biphenol (H₂–Biphen) yield the partially and fully phenolate substituted complexes [VMes(OAr)₂(THF)₂] (OAr = IPP ( 1 ), TBP ( 2 )), [VMes₂(OMes)(THF)] ( 4 ), [V(OAr)₃(THF)₂] (OAr = TBP ( 3 ), OMes ( 5 )), and [V₂(Biphen)₃(THF)₄] ( 6 ). Treatment of 6 with Li₂Biphen(Et₂O)₄ results in formation of [{Li(OEt₂)}₃V(Biphen)₃] ( 7 ) and with MesLi complexes [{Li(THF)₂}₂VMes(Biphen)₂] · THF ( 8 ) and [{Li(DME)}VMes₂(Biphen)] ( 9 ) are formed. Reacting [VCl₃(THF)₃] with LiOMes in 1 : 1 to 1 : 4 ratios yields the componds [VCl_3–n(OMes)_n(THF)₂] (n = 1 ( 5 b ), 2 ( 5 a ), 3 ( 5 )) and [{Li(DME)₂}V(OMes)₄] ( 5 c ), the latter showing thermochromism due to a complexation/decomplexation equilibrium of the solvated cation. The mixed ligand mesityl phenolate complexes [{Li(DME)_n}{VMes₂(OAr)₂}] (OAr = IPP ( 10 ), TBP ( 11 ), OMes ( 12 ) (n = 2 or 3) and [{Li(DME)₂}{VMes(OMes)₃}] ( 15 ) are obtained by reaction of 1 , 2 , 5 a and 5 with MesLi. With [{Li(DME)₂(THF)}{VMes₃(IPP)}] ( 13 ) a ligand exchange product of 10 was isolated. Addition of LiOMes to [VMes₃(THF)] forming [Li(THF)₄][VMes₃(OMes)] ( 14 ) completes the series of [Li(solv.)_x][VMes_4–n(OMes)_n] (n = 1 to 4) complexes which have been oxidised to their corresponding neutral [VMes_4–n(OMes)_n] derivatives 16 to 19 by reaction with p‐chloranile. They were investigated by epr spectroscopy. The molecular structures of 1 , 3 , 5 , 5 a , 5 a – Br , 7 , 10 and 13 have been determined by X‐ray analysis. In 1 (monoclinic, C2/c, a = 29.566(3) Å, b = 14.562(2) Å, c = 15.313(1) Å, β = 100.21(1)°, Z = 8), 3 (orthorhombic, Pbcn, a = 28.119(5) Å, b = 14.549(3) Å, c = 17.784(4) Å, β = 90.00°, Z = 8), ( 5 ) (triclinic, P1, a = 8.868(1) Å, b = 14.520(3) Å, c = 14.664(3) Å, α = 111.44(1)°, β = 96.33(1)°, γ = 102.86(1)°, Z = 2), 5 a (monoclinic, P2₁/c, a = 20.451(2) Å, b = 8.198(1) Å, c = 15.790(2) Å, β = 103.38(1)°, Z = 4) and 5 a – Br (monoclinic, P2₁/c, a = 21.264(3) Å, b = 8.242(4) Å, c = 15.950(2) Å, β = 109.14(1)°, Z = 4) the vanadium atoms are coordinated trigonal bipyramidal with the THF molecules in the axial positions. The central atom in 7 (trigonal, P3c1, a = 20.500(3) Å, b = 20.500(3) Å, c = 18.658(4) Å, Z = 6) has an octahedral environment. The three Li(OEt₂)⁺ fragments are bound bridging the biphenolate ligands. The structures of 10 (monoclinic, P2₁/c, a = 16.894(3) Å, b = 12.181(2) Å, c = 25.180(3) Å, β = 91.52(1)°, Z = 4) and 13 (orthorhombic, Pna2₁, a = 16.152(4) Å, b = 17.293(6) Å, c = 16.530(7) Å, Z = 4) are characterised by separated ions with tetrahedrally coordinated vanadate(III) anions and the lithium cations being the centres of octahedral and trigonal bipyramidal solvent environments, respectively.     

Darstellung und Eigenschaften von Phthalocyaninato(2–)indaten(III) mit einzähnigen Acido-Liganden; Kristallstruktur von Tetra(n-butyl)ammonium-cis-difluoro-Phthalocyaninato(2–)indat(III)-Hydrat

Preparation and Properties of Phthalocyaninato(2–)indates(III) with Monodentate Acido Ligands; Crystal Structure of Tetra(n-butyl)ammonium cis -Difluorophthalocyaninato(2–)indate(III) Hydrate Tetra(n-butyl)ammonium cis-diacidophthalocyaninato(2–)indates(III) with the monodentate acido ligands fluoride, chloride, cyanide and formiate are synthezised by the reaction of chlorophthalocyaninatoindium(III) or cis-dihydroxophthalocyaninatoindate(III) with the respective tetra(n-butyl)ammonium salt or ammonium formiate and are characterized by their UV/VIS spectra and their vibrational spectra. The difluoro-complex salt crystallizes as a hydrate ((ⁿBu₄N)^cis[In(F)₂pc^2–] · H₂O) in the monoclinic space group P2₁/n (no. 14) with cell parameters: a = 13.081(3) Å, b = 13.936(2) Å, c = 23.972(2) Å; β = 97.79(1)°, Z = 4. Hexa-coordinated indium is surrounded by four isoindole nitrogen atoms (N_iso) and two cis-positioned fluorine atoms. The average In–F and In–N_iso distance are 2.0685(4) and 2.2033(5) Å, respectively, and the F–In–F angle is 81.5(1)°. The In atom is displaced outside the centre (Ct) of the N_iso plane towards the fluoride ligands: d(In–Ct) = 0.953(1) Å. The phthalocyaninato(2–) core is nonplanar (unsymmetrical concave distortion).     

Synthesis and Characterization of Methylzinc Tri(tert‐butyl)silylphosphanide as well as Related Sodium and Potassium Phosphanylzincates

The reaction of dimethylzinc and tri(tert‐butyl)silylphosphane in toluene yielded dimeric methylzinc tri(tert‐butyl)silylphosphanide ( 1 ) which crystallized tetrameric. Compound 1 was deprotonated with sodium in DME and the solvent‐separated dimeric ion pair [(dme)₃Na]⁺ [(dme)Na(MeZn)₂(μ‐PSitBu₃)₂]^? ( 2 ) was isolated. The reaction of 1 in THF with two equivalents of potassium and one equivalent of tri(tert‐butyl)silylphosphane gave dimeric [{tBu₃Si(H)P}{(thf)₂K}₂(MeZn)(PSitBu₃)]₂ ( 3 ). Both of these phosphanylzincates contain Zn₂P₂ cycles with Zn‐P bond lengths of approximately 237 pm, whereas in 1 larger Zn‐P bond lengths of 248.5 pm were found due to the larger coordination numbers of the phosphorus and zinc atoms.