Darstellung und Eigenschaften von Tetra(n-butyl)ammonium-cis-trifluorophthalocyaninato(2–)zirconat(IV) und -hafnat(IV); Kristallstruktur von (nBu4N)cis[Hf(F)3pc2–]

Preparation and Properties of Tetra(n-butyl)ammonium cis -Trifluorophthalocyaninato(2–)zirconate(IV) and -hafnate(IV); Crystal Structure of (ⁿBu₄N) ^cis [Hf(F)₃pc^2–] cis-Dichlorophthalocyaninato(2–)metal(IV) of zirconium and hafnium reacts with excess tetra(n-butyl)-ammoniumfluoride trihydrate to yield tetra(n-butyl)-ammonium cis-trifluorophthalocyaninato(2–)metalate(IV), (ⁿBu₄N)^cis[M(F)₃pc^2–] (M = Zr, Hf). (ⁿBu₄N)^cis[Hf(F)₃pc^2–] crystallizes in the monoclinic space group P2₁/n (# 14) with cell parameters a = 13.517(1) Å, b = 13.856(1) Å, c = 23.384(2) Å, α = 92.67(1)°, Z = 4. The Hf atom is in a ”︁square base-trigonal cap”︁”︁ polyhedron, coordinating three fluorine atoms and four isoindole nitrogen atoms (N_iso). The Hf atom is sandwiched between the (N_iso)₄ and F₃ planes (d(Hf–Ct_N) = 1.218(3) Å; d(Hf–Ct_F) = 1.229(3) Å; Ct_N/F: centre of the (N_iso)₄, respectively F₃ plane). The average Hf–N_iso and Hf–F distances are 2.298 and 1.964 Å, respectively, the average F–Hf–F angle is 84.9°. The pc^2– ligand is concavely distorted. The optical spectra show the typical metal independent π-π* transitions of the pc^2– ligand at c. 14700 and 29000 cm^–1. In the FIR/MIR spectra vibrations of the MF₃ skeleton are detected at 545, 489, 274 cm^–1 (M = Zr) and 536, 484, 263 cm^–1 (M = Hf), respectively.     

Darstellung und Eigenschaften der Phthalocyaninato(2–)metallate(I) von Cobalt,Rhodium und Iridium; Kristallstruktur von Tetra(n-butyl)ammoniumphthalocyaninato(2–)cobaltat(I)-Aceton-Solvat

Syntheses and Properties of Phthalocyaninato(2–)metallates(I) of Cobalt, Rhodium, and Iridium; Crystal Structure of Tetra(n-butyl)ammonium Phthalocyaninato(2–)cobaltate(I) Acetone Solvate Cobaltphthalocyaninate(2–) reacts with tetra(n-butyl)ammonium boranate in acetone yielding soluble tetra(n-butyl)ammonium phthalocyaninato(2–)cobaltate(I). The green platelets of its acetone solvate crystallize in the monoclinic space group P1 2₁/c (no. 14) with cell parameters: a = 12.370(1) Å, b = 23.370(3) Å, c = 15.952(8) Å, β = 93.55(2)°, Z = 4. The Co atom is located in the centre of the distorted phthalocyaninate (waving distortion). The average Co–N_iso distance is 1.894 Å. Dichlorophthalocyaninato(2–)metal(III) acid of rhodium and iridium reacts in boiling sodium isopropylate/isopropanol with tetra(n-butyl)ammonium boranate yielding violet tetra(n-butyl)ammonium phthalocyaninato(2–)rhodate(I) and -iridate(I). The UV-VIS-NIR spectra show normal π–π* transitions of the pc^2– ligand which are shifted in the series Co < Rh < Ir to higher energy. Absorbances (in 10³ cm^–1) at 18.2/19.4/21.4/23.6 (Co), 22.0/22.8/40.4 (Rh) and 25.6 (Ir) are assigned to M → pc^2– charge transfer transitions. The vibrational spectra are typical for the pc^2– ligand. The very low absorbance of the IR bands at 916/1067/1330 cm^–1 is diagnostic for low-valent metal phthalocyaninates.     

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).     

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.     

Bis(triphenylphosphin)iminium-bis(methoxo)phthalocyaninato(2–)ferrat(III) – Synthese und Kristallstruktur

Bis(triphenylphosphine)iminium Bis(methoxo)phthalocyaninato(2–)ferrate(III) – Synthesis and Crystal Structure Chlorophthalocyaninato(2–)ferrate(III) reacts with bis(triphenylphosphine)iminium hydroxide in methanol/acetone solution to yield blue crystals of bis(triphenylphosphine)iminium bis(methoxo)phthalocyaninato(2–)ferrate(III). The complex salt crystallizes as an acetone/methanol solvate (^bPNP)[Fe(OCH₃)₂pc^2–] · (CH₃)₂CO · 1.5 CH₃OH in the triclinic space group P 1 (no. 2) with the cell parameters a = 13.160(5) Å, b = 15.480(5) Å, c = 17.140(5) Å, α = 97.54(5)°, β = 91.79(5)°, γ = 95.44(5)°. The Fe atom is located in the centre of the pc^2– ligand coordinating four isoindole N atoms (N_iso) of the pc^2– ligand and two O atoms of the methoxo ligands in a mutual trans arrangement. The average Fe–O and Fe–N_iso distances are 1.887 and 1.943 Å, respectively. The cation adopts the bent conformation (< P–N–P = 140.4(2)°) with P–N distances of 1.579(3) and 1.575(3) Å.     

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.     

Darstellung und Eigenschaften von trans-Di(fluoro)phthalocyaninato(2–)-rhenat(III); Kristallstruktur des linear-Bis(triphenylphosphin)iminium-Doppelsalzes l(PNP)trans[Re(F)2pc2–] · 0,33l(PNP)F · 2 H2O

Synthesis and Properties of trans -Di(fluoro)phthalocyaninatorhenate(III); Crystal Structure of the linear -Bis(triphenylphosphine)iminium Double Salt ^l (PNP) ^trans[Re(F)₂pc^2–] · 0.33^l (PNP)F · 2 H₂O trans-Bis(triphenylphosphine)phthalocyaninato(2–)rhenium(II) reacts with (ⁿBu₄N)F · 3 H₂O in acetone on air yielding trans-di(fluoro)phthalocyaninato(2–)rhenate(III), ^trans[Re(F)₂pc^2–]^–. The complex anion is precipitated as tetra(n-butyl)ammonium (ⁿBu₄N), or after addition of (PNP)HSO₄ as linear-bis(triphenylphosphine)iminium (^l(PNP)) salt. The latter crystallizes as a double salt of formula ^l(PNP)^trans[Re(F)₂pc^2–] · 0.33^l(PNP)F · 2 H₂O in the cubic space group I23 (no. 197) with the cell parameter a = 21.836(2) Å; V = 10412(2) ų; Z = 6. The Re atom is located in the centre of the (N_iso)₄ plane (N_iso: isoindole-N atom) and coordinates axially two fluorine atoms in a mutual trans position. The Re–N and Re–F distance is 2.035(6) and 1.798(7) Å, respectively. According to the short Re–F distance the asymmetric Re–F stretching vibration is observed in the MIR spectrum at 746 cm^–1. Obviously due to a large spin-orbit coupling, the complex salt with an electronic low-spin d⁴ ground state of Re^III (S = 1) is diamagnetic. Hence a sharp signal is observed at –126.1 ppm in the ¹⁹F NMR spectrum. The UV-VIS-NIR spectrum shows the typical π-π* transitions at 15000 (B), 29500 (Q) and 36900 cm^–1 (N) and trip-multiplet transitions at 9500/10500 cm^–1 and 13200/14100 cm^–1.     

trans-Bis(triphenylphosphin)phthalocyaninato(2–)rhenium(II): Synthese,Eigenschaften und Kristallstruktur

trans -Bis(triphenylphosphine)phthalocyaninato(2–)rhenium(II): Synthesis, Properties, and Crystal Structure Dirheniumheptoxide reacts with phthalodinitrile in boiling 1-chloronaphthalene and subsequent reprecipitation of the green raw product from conc. sulfuric acid to yield an oxo-phthalocyaninate of rhenium, which is reduced by molten triphenylphosphine forming dark green trans-bis(triphenylphosphine)phthalocyaninato(2–)rhenium(II), ^trans[Re(PPh₃)₂pc^2–]. The latter crystallizes triclinic in the space group P 1 with the cell parameters as follows: a = 11.512(2) Å, b = 12.795(2) Å, c = 12.858(2) Å, α = 64.42(2)°, β = 79.45(2)°, γ = 72.74(1)°; V = 1628.1(5); Z = 1. Re is in the centre of the (N_p)₄ plane (N_p: N1, N3) and coordinates two triphenylphosphine ligands axially in trans position. The average Re–N_p and Re–P distances are 2.007(1) and 2.516(3) Å, respectively. Despite the many extra bands the typical B, Q and N regions of the pc^2– ligand are observed at ca. 16500, 28900/32900 and 35300 cm^–1. A weak band group at ca. 8900 cm^–1 is attributed to a trip-multiplet transition, another one at ca. 14500 cm^–1 to a P → Re charge transfer. The vibrational spectra are dominated by internal vibrations of the pc^2– ligand. The very weak intensity of the IR bands at 905 and 1327 cm^–1 are diagnostic of the presence of Re^II.     

Synthese und Eigenschaften von (Acido)(nitrosyl)phthalocyaninato(2–)ruthenium

Synthesis and Properties of (Acido)(nitrosyl)phthalocyaninato(2–)ruthenium (Acido)(nitrosyl)phthalocyaninato(2–)ruthenium, [Ru(X)(NO)pc^2–] (X = F, Cl, Br, I, CN, NCO, NCS, NCSe, N₃, NO₂) is obtained by acidification of a solution of bis(tetra(n-butyl)ammonium) bis(nitro)phthalocyaninato(2–)ruthenate(II) in tetrahydrofurane with the corresponding conc. mineral acid or aqueous ammonium salt solution. The nitrite-nitrosyl conversion is reversal in basic media. The cyclic and differential pulse voltammograms show mainly three quasi-reversible one-electron processes at 1.05, –0.65 and –1.25 V, ascribed to the first ring oxidation and the stepwise reduction to the complexes of type {RuNO}⁷ and {RuNO}⁸, respectively. The B < Q < N regions in the electronic absorption spectra are still typical for the pc^2– ligand, but are each split into two strong absorptions (14500/16500(B); 28000/30500(Q); 34500/37000 cm^–1(N)), whose relative intensities strongly depend on the nature of the axial ligand X. In the IR spectra is active the N–O stretching vibration between 1827 (X = I) and 1856 cm^–1 (F), the C–N stretching vibration at 2178 (X = NCO), 2072 (NCS), 2066 (NCSe), 2093 cm^–1 (CN), the N–N stretching vibration of the azide ligand at 2045 cm^–1, the fundamentals of the nitrito(O) ligand at 1501, 932, and 804 cm^–1, and the Ru–X stretching vibration at 483 (F), 332 (Cl), 225 (Br), 183 (I), 395 (N₃), 364 (ONO), 403 (CN), 263 (NCS), and 231 cm^–1 (NCSe). In the resonance Raman spectra, excited in coincidence with the B region, the Ru–NO stretching vibration and the very intense Ru–N–O deformation vibration are selectively enhanced between 580 and 618 cm^–1, and between 556 and 585 cm^–1, respectively.     

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 .     

Darstellung,Kristallstrukturen und Schwingungsspektren von [Pt(N3)6]2– und [Pt(N3)Cl5]2–, 195Pt‐ und 15N‐NMR‐Spektren von [Pt(N3)nCl6–n]2– und [Pt(15NN2)n(N215N)6–n]2–, n = 0–6

Synthesis, Crystal Structures, and Vibrational Spectra of [Pt(N₃)₆]^2– and [Pt(N₃)Cl₅]^2–, ¹⁹⁵Pt and ¹⁵N NMR Spectra of [Pt(N₃)_nCl_6–n]^2– and [Pt(¹⁵NN₂)_n(N₂¹⁵N)_6–n]^2–, n = 0–6 By ligand exchange of [PtCl₆]^2– with sodium azide mixed complexes of the series [Pt(N₃)_nCl_6–n]^2– and with ¹⁵N‐labelled sodium azide (Na¹⁵NN₂) mixtures of the isotopomeres [Pt(¹⁵NN₂)_n(N₂¹⁵N)_6–n]^2–, n = 0–6 and the pair [Pt(¹⁵NN₂)Cl₅]^2–/[Pt(N₂¹⁵N)Cl₅]^2– are formed. X‐ray structure determinations on single crystals of (Ph₄P)₂[Pt(N₃)₆] ( 1 ) (triclinic, space group P1, a = 10.175(1), b = 10.516(1), c = 12.380(2) Å, α = 87.822(9), β = 73.822(9), γ = 67.987(8)°, Z = 1) and (Ph₄As)₂[Pt(N₃)Cl₅] · HCON(CH₃)₂ ( 2 ) (triclinic, space group P1, a = 10.068(2), b = 11.001(2), c = 23.658(5) Å, α = 101.196(14), β = 93.977(15), γ = 101.484(13)°, Z = 2) have been performed. The bond lengths are Pt–N = 2.088 ( 1 ), 2.105 ( 2 ) and Pt–Cl = 2.318 Å ( 2 ). The approximate linear azido ligands with N^α–N^β–N^γ‐angles = 173.5–174.6° are bonded with Pt–N^α–N^β‐angles = 116.4–121.0°. In the vibrational spectra the PtCl stretching vibrations of (n‐Bu₄N)₂[Pt(N₃)Cl₅] are observed at 318–345, the PtN stretching modes of (n‐Bu₄N)₂[Pt(N₃)₆] at 401–428 and of (n‐Bu₄N)₂[Pt(N₃)Cl₅] at 408–413 cm^–1. The mixtures (n‐Bu₄N)₂[Pt(¹⁵NN₂)_n(N₂¹⁵N)_6–n], n = 0–6 and (n‐Bu₄N)₂[Pt(¹⁵NN₂)Cl₅]/(n‐Bu₄N)₂[Pt(N₂¹⁵N)Cl₅] exhibit ¹⁵N‐isotopic shifts up to 20 cm^–1. Based on the molecular parameters of the X‐ray determinations the vibrational spectra are assigned by normal coordinate analysis. The average valence force constants are f_d(PtCl) = 1.93, f_d(PtN^α) = 2.38 and f_d(N^αN^β, N^βN^γ) = 12.39 mdyn/Å. In the ¹⁹⁵Pt NMR spectrum of [Pt(N₃)_nCl_6–n]^2–, n = 0–6 downfield shifts with the increasing number of azido ligands are observed in the range 4766–5067 ppm. The ¹⁵N NMR spectrum of (n‐Bu₄N)₂[Pt(¹⁵NN₂)_n(N₂¹⁵N)_6–n], n = 0–6 exhibits by ¹⁵N–¹⁹⁵Pt coupling a pseudotriplett at –307.5 ppm. Due to the isotopomeres n = 0–5 for terminal ¹⁵N six well‐resolved signals with distances of 0.03 ppm are observed in the low field region at –201 to –199 ppm.     

Bis(phthalocyaninato(2–)rhenium(II)): Synthesis,Properties, and Crystal Structure

Blue, paramagnetic bis(phthalocyaninato(2–)rhenium(II)) (μ_eff = 0,88 μ_B, per Re, at 300 K) is prepared by thermal decomposition of trans-bis(triphenylphosphine)phthalocyaninato(2–)rhenium(II), in boiling triphenylphosphine. It crystallizes in the triclinic space group P 1 with cell parameters as follows: a = 7.799(3) Å, b = 12.563(7) Å, c = 12.69(1) Å, α = 89.97(5)°, β = 94.14(5)°, γ = 106.39(4)°; Z = 1. Two cofacial phthalocyaninates are bonded together by a Re–Re bond with a Re–Re distance of 2.285(2) Å. The Re atoms are located distinctly outside the centre of the (N_iso)₄ planes by 0.426(3) Å. The Re–N_iso distance varies from 1.99(1) to 2.04(1) Å (average 2.02 Å). The pc^2– ligands are in an eclipsed conformation and concavely distorted. In the UV-VIS-NIR spectrum the B region is split into two bands of comparable intensity due to strong excitonic coupling. The Re–Re stretching vibration at 240 cm^–1 is selectively enhanced in the resonance Raman spectrum (λ_exc = 488 nm).     

Crystal Structure of Mixed Crystals of the Tetra(n-butyl)ammonium Salts of cis-Tetrafluorophthalocyaninato(2−)tantalate(V) and cis-Trifluorophthalocyaninato(2−)tantalate(IV)

cis-Trichlorophthalocyaninato(2?)tantalate(V) reacts with excess tetra(n-butyl)ammonium fluoride trihydrate yielding mixed crystals of the tetra(n-butyl)ammonium salts of cis-tetrafluorophthalocyaninato(2?)tantalate(V) and cis-trifluorophthalocyaninato(2?)tantalate(IV) in the ratio five to four. These crystallize in the monoclinic space group P2₁/ n with cell parameters: a = 13.368(2) Å, b = 13.787(2) Å, c = 23.069(3) Å, β = 93.35(1)°, Z = 4. Ta^v is octacoordinated with four F atoms and four N_iso atoms in an antiprismatic cis-arrangement. The Ta^v-F distance varies from 1.919(7) to 1.966(4) Å. Ta^IV is heptacoordinated with three F atoms in a cis-arrangement. The Ta^IV-F distance varies from 1.74(1) to 1.966(4) Å. The Ta atom is located out of the centre of the N₄ plane towards the F atoms by 1.234(3) Å. The Ta–N distances range from 2.261(6) to 2.310(6) Å.     

Ruthenium(II)-Phthalocyaninate(2–): Darstellung und Eigenschaften von Acido(carbonyl)phthalocyaninato(2–)ruthenat(II), [Ru(X)(CO)Pc2−]− (X = Cl,Br, I,NCO, NCS,N3)

Ruthenium(II) Phthalocyaninates(2–): Synthesis and Properties of (Acido)(carbonyl)phthalocyaninato(2–)ruthenate(II), [Ru(X)(CO)Pc^2?]^? (X = Cl, Br, I, NCO, NCS, N₃) (ⁿBu₄N)[Ru(OH)₂Pc^2?] is reduced in acetone with carbonmonoxid to blue-violet [Ru(H₂O)(CO)Pc^2?], which yields in tetrahydrofurane with excess (ⁿBu₄N)X acido(carbonyl)phthalocyaninato(2–)ruthenate(II), [Ru(X)(CO)Pc^2?]^? (X = Cl, Br, I, NCO, NCS, N₃) isolated as red-violet, diamagnetic (ⁿBu₄N) complex salt. The UV-Vis spectra are dominated by the typical π-π* transitions of the Pc^2? ligand at approximately 15100 (B), 28300 (Q₁) und 33500 cm^?1 (Q₂), only fairly dependent of the axial ligands. v(C? O) is observed at 1927 (X = I), 1930 (Cl, Br), 1936 (N₃, NCO) 1948 cm^?1 (NCS), v(C? N) at 2208 cm^?1 (NCO), 2093 cm^?1 (NCS) and v(N? N) at 2030 cm^?1 only in the MIR spectrum. v(Ru? C) coincides in the FIR spectrum with a deformation vibration of the Pc ligand, but is detected in the resonance Raman(RR) spectrum at 516 (X = Cl), 512 (Br), 510 (N₃), 504 (I), 499 (NCO), 498 cm^?1 (NCS). v(Ru? X) is observed in the FIR spectrum at 257 (X = Cl), 191 (Br), 166 (I), 349 (N₃), 336 (NCO) and 224 cm^?1 (NCS). Only v(Ru? I) is RR-enhanced.     

Gewellt und eben – La6(C2)‐Oktaederschichten in Lanthancarbidchloriden

Sheets of La₆(C₂) Octahedra in Lanthanum Carbide Chlorides – undulated and plane The reaction of Ln, LnCl₃ (Ln = La, Ce) and C yields the hitherto unknown compounds La₈(C₂)₄Cl₅, Ce₈(C₂)₄Cl₅, La₁₄(C₂)₇Cl₉, La₂₀(C₂)₁₀Cl₁₃, La₂₂(C₂)₁₁Cl₁₄, La₃₆(C₂)₁₈Cl₂₃ and La₂(C₂)Cl. The gold‐ resp. bronze‐coloured metallic compounds are sensitive to moisture. The reaction temperatures are 1030 °C, 1000 °C, 970 °C, 1020 °C, 1020 °C, 1080 °C and 1030 °C in the order of compounds given, which mostly crystallize in the monoclinic space group P2₁/c with a = 7.756(1) Å, b = 16.951(1) Å, c = 6.878(1) Å, β = 104.20(1)° (La₈(C₂)₄Cl₅), a = 7.669(2) Å, b = 16.784(3) Å, c = 6.798(1) Å, β = 104.05(1)° (Ce₈(C₂)₄Cl₅), a = 7.669(2) Å, b = 16.784(3) Å, c = 6.789(1) Å, β = 104.05(3)° (La₂₀(C₂)₁₀Cl₁₃), a = 7.770(2) Å, b = 47.038(9) Å, c = 6.901(1) Å, β = 104.28(3)° (La₂₂(C₂)₁₁Cl₁₄) and a = 7.764(2) Å, b = 77.055(15) Å, c = 6.897(1) Å, β = 104.26(3)° (La₃₆(C₂)₁₈Cl₂₃), respectively. La₁₄(C₂)₇Cl₉‐(II) crystallizes in Pc with a = 7.775(2) Å, b = 29.963(6) Å, c = 6.895(1) Å, β = 104.21(3)° and La₂(C₂)Cl in C2/c with a = 14.770(2) Å, b = 4.187(1) Å, c = 6.802(1) Å, β = 101.50(3)°. The crystal structures are composed of distorted C₂ centered La‐octahedra which are condensed into chains via common edges. Three and four such chains join into ribbons, and these are connected into undulated layers with Cl atoms between them. The variations of the structure principle are analyzed systematically.     

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).     

Bis(bis(triphenylphosphin)iminium)-μ-nitrido-bis(azidophthalocyaninato(2–)ferrat(IV))-Triiodid Diethylether-Disolvat: Synthese,Eigenschaften und Kristallstruktur

Bis(bis(triphenylphosphine)iminium) μ-Nitrido-bis(azidophthalocyaninato(2–)ferrate(IV)) Triiodide Diethylether Di-Solvate: Synthesis, Properties, and Crystal Structure Bis(bis(triphenylphosphine)iminium) μ-nitrido-bis(azidophthalocyaninato(2–)ferrate(IV)) triiodide is prepared as a diethylether di-solvate by substitution of μ-nitrido-bis(pyridinephthalocyaninato(2–)iron(IV)) pentaiodide with bis(triphenylphosphine)iminium azide in acetone and precipitation by slow diffusion of diethylether. The doublesalt crystallizes monoclinically in the space group C12/c1 with cell parameters: a = 34.567(9) Å, b = 20.237(9) Å, c = 21.251(5) Å, β = 119.79(2)°; Z = 4. The Fe atoms are located almost in the centre (Ct) of the (N_iso)₄ planes (d(Fe–Ct) = 0.080(1) Å; N_iso: isoindoline N atom). The average Fe–N_iso distance is 1.947(5) Å, the Fe-(μ-N) distance 1.650(1) Å. The Fe-(μ-N)–Fe skeleton is linear (177.4(4)°). Both waving pc^2– ligands are in a staggered conformation (skew angle φ = 38.5(5)°). Fe coordinates linear azide (d(Fe–N_azide) = 2.152(7) Å) with an angle of 121.2(6)°. The isolated triiodide ion is almost linear (d(I–I) = 2.936(2) Å). The PNP cation obtains an hybrid conformation (∠(P–N–P) = 157.4(2)°). The asymmetrical Fe-(μ-N)–Fe stretching vibration is observed in the IR spectrum at 997 cm^–1, the symmetrical one is selectively enhanced in the resonance Raman (RR) spectrum at 478 cm^–1. The corresponding I–I stretching vibrations of the triiodide ion are present in the actual spectra at 134 (IR) and 115 cm^–1 (RR). An IR band at 334 cm^–1 is attributed to the asymmetrical Fe–N_azide stretching vibration.     

Conformational Heterogeneity in Diphthalocyaninato(2–)metallates(III) of Sc,Y, In,Sb, Bi,La, Ce,Pr, and Sm

Potassium diphthalocyaninato(2–)metallate(III), K[M(pc^2–)₂] (M = Bi, La, Ce, Pr, Sm, Sb, In) has been prepared by melting the metal chloride, iodide or acetate with 1,2‐dicyanobenzene in the presence of potassium methylate. Crystallisation with tetra(n‐butyl)ammonium bromide or hydroxide ((ⁿBu₄N)Br/OH), tetra(n‐pentyl)ammonium chloride ((ⁿPe₄N)Cl) or bis(triphenylphosphine)iminium halide ((PNP)X; X = Br, I) yields the corresponding red‐purple complex salt (ⁿBu₄N)[M(pc^2–)₂] (M = Bi ( 1 ), La ( 3 ), Ce ( 2 )), (ⁿBu₄N)[M(pc^2–)₂] · x CH₃OH (M = Bi ( 5 ), Pr ( 6 ), Sm ( 7 ); 0 9 x 9 1), (ⁿPe₄N)[La(pc^2–)₂] ( 4 ), (ⁿBu₄N)[Pr(pc^2–)₂] · 2 py ( 10 ), (ⁿBu₄N)[Sb(pc^2–)₂] · 2 thf ( 11 ), (PNP)₂[M(pc^2–)₂]Br · 2 Et₂O (M = Sb ( 12 ), Bi ( 13 )), and (PNP)₂[In(pc^2–)₂]I · 2 Et₂O ( 14 ). Bronze coloured diphthalocyaninato(1–)metal(III) polyiodide, [M(pc^–)₂]I₂ (M = Sc, Y) has been prepared similarly in the presence of ammonium iodide. Reduction with (ⁿBu₄N)OH provides (ⁿBu₄N)[M(pc^2–)₂] · x CH₃OH (M = Y ( 8 ), Sc ( 9 ); 0 9 x 9 1). Spectral properties (UV/VIS/NIR; IR; resonance Raman) of diphthalocyaninates in their different ring oxidation states (2–/2–; 2–/1–; 1–/1–) are discussed. 1 – 3 crystallise in the tetragonal (P4/ncc), 5 – 9 in the orthorhombic (Pna2₁), 10 , 11 in the triclinic (P‐1), and 4 , 12 – 14 in the monoclinic crystal system ( 4 : P2₁/m; 12 : C2/c; 13 , 14 : P2/c). Ecliptic rotamers with skew angles ranging from 4.1° to 6.0° are found in 1 – 3 , and staggered rotamers with skew angles ranging from 35.8° to 45.0° are found in 4 – 14 . The mean M–N_i bond lengths and interplanar distances increase monotonically with the ionic radius of the metal ion. Both distances deviate notably from this linear correlation in the Sb^III and Bi^III derivatives. The discrepancy is presumably due to the sterical dominance of the ns² lone‐pair character. The actual size of eight co‐ordinated Sb^III and Bi^III is estimated to be R₈ ≈ 1.02(Sb)/1.11(Bi) Å. In every complex salt, the pc ligand is severely distorted from planarity and can adopt domed, saddled, waved and mixed non‐planar conformations; the crystal symmetry is the most important factor for the conformational heterogeneity.     

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 ).