Raman spectrum of carbonates MIICO3 in the 1100-1000cm −1 region: observation of the ν1, mode of the isotopic (C16O182O)2− ion

The Raman spectrum of a series of carbonates M^IICO₃ with aragonite or calcite structure has been reinvestigated in the 1100-1000 cm⁻¹ region, corresponding to the totally symmetric stretch (ν₁) of the (CO₃)²⁻ anion. Besides the very strong peak corresponding to the ν₁ mode of the (C¹⁶O₃)²⁻ ion, nearly all spectra exhibit a very weak satellite peak whose frequency agrees well with the calculated ν₁ frequency of the isotopic ion (C¹⁶O¹⁸₂O)⁻². Small deviations from the theoretical values are qualitatively discussed on the basis of vibrational couplings between near-neighbour anions.     

The Hexacyanodiborane(6) Dianion [B2(CN)6]2−

Diborane(6) dianions with substituents that are bonded to boron via carbon are very reactive and therefore only a few examples are known. Diborane(6) derivatives are the simplest catenated boron compounds with an electron‐precise B–B σ‐bond that are of fundamental interest and of relevance for material applications. The homoleptic hexacyanodiborane(6) dianion [B₂(CN)₆]²⁻ that is chemically very robust is reported. The dianion is air‐stable and resistant against boiling water and anhydrous hydrogen fluoride. Its salts are thermally highly stable, for example, decomposition of (H₃O)₂[B₂(CN)₆] starts at 200 °C. The [B₂(CN)₆]²⁻ dianion is readily accessible starting from 1) B(CN)₃²⁻ and an oxidant, 2) [BF(CN)₃]⁻ and a reductant, or 3) by the reaction of B(CN)₃²⁻ with [BHal(CN)₃]⁻ (Hal=F, Br). The latter reaction was found to proceed via a triply negatively charged transition state according to an S_N2 mechanism.     

Thermisch beständige Trialkyl-2,2,2-trifluor-1-(trifluormethyl)-ethoxy-phosphonium Iodide

Thermally Stable Trialkyl-2,2,2-trifluoro-1-(trifluoromethyl)-ethoxyphosphonium Iodides The phosphinites R¹R²POCH(CF₃)₂ (R¹ = R² = Me, tBu; R¹ = Me, R² = tBu) react with methyl iodide to give the thermally very stable phosphonium iodides [R¹R²MePOCH(CF₃)₂]⁺I^?. In the case of tBu₂POCH(CF₃)₂ a sublimable 1:1 adduct is formed with boron trichloride.     

Ordre local dans quelques verres fluores du systeme PbF2MIItF2MIIItF3 par EXAFS

The local environment of transition metal (M_t) and lead has been studied by EXAFS for some fluoride glasses in the system PbF₂M^II_tF₂M^III_tF₃ (M^II_t = Mn²⁺, Zn²⁺; M^III_t = Fe³⁺, Ga³⁺). Theoretical phase shifts and backscattering amplitude are used after testing with crystallized fluorides of various structures. Transition metals are sixfold coordinated and M_tF distances are very close to those known in crystallized compounds. Lead has eight to nine fluorine neighbors forming a very distorted polyhedra. Radial distributions, partially corrected for phase shifts, show a very weak second peak but the second neighbors nature and the distances cannot be determined without ambiguity.     

Vibrational spectral studies of ion-ion and ion-solvent interactions. I. Zinc nitrate in water

Raman and infrared line parameters of Zn(NO₃)₂-H₂O systems ranging from dilute solutions (25°C) to ionic liquids of low water content (75°C) are reported. At 25°C the solutions contain a very low concentration of inner sphere [Zn(ONO₂)(H₂O)₅]⁺, outer sphere [Zn(H₂O)₆]²⁺[NO₃]^–, Zn(H₂O) ₆ ²⁺ , and NO ₃ ^– (aq.). In the ionic liquids the ion triplet also exists. Manifestations of a change from the octahedral coordination of zinc to tetrahedral coordination when the water content is very low include the appearance of a 285 cm^–1 band from the zinc nitrate bond and a shift to higher frequencies of the band from zinc-water.     

Theoretical study of Na(4p2P) + Na(3s2S) and Cd(5p3P0) + Na(3s2S) collisions and their role in the energy transfer between Cd.* and Na

We have computed the cross sections for the energy transfer process Cd(5p³P₀) + Na(3s²S) → Cd(5s¹S) + Na(4p²P) and for the state changing collision Na(4p²P) + Na(3s²S) → Na(3d²D) + Na(3s²S), based on theoretical interaction potentials for the NaCd and Na2 systems, respectively. Our calculations shed light on the interpretation of experiments with laser excited Na+Cd vapour mixtures [1]. It turns out that Cd(5p³P₀), in rapid equilibrium with the doorway state Cd(5p³P₁), efficiently transfers energy to Na, populating the 4p²P state. The collisions with ground state Na cause a very fast conversion of the 4p³P₁ to the 3d²D state, from which the strongest emission is observed.     

Coordination Chemistry of Diiodine and Implications for the Oxidation Capacity of the Synergistic Ag+/X2 (X=Cl,Br, I) System

The synergistic Ag⁺/X₂ system (X=Cl, Br, I) is a very strong, but ill‐defined oxidant—more powerful than X₂ or Ag⁺ alone. Intermediates for its action may include [Ag_m(X₂)_n]^m+ complexes. Here, we report on an unexpectedly variable coordination chemistry of diiodine towards this direction: ( A )Ag‐I₂‐Ag( A ), [Ag₂(I₂)₄]²⁺( A ^?)₂ and [Ag₂(I₂)₆]²⁺( A ^?)₂?(I₂)_x≈0.65 form by reaction of Ag( A ) ( A =Al(OR^F)₄; R^F=C(CF₃)₃) with diiodine (single crystal/powder XRD, Raman spectra and quantum‐mechanical calculations). The molecular ( A )Ag‐I₂‐Ag( A ) is ideally set up to act as a 2 e^? oxidant with stoichiometric formation of 2 AgI and 2 A ^?. Preliminary reactivity tests proved this ( A )Ag‐I₂‐Ag( A ) starting material to oxidize n‐C₅H₁₂, C₃H₈, CH₂Cl₂, P₄ or S₈ at room temperature. A rough estimate of its electron affinity places it amongst very strong oxidizers like MF₆ (M=4d metals). This suggests that ( A )Ag‐I₂‐Ag( A ) will serve as an easily in bulk accessible, well‐defined, and very potent oxidant with multiple applications.     

Reactivity of the tetrahydroborate copper(I) complexes [(PR3)2Cu(η2-BH4)] (R = Ph,Cy) toward CO2, COS,and SCNPh

CO₂, COS, and SCNPh react under very mild conditions with the copper(I)-tetrahydroborate complexes [(PR₃)₂Cu(η²-BH₄)] (R = Ph, Cy); CO₂ and COS give the complexes [(PR₃)₂Cu(η²-O₂CH)] and [(PR₃)₂Cu(η²-OSCH)] respectively, whereas SCNPh gives the η²-dithiocarbamate complexes [(PR₃)₂Cu-(η²-S₂CNHPh)]. Addition of PPh₃ under CO₂ to solutions of [(PPh₃)₂Cu-(η²-BH₄)] gives [(PPh₃)₃Cu(η¹-O₂CH)] while addition of PPh₃ and NBu₄ClO₄ under CO₂ gives [(PPh₃)₃Cu(η-O₂CH)Cu(PPh₃)₃] ClO₄.     

Solubility parameters of poly(sulfonyldiphenylene phenylphosphonate) and its miscibility with poly(ethylene terephthalate)

The solubility behaviors of poly(sulfonyldiphenylene phenylphosphonate) (PSPPP), a very efficient flame retardant for poly(ethylene terephthalate) (PET), in more than 50 solvents were examined. Its solubility parameters (δ) were determined by the intrinsic viscosity and turbidic titration methods. The two methods obtained consistent results, δ = 21.0–21.6 J^1/2/cm^3/2 and δ = 21.0 J^1/2/cm^3/2, and the three‐dimensional solubility parameters were δ_d = 18.9 J^1/2/cm^3/2, δ_p = 8.8 J^1/2/cm^3/2, and δ_h = 5.9 J^1/2/cm^3/2. The miscibility of PSPPP with PET was estimated by the calculation of the heats of mixing, which were related to the difference between the solubility parameters of PSPPP and PET. Fourier transform infrared was used to examine the interactions between PSPPP and PET macromolecules, which were the internal factors of polymer–polymer miscibility. The results showed that PSPPP and PET were miscible within a very wide composition range, especially with less than 15 wt % PSPPP, a composition of interest for the preparation of flame‐retardant PET. © 2003 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 41: 2296–2301, 2003     

Detailed Analysis of the Crystal Structures and Magnetic Properties of a Dysprosium(III) Phthalocyaninato Sextuple-Decker Complex: Weak f–f Interactions Suppress Magnetic Relaxation

In the research field of single-molecule magnets (SMMs), lanthanoid–lanthanoid interactions, so-called f–f interactions, are known to affect the SMM properties, although their magnitudes are small. In this article, an SMM with very weak f–f interactions is reported, and the effects of the interactions on the SMM properties are discussed. X-ray structural analysis of the Dy^III-Cd^II-phthalocyaninato sextuple-decker complex (Dy₂Cd₃) reveals that the intramolecular Dy−Dy length in Dy₂Cd₃ is more than 13 Å, which is longer than the intermolecular Dy−Dy length. Even though the two Dy^III ions are far apart, intermolecular ferromagnetic dipole–dipole interactions are observed in Dy₂Cd₃. From detailed analysis of ac magnetic susceptibilities, quantum tunneling of the magnetization (QTM) in Dy₂Cd₃ is partially suppressed owing to the existence of very weak Dy−Dy interactions. Our results show that even very weak Dy−Dy interactions act as a dipolar bias, suppressing QTM.     

Coordination Chemistry of Diiodine and Implications for the Oxidation Capacity of the Synergistic Ag+/X2 (X=Cl,Br, I) System

The synergistic Ag⁺/X₂ system (X=Cl, Br, I) is a very strong, but ill‐defined oxidant—more powerful than X₂ or Ag⁺ alone. Intermediates for its action may include [Ag_m(X₂)_n]^m+ complexes. Here, we report on an unexpectedly variable coordination chemistry of diiodine towards this direction: ( A )Ag‐I₂‐Ag( A ), [Ag₂(I₂)₄]²⁺( A ⁻)₂ and [Ag₂(I₂)₆]²⁺( A ⁻)₂⋅(I₂)_x≈0.65 form by reaction of Ag( A ) ( A =Al(OR^F)₄; R^F=C(CF₃)₃) with diiodine (single crystal/powder XRD, Raman spectra and quantum‐mechanical calculations). The molecular ( A )Ag‐I₂‐Ag( A ) is ideally set up to act as a 2 e⁻ oxidant with stoichiometric formation of 2 AgI and 2 A ⁻. Preliminary reactivity tests proved this ( A )Ag‐I₂‐Ag( A ) starting material to oxidize n‐C₅H₁₂, C₃H₈, CH₂Cl₂, P₄ or S₈ at room temperature. A rough estimate of its electron affinity places it amongst very strong oxidizers like MF₆ (M=4d metals). This suggests that ( A )Ag‐I₂‐Ag( A ) will serve as an easily in bulk accessible, well‐defined, and very potent oxidant with multiple applications.     

Selective Deuterium Exchange of Pheny 1-2-Propanone

We required assymmetrically labelled phenyl-2-propanone for secondary deuterium isotope effect studies. While benzoyl acetone has been exchanged selectively at the methylene position,¹ attempts to deuterate phenyl-2-propanone selectively have failed.²,³ Since highly selective conditions for ketone exchange are not very common,⁴ I wish to report a very simple, mild, and convenient procedure for synthesizing PhCD₂COCH₃, and PhCH₂COCD₃ in high yield and isotopic purity.     

Gitterschwingungsspektren. LXIII. Be(lO3)2 · 4 H2O,ein Hydrat mit ungewöhnlicher Bindungsstruktur und Gitterdynamik

Lattice Vibration Spectra. LXIII. Be(IO₃)₂ · 4 H₂O, a Hydrate with Unusual Bonding and Lattice Dynamics The IR and Raman spectra (4000–50 cm^?1) of Be(IO₃)₂ · 4 H₂O and of deuterated specimens are recorded at 90 and 300 K and discussed in terms of the unusual relations of the masses of the atoms involved and the large polarization power of the beryllium ions. Thus, the translatory modes of the Be²⁺ ions (BeO₄ skeleton vibrations), the librations of the H₂O molecules, and the internal vibrations of the IO₃^? ions in the spectral regions of 300–400 and 600–1000 cm^?1 couple and coincide producing unusual v_H/v_D isotopic ratios of partly < 1. The H-bond donor strengths of the water molecules is so much increased (due to the very large ionic potential of Be²⁺ ions, viz. 49 e nm^?1) (synergetic effect) that the H-bonds formed are similar in strength as those in hydrates of hydroxides with the very strong H-bond acceptor group OH^? (v_OD of matrix isolated HDO molecules 2 074 and 2 244 (H₂O I) and 2 206 and 2 349 cm^?1 (H₂O II))     

Reaction des p-phenylphospholes avec le dicyclopentadienyl-difer-tetracarbonyle,synthese et etude spectrochimique des phosphaferrocenes

In boiling benzene, 1-phenyl-3,4-dimethylphosphole (L) with [(C₅H₅)Fe(CO)₂]₂ gives mainly a classical σ-complex in which L relaces one terminal CO. In boiling xylene, however, L also gives 3,4-dimethylphosphaferrocene and 2-phenyl-3,4-dimethylphosphaferrocene resulting from a P—Ph bond cleavage followed by a C-phenylation of the phospholyl nucleus in the second case. The same reaction with 1-phenylphosphole yields phosphaferrocene itself and a mixture of 2- and 3-phenylphosphaferrocene. The phosphaferrocenes thus prepared are exclusively acetylated at the phospholyl nucleus by the CH₃CGClAlCl₃ complex in CH₂Cl₂.With the unsubstituted phosphaferrocene, the acetylation takes place at the 2 and 3 positions (ratio $\text{2}\text{3}$ ～ $\text{85}\text{15}$) ¹H, ¹³C, ¹³P NMR and mass spectral data are given. The phosphaferrocene system is characterized by a very large ¹J(P—C) coupling (～60 Hz) and a very shielded phosphorus atom.     

Binukleare Nickel(II)‐Komplexe mit Oxalamidinaten als Brückenliganden: Synthese und Strukturen von Verbindungen mit planarer,tetraedrischer, tetragonal‐pyramidaler und oktaedrischer Koordination

Binuclear Nickel(II) Complexes with Oxalamidinates as Bridging Ligands: Synthesis and Struktures of Compounds with Planar, Tetrahedral, Tetragonal‐pyramidal, and Octahedral Coordination Oxalamidines R¹–NH–C(=NR²–C(=NR²)–NH–R¹ react selectively with Ni(acac)₂ under formation of the planar complexes [(acac)Ni(oxalamidinate)Ni(acac)]. Two crystal structures of the binuclear complexes with R = R′ = Ph ( 1 ) or p‐tolyl ( 2 ) show that the bridging oxalamidinates bind as bidendate ligands at each Nickel(II) atom. In contrast, the more sterically demanding fragment (Ph₃P)NiBr can only coordinate at sterically less demanding oxalamidinates to form complexes of the type [(Ph₃P)NiBr]₂(oxalamidinate) with tetrahedral coordination of Ni^II found by X‐ray analyses. Oxalamidines containing additional donor atoms in the side arms react very different, but in each case under formation of binuclear complexes, such as [(acac)₂Ni]₂( H₂E ) ( 8 ) (with R¹: –(CH₂)₃PPh₂, R²: p‐tolyl) in which the oxalamidine acts as bidentate neutral P,N‐ligand and the Ni^II atom has an octahedral environment. H₂F (with R¹: –(CH₂)₃PPh₂, R²: Mesityl), however, yields the planar complex [(acac)Ni]₂( F ) ( 9 ) with dianionic oxalamidinate under elimination of acetylacetone. There is no coordination of the donor groups of the side arms in the solid state of complex 9 , in contrast to the analogous binuclear complex [(acac)Ni]₂( H ) 10 (R¹: –CH₂–CH₂‐2‐pyridyl, R²: Mesityl). In this complex a distorted tetragonal‐pyramidal coordination of Ni^II is achieved. 2 reacts with an excess of LiCH₃ under elimination of the oxalamidinate to form the cluster compound Li₄(THF)₄Ni₂Me₈ in very good yields, while 9 yields the THF poorer cluster Li₂(THF)₂Li₂Ni₂Me₈ under similar conditions.     

[Ru(bpy)3]2+-trivalent titanium. A photochemical system with hydrogen production from aqueous solutions by visible light

Molecular hydrogen, detected by gas-chromatographic and mass-spectrometric measurements, was obtained by irradiating with visible light aqueous hydrochloridic solutions of [Ru(bpy)₃]²⁺ and trivalent titanium. The active species is the ³CT of [Ru(bpy)₃]²⁺, which is quenched by Ti(III). The suggested mechanism is an electron transfer with Ti(II) formation. The back reaction between [Ru(bpy)₃]³⁺ and Ti(II) is hindered by the very fast competitive reaction of Ti(II) (not stable in acid aqueous solutions) with H⁺, carrying to hydrogen evolution.     

Infrared Spectroscopic Studies on the Surface Chemistry of High‐Surface‐Area Gallia Polymorphs

Polymorphs α, β, and γ of Ga₂O₃ having hexagonal (corundum‐type), monoclinic and cubic (spinel‐type) structure, respectively, were prepared in a high‐surface‐area form, and characterized by powder X‐ray diffraction. Nitrogen adsorption at 77 K showed these gallia samples to have specific surface areas of 77 (α‐Ga₂O₃), 40 (β‐Ga₂O₃) and 120 m² g^?1 (γ‐Ga₂O₃). Fourier transform infrared spectroscopy of adsorbed carbon monoxide (at 77 K) and pyridine (at room temperature) showed that the three gallia polymorphs have a very similar surface Lewis acidity, regardless of their different crystal structures. This Lewis acidity was assigned, mainly, to coordinatively unsaturated tetrahedral Ga³⁺ ions situated on the surface of the small crystallites which constitute the different metal oxide varieties. Ga³⁺···CO adducts formed after CO adsorption gave (in all cases) a characteristic C–O stretching band at 2195–2200 cm^?1, while Lewis‐type adducts formed with adsorbed pyridine were characterized by IR absorption bands at 1610–1612 and 1446–1450 cm^?1. The three (partially hydroxylated) gallia polymorphs showed also a very weak Brønsted acidity, which they manifested by forming hydrogen‐bonded adducts with both CO and pyridine; however no protonation of adsorbed pyridine occurred.     

Thermodynamic and mechanistic studies of initial stages in propane aromatisation over Ga-modified H-ZSM-5 catalysts

¹³C MAS NMR has been performed in situ to investigate the early stages in the conversion of propane to aromatics on Ga-containing ZSM-5 catalysts. Propane 2-¹³C was used as labelled reactant. The scrambling of the ¹³C label in the very early stages of the propane conversion, even at 573 K, indicates that the first reaction intermediate is a protonated pseudocyclopropane (PPCP) species formed by activation of propane on a (Ga³⁺,O²⁻) ion pair and its protonation by a nearby Brønsted acidic site. This PPCP species can decompose in several ways leading to H₂, CH₄, C₂H₄, C₂H₆, and C₃H₆ as primary products. The very same molecules can also be produced as secondary products by cracking and hydrogen transfer at high conversion. CH⁺₃, C₂H⁺₅ and C₃H⁺₇ carbenium ions which are formed by decomposition of PPCP can react further with alkane or olefinic species. Reaction of CH⁺₃ (stabilised by a basic anionic framework oxygen) with propane (activated on a Ga site) may yield n-butane as indicated by the increase in the n-butane/i-butane ratio when the catalyst contains gallium.     

Sterically Demanding Novel Triazole Based Tertiary Phosphines: Synthesis,Transition Metal Chemistry and Catalytic Applications

Sterically demanding 2,6-dibenzhydryl-4-methylphenyl and 1,2,3-triazole based tertiary phosphines, [Ar*{1,2,3-N₃C(Ph)C(PR₂)}] (R=Ph, 3 ; R=ⁱPr, 4 ) were obtained by the temperature-controlled lithiation of 1-(2,6-dibenzydryl-4-methyl)-5-iodo-4-phenyl-1H-1,2,3-triazole ( 2 ) followed by the reaction with R₂PCl (R=Ph, ⁱPr). Treatment of 3 with H₂O₂, elemental sulfur and selenium yielded chalcogenides [Ar*{1,2,3-N₃C(Ph)C(P(E)Ph₂)}] (E=O, 5 ; E=S, 6 ; E=Se, 7 ). The reaction of 3 with [Pd(COD)Cl₂] in 1 : 1 molar ratio, afforded dimeric complex [Pd(μ₂-Cl)Cl{Ar*{1,2,3-N₃C(Ph)C(PPh₂)}-κ¹-P}]₂ ( 8 ), whereas the reactions of 3 and 4 with [Pd(η³-C₃H₅)Cl]₂ in 2 : 1 molar ratios produced complexes [Pd(η³-C₃H₅)Cl{Ar*{1,2,3-N₃C(Ph)C(PR₂)}-κ¹-P}] (R=Ph, 9 ; R=ⁱPr, 10 ). Treatment of 3 with [Pd(OAc)₂] in 1 : 1 molar ratio afforded a rare trinuclear complex [{Pd₃(OAc)₄}{Ar*{1,2,3-N₃C(C₆H₄)C(PPh₂)}-κ²-C,P}₂] ( 11 ). Treatment of 3 and 4 with [AuCl(SMe₂)] resulted in [AuCl{Ar*{1,2,3-N₃C(Ph)C(PR₂)}-κ¹-P}] (R=Ph, 12 ; R=ⁱPr, 13 ). Bulky phosphine 4 was very effective in Suzuki-Miyaura coupling and amination reactions with very low catalyst loading. Molecular structures of 3 – 5 , and 8 – 13 were confirmed by single-crystal X-ray diffraction studies.     

Sequence analysis and kinetic study of the polymerization of 1,4-bis(hydroxydimethylsilyl)benzene with sir2Cl2

²⁹Si NMR rate studies of the bulk reaction of 1,4-bis(hydroxydimethylsilyl)benzene (BHB) with dichlorodimethylsilane, dichloromethylphenylsilane, and dichlorodiphenylsilane show a very rapid kinetic equilibrium giving aryl-SiMe₂Cl groups in place of the aryl-SiMe₂OH of the BHB and OH groups in place of Cl in the dichlorosilane. This is followed by a slow condensation polymerization of the 1,4-bis(chlorodimethylsilyl)benzene with the hydroxy terminated disilane groups. The very rapid initial rates could be followed with ²⁹Si NMR using the INEPT pulse sequence despite the very long ²⁹Si relaxation times. Condensation polymerization is complete within minutes for BHB + SiMe₂Cl₂, but hours and days are required for the SiMePhCl₂ and SiPh₂Cl₂, respectively, at +22°C. Initial reaction kinetics in the presence of Cr(acac)₃ are not identical to those obtained using the INEPT pulse sequence and no relaxation reagent.