Mass-spectrometric study of tetrafluorohydrazine and the products resulting from its breakdown under electron impact

Conclusions Electron-impact methods have been used to study positive (NF⁺, NF₂ ⁺, N₂F₂ ⁺) and negative (F^–, F₂ ^–, N₂F^–, NF₂ ^–) ion formation in the mass spectra of tetrafluorohydrazine and its decomposition products.Translated from Izvestiya Akademii Nauk SSSR, Seriya Khimicheskaya, No. 6, pp. 1306–1311, June, 1978.The authors would like to thank V. Ya. Rosolovskii for a discussion of the results obtained in this work.     

Vibrational spectroscopy of complex compounds of gold pentafluoride

IR and Raman spectra of X⁺ AuF₆ ^? (X=CIF₂, CIO₂, CIOF₂, CIF₄, CIF₆) were studied. The vibration frequencies of these compounds in the solid phase and in solutions in anhydrous HF were assigned. Peculiar features of the vibrational spectra of solid X⁺ AuF₆ ^?, associated both with structural transformations of cations and anions in the crystal lattice field and cation—anion interactions and also with the Jahn—Teller effect, Fermi resonance, non-rigid intramoleciular rearrangements.,etc., were discussed.     

Fluorierung von Cyanurchlorid und Tieftemperatur-Kristallstruktur von [(ClCN)3F]+ [AsF6]−

Fluorination of Cyanuric Chloride and Low-Temperature Crystal Structure of [(ClCN)₃F]⁺[AsF₆]^? The low-temperature fluorination of cyanuric chloride, (ClCN)₃, with F₂/AsF₅ in SO₂F₂ solution yielded the salt [(ClCN)₃F]⁺ [AsF₆]^? ( 1 ) essentially in quantitative yield. Compound 1 was identified by a low-temperature single crystal X-ray structure determination: R 3 c, trigonal, a = b = 10.4246(23) Å, c = 15.1850(24) Å, V = 1429.1(4) Å 3, Z = 6, R_F = 0.056, R_w = 0.076 (for significant reflections), R_F = 0.088, R_w = 0.079 (for all reflections). Fluorination of neat (ClCN)₃ with [NF₄]⁺ [Sb₂F₁₁]^? yielded NF₃, CClF₃, SbF₃, N₂ and traces of CF₄. A qualitative scale for the oxidizing strength of the oxidative fluorinators NF₄⁺ and (XCN)₃F⁺ (X = H, F, Cl) has been computed ab initio.     

On the synthesis of the N2F+5 cation. A critical comment on the paper by Toy and Stringham.

Toy and Stringham recently reported [1] the synthesis of N₂F⁺₅ (CF₃)₃CO^-, a salt containing the novel pentafluorohydrazinium cation. This cation would be of significant academic and practical interest [2] since it would constitute the first known example of a substituted NF⁺₄ cation, i.e. an NF⁺₄ cation in which a fluorine ligand is replaced by an NF₂ group. According to the authors of [1], N₂F⁺₅(CF₃)₃CO^- was formed in a very unusual reaction involving the transfer of a fluorine cation from (CF₃)₃COF to N₂F₄ according to:

     

Gas‐phase reactions of XH3+ (X = C,Si, Ge) with NF3: a comparative investigation on the detailed mechanistic aspects

The gas‐phase reaction of CH₃⁺ with NF₃ was investigated by ion trap mass spectrometry (ITMS). The observed products include NF₂⁺ and CH₂F⁺. Under the same experimental conditions, SiH₃⁺ reacts with NF₃ and forms up to six ionic products, namely (in order of decreasing efficiency) NF₂⁺, SiH₂F⁺, SiHF₂⁺, SiF⁺, SiHF⁺, and NHF⁺. The GeH₃⁺ cation is instead totally unreactive toward NF₃. The different reactivity of XH₃⁺ (X = C, Si, Ge) toward NF₃ has been rationalized by ab initio calculations performed at the MP2 and coupled cluster level of theory. In the reaction of both CH₃⁺ and SiH₃⁺, the kinetically relevant intermediate is the fluorine‐coordinated isomer H₃X‐F‐NF₂⁺ (X = C, Si). This species forms from the exoergic attack of XH₃⁺ to one of the F atoms of NF₃ and undergoes dissociation and isomerization processes which eventually result in the experimentally observed products. The nitrogen‐coordinated isomers H₃X‐NF₃⁺ (X = C, Si) were located as minimum‐energy structures but do not play an active role in the reaction mechanism. The inertness of GeH₃⁺ toward NF₃ is also explained by the endoergic character of the dissociation processes involving the H₃Ge‐F‐NF₂⁺ isomer. Copyright © 2009 John Wiley & Sons, Ltd.     

Complex of cesium and rubidium fluorides with bromine trifluoride

Vibrational spectra are reported for the new complexes CsF·3BrF₃, RbF·3BrF₃, and RbF·2BrF₃ and the previously known complex CsF·2BrF₃. The spectra suggest that these compounds are salts having general formulas M⁺Br₃F^?₁₀ and M⁺Br₂F^?₇.     

Fluorine absorption spectra and some fluorides in condensed state

The absorption spectra of liquid F₂, NF₃, N₂F₄, CF₄, BF₃, NF₃, SF₆ have been obtained at diminished temperatures in the near ultra-violet region of the spectrum. It is shown that the absorption spectrum does not differ from the spectra in the gaseous phase, therefore the elementary absorption act is characterized by the cross section of photon absorption by an individual molecule. The absorption cross sections of the above mentioned molecules are represented in the liquid phase, which do not differ strongly from absorption cross sections of these molecules in the gaseous phase. The dependence of the absorption cross sections of liquid fluorine on its concentrations in solutions with N₂, Ar, NF₃, O₂ at - 196°C has been studied. The cross sections of photon absorption by the fluoride molecule in different liquid media with small fluorine concentrations have been obtained.     

Vibrational spectra of trinitromethane derivatives

Spectroscopic parameters of trinitromethane derivatives RC(NO₂)₃ (R = F, Cl, Br, I, NC, NF₂, N₃) were determined. Vibrational frequencies and modes were calculated and the assignment of experimental spectra was performed. Spectral features due to the mutual influence of the C(NO₂)₃ group and other atomic groups and particular atoms were revealed.     

The two-photon excitation spectrum of triphenylene in n-heptane single crystals: Chem. Phys. Letters 57 (1978) 496

Chemiluminescence spectra and photon yields resulting from reactions of copper atoms with N₂O, O₂, NO, NF₃, SF₆, F₂, Cl₂, Br₂, and I₂ have been obtained between 200 and 1100 nm. The most interesting feature of these spectra is the strong and peculiar emission from copper atoms observed in the Cu + NF₃ reaction; population inversion has been obtained between some of the Cu states and it is suggested that this is due to energy transfer from N₂(A) formed in the reaction to copper atoms.     

Formation Mechanism of NF4+ Salts and Extraordinary Enhancement of the Oxidizing Power of Fluorine by Strong Lewis Acids

Although the existence of the NF₄⁺ cation has been known for 51 years, and its formation mechanism from NF₃ , F₂ , and a strong Lewis acid in the presence of an activation energy source had been studied extensively, the mechanism had not been established. Experimental evidence had shown that the first step involves the generation of F atoms from F₂ , and also that the NF₃⁺ cation is a key intermediate. However, it was not possible to establish whether the second step involved the reaction of a F atom with either NF₃ or the Lewis acid (LA). To distinguish between these two alternatives, a computational study of the NF₄ , SbF₆ , AsF₆ , and BF₄ radicals was carried out. Whereas the heats of reaction are small and similar for the NF₄ and LAF radicals, at the reaction temperatures, only the LAF radicals possess sufficient thermal stability to be viable species. Most importantly, the ability of the LAF radicals to oxidize NF₃ to NF₃⁺ demonstrates that they are extraordinary oxidizers. This extraordinary enhancement of the oxidizing power of fluorine with strong Lewis acids had previously not been fully recognized.     

Crystal Growth and Crystal Structures of Gold(V) Compounds: Cu(AuF6)2, Ag(AuF6)2, and O2(CuF)3(AuF6)4 ⋅ HF

Crystal growth from anhydrous hydrogen fluoride solutions of M²⁺ (M=Cu, Ag) and [AuF₆]⁻ gave M(AuF₆)₂ salts (M=Cu, Ag). Similar attempts to prepare single crystals of the corresponding nickel, zinc and magnesium salts failed. The crystal structure of Cu(AuF₆)₂ consists of layers of Cu²⁺ cations connected by [AuF₆]⁻ anions, thus forming slabs. Only van der Waals interactions exist between adjacent slabs. The crystal structure of Ag(AuF₆)₂ consists of a three-dimensional framework in which Ag⁺ cations are linked by [AuF₆]⁻ anions. Both structures are members of the M^II(X^VF₆)₂ family, in which seven different structure types have been observed to date. In the crystal structure of O₂(CuF)₃(AuF₆)₄ ⋅ HF, the bridging AuF₆ units connect [−Cu−F−Cu−F−]_∞ chains to form stacks between which O₂⁺ cations and HF molecules are located.     

Xenon-nitrogen chemistry: gas-phase generation and theoretical investigation of the xenon-difluoronitrenium ion F2N-Xe+

The xenon–difluoronitrenium ion F₂N? Xe⁺, a novel xenon–nitrogen species, was obtained in the gas phase by the nucleophilic displacement of HF from protonated NF₃ by Xe. According to Møller–Plesset (MP2) and CCSD(T) theoretical calculations, the enthalpy and Gibbs energy changes (ΔH and ΔG) of this process are predicted to be ?3 kcal mol^?1. The conceivable alternative formation of the inserted isomers FN? XeF⁺ is instead endothermic by approximately 40–60 kcal mol^?1 and is not attainable under the employed ion‐trap mass spectrometric conditions. F₂N? Xe⁺ is theoretically characterized as a weak electrostatic complex between NF₂⁺ and Xe, with a Xe? N bond length of 2.4–2.5 Å, and a dissociation enthalpy and free energy into its constituting fragments of 15 and 8 kcal mol^?1, respectively. F₂N? Xe⁺ is more fragile than the xenon–nitrenium ions (FO₂S)₂NXe⁺, F₅SN(H)Xe⁺, and F₅TeN(H)Xe⁺ observed in the condensed phase, but it is still stable enough to be observed in the gas phase. Other otherwise elusive xenon–nitrogen species could be obtained under these experimental conditions.     

Toward the preparation of the HAuF6, HAu2F11, and HAu3F16 superacids: Theoretical study

We apply the B3LYP and QCISD theoretical methods with the 6-311++G(d,p) basis set and the LANL2DZ effective core potentials to investigate the reaction paths leading to the preparation of the HAuF₆, HAu₂F₁₁, and HAu₃F₁₆ superacids. The Gibbs free energies of deprotonation of these systems are calculated to estimate their acid strength. The thermodynamic stability of the corresponding anionic precursors ((AuF₆)^–, (Au₂F₁₁)^–, and (Au₃F₁₆)^–) and their vertical excess electron detachment energies are evaluated and discussed. The suggested route of the HAu₂F₁₁ preparation involves the F^– attachment to the Au₂F₁₀ reactant which results in the formation of the (Au₂F₁₁)^– anion whose protonation yields the HAu₂F₁₁ superacid. The suggested HAuF₆ superacid preparation route is based on a qualitatively similar scheme and involves the conversion of the AuF₅ reactant into the (AuF₆)^– anion followed by its protonation. The proposed path for the HAu₃F₁₆ superacid preparation involves the attachment of AuF₅ to HAu₂F₁₁.     

A raman,infra-red and n.m.r. spectroscopic study of the pentafluorotellurate(IV) ion

The Raman, and infra-red spectra of Na⁺, K⁺, Rb⁺, Cs⁺, NH₄⁺, C₅H₅NH⁺ and $\text{n}$-Bu₄N⁺ salts of the TeF₅^- ion are reported. They are assigned C_s symmetry. ¹⁹F n.m.r. spectra of the $\text{n}$-Bu₄N⁺ salt show J(F_ax-F_eq)50.4Hz, J(¹⁹F_eq-¹²⁵Te)1375.7Hz, J(¹⁹F_ax-¹²⁵Te)2883.3Hz and J(¹⁹F_eq-¹²³Te)1143.8Hz. No n.m.r. evidence was found for TeF₆^2-.     

Structural and vibrational characterization of [KrF][AuF6] and α-[O2][AuF6] using single crystal X-ray diffraction, Raman spectroscopy and electron structure calculations

The salt [KrF][AuF₆] has been prepared by the direct oxidation of gold powder in anhydrous HF at 20 °C using the potent oxidative fluorinating agent KrF₂. The KrF⁺ salt readily oxidizes molecular oxygen at ambient temperature to yield [O₂][AuF₆]. Variable temperature Raman spectroscopy has been used to identify a reversible phase transition in [O₂][AuF₆], which occurs between −114 and −118 °C. Single crystal X-ray diffraction has been used to characterize the low-temperature, α-phase of [O₂][AuF₆]. The phase transition is attributed to ordering of the O₂⁺ cation in the crystal lattice, which is accompanied by minor distortions of the AuF₆⁻ anion. The α-phase of [O₂][AuF₆] crystallizes in the triclinic space group , with a=4.935(6) Å, b=4.980(6) Å, c=5.013(6) Å, α=101.18(1)°, β=90.75(2)°, γ=101.98(2)°, V=342.97 Å³, Z=1, and R₁=0.0481 at −122 °C. The structure of the precursor, [KrF][AuF₆], has also been determined by single crystal X-ray diffraction and crystallizes in the monoclinic space group Cc with a=7.992(3) Å, b=7.084(3) Å, c=10.721(4) Å, β=105.58(1)°, V=584.8(4) Å³, Z=4 and R₁=0.0389 at −125 °C. The KrF⁺ and AuF₆⁻ ions interact by means of a FKr---FAu fluorine bridge that is bent by 125.3(7)° about the bridge fluorine. The KrF_t and Kr---F_b bond lengths in [KrF][AuF₆] were determined to be 1.76(1) and 2.15(1) Å, respectively. The energy minimized structures of the [KrF][AuF₆] ion-pair and the AuF₆⁻ anion have been determined at the Hartree-Fock (HF), MP2 and local density functional (LDF) levels of theory. These calculations have also been used to assign the vibrational spectrum of the [KrF][AuF₆] ion-pair in greater detail and to reassign the vibrational spectrum of the AuF₆⁻ anion.     

Recent achievements in the synthesis and characterization of metal hexafluorantimonates and hexafluoroaurates

The efforts to prepare new MSbF₆/MSb₂F₁₁ (A = In, Cu, Au, Hg) compounds were partly successful. Reaction between InBF₄ and excess SbF₅ in anhydrous hydrogen fluoride (aHF) yields a mixture of InF₃·3SbF₅ and unidentified SbF₃·xSbF₅. The attempts to synthesize MSbF₆/MSb₂F₁₁ salts (A = Au, Hg) by controlled reduction of Au(SbF₆)₂ or Hg(SbF₆)₂ solutions in aHF/SbF₅ by elemental hydrogen, resulted in the precipitation of metallic Au or Hg₂(Sb₂F₁₁)₂. In the reaction of metallic Cu and deficit SbF₅, the synthesis of CuSbF₆ was achieved. CuSbF₆, like CuAsF₆, is a rare example of a Cu(I) compound in a pure fluorine environment.Vibrational spectra of M(II) hexafluoroantimonates (M = Ni, Fe, Co, Cu, Cr, Pd, Ag) were reinvestigated. It was found that many of them originally assigned to M(SbF₆)₂ compounds, belong to their mixtures with oxonium salts H₃OM(SbF₆)₃, H₃OSbF₆, and/or H₃OSb₂F₁₁.Reactions were studied between MF₂/2AuF₃ (M = Ni, Cu, Ag, Zn, Cd and Hg) and KrF₂ or UV-irradiated elemental fluorine in aHF as solvent at room temperature. On the basis of mass balances, Raman spectroscopy and X-ray powder diffraction analysis it can be concluded that the isolated solids have structures that can be considered in terms of an M(AuF₆)₂ formulation. Previously reported syntheses and characterization of M(AuF₆)₂ (M = Mg, Ca, Sr, Ba) were reinvestigated. In the case of M = Ba two different Au⁻F₆ salts were isolated.Raman spectra of the majority of synthesized metal hexafluoroaurates (M = Ni, Cu, Ag, Zn, Cd, Hg, Mg and Ca) show more bands than expected for regular Au⁻F₆ anion, indicating that the salts obtained exhibit relatively strong cation-anion interactions. The Raman spectra of the remaining Sr and Ba salts show the presence of more regular Au⁻F₆ octahedra, indicating weak cation-anion interactions.     

A comparison of enthalpies of tetrafluoroammonium salts and other fluoro-nitrogen species

It is shown that enthalpies of nitrogen fluorides and oxo fluorides deviate markedly from enthalpies of corresponding hydroxo compounds, whereas there is good agreement (circa 2%) between carbon mono, di and trifluoro compounds and their hydroxo analogues. The extent of deviation correlates with the extra number of lone pair repulsions of fluoro over oxo compounds. The enthalpy of NF₄⁺(g) can be extrapolated from the other (N,F) and (N,O,F) compounds. The enthalpies of solid NF₄⁺ salts are close to those of corresponding NO₂⁺ salts and from this an exothermic heat of formation for NF₄⁺F^? is predicted.     

Investigation of Molecular Alkali Tetrafluorido Aurates by Matrix-Isolation Spectroscopy

Molecular alkali tetrafluorido aurate ion pairs M[AuF₄] (M=K, Rb, Cs) are produced by co-deposition of IR laser-ablated AuF₃ and MF in solid neon under cryogenic conditions. This method also yields molecular AuF₃ and its dimer Au₂F₆. The products are characterized by their Au–F stretching bands and high-level quantum-chemical calculations at the CCSD(T)/triple-ζ level of theory. Structural changes in AuF₄⁻ associated with the coordination of the anion to different alkali cations are proven spectroscopically and discussed.     

Synthesis and Characterization of Fluorodinitroamine,FN(NO2)2

NF₃ and N(NO₂)₃ are known compounds, whereas the mixed fluoronitroamines, FN(NO₂)₂ and F₂NNO₂, have been unknown thus far. One of these, FN(NO₂)₂, has now been prepared and characterized by multinuclear NMR and Raman spectroscopy. FN(NO₂)₂ is the first known example of an inorganic fluoronitroamine. It is a thermally unstable, highly energetic material formed by the fluorination of the dinitramide anion using NF₄⁺ salts as the preferred fluorinating agent.