129Xe-Kernresonanzuntersuchungen von Xenonverbindungen. I. Einfache Xenonderivate

¹²⁹Xenon-NMR Spectra of Xenon Compounds. I. Simple Xenon Derivatives The ¹²⁹Xe-NNR Spectra of simple Xenon compounds have been measured. The analytical value of this method is described. The spectra of Xe, XeF₂, XeF₄, XeOF₄, and XeO₃ are in agreement with the known structures, while XeF₃ is found as Xe₄F₂₄ in inert solution at low temperatures. This had been described recently.     

Zur kenntnis von AlF3 und InF3 [1]

The lattice constants of AlF₃ and InF₃ were redetermined (AlF₃: a = 4.9254(7) Å, c = 12.4472(52) Å; InF₃: a = 5.4103(7) Å, c = 14.3775(21) Å). Using single crystals, the structures of both fluorides were refined anisotropically. The Madelung Part of Lattice Energy, MAPLE, is calculated and compared with the MAPLE values of other fluorides. The structures are discussed with respect to and compared with hypothetical forms containing undisturbed closest packings of F_?.     

Mass spectrometry of graphite intercalation compounds of binary fluorides of xenon,xenon oxide tetrafluoride and arsenic pentafluoride

Thermal decomposition of the intercalates of XeF₆, XeF₄, XeOF₄ and AsF₅ in graphite has been studied using a molecular beam source mass spectrometer. The product of the hydrolysis of the intercalate of XeF₆ has also been examined. The species liberated at low temperatures (T < 150°C) may be either the ones originally intercalated (XeOF₄, AsF₅) or the next lower oxidation state (XeF₄ from XeF₆, and XeF₂ from XeF₄. At higher temperatures (200-400°C) the intercalated XeF₄, XeF₂ or XeF₄ attack the graphite lattice, and evolve large quantities of xenon, and subsequently fluorocarbons and/or carbonyl fluoride. In contrast, the intercalate of AsF₅ evolves AsF₅ as the dominant gas over most of the temperature range, with a much lower degree of fluorination of the graphite lattice. The hydrolysis product of the XeF₆ intercalate was similar to the intercalate of XeF₄, but the evidence indicates that the hydrolysis proceeded well beyond XeOF₄. The extent of attack upon the graphite lattice correlates well with the oxidizing or fluorinating ability of the intercalated compound.     

Solid-state energetics and electrostatics: Madelung constants and Madelung energies

The Madelung constants of ionic solids relate to their geometry and electrostatic interactions. Furthermore, because of issues in their evaluation, they are also of considerable mathematical interest. The corresponding Madelung (electrostatic, coulomb) energy is the principal contributor to the lattice energies of ionic systems, and these energies largely influence many of their physical properties. The Madelung constants are here defined and their properties considered. A difficulty with their application is that they may be defined relative to various lattice distances, and with various conventions for inclusion of the charges, leading to possible confusion in their use. Instead, the unambiguous Madelung energy, E(M), is to be preferred in chemistry. An extensive list of Madelung energies is presented. From this data set, it is observed that there is a strong linear correlation between the lattice energies of ionic solids, U(POT), and their Madelung energies: U(POT)/kJ mol(-1) = 0.8519E(M) + 293.9. This correlation establishes that the lattice energy, U(POT), for ionic solids is about 15% smaller than the attractive Madelung energy, the difference arising from the repulsions unaccounted for by the solely coulombic Madelung energy calculation. Correlations of U(POT) against E(M) for alkali metal hydrides and transition metal compounds, each having considerable covalency, show much reduced Madelung contributions to the lattice energy. These correlations permit ready estimation of lattice energies, and are the first to be based on actual data rather than a broad analysis. The independent volume-based thermodynamic (VBT) method, which relies on a separate correlation with the formula unit volume of the ionic material, complements these correlations.     

A Raman spectroscopic study of the XeOF4/XeF2 system and the X-ray crystal structure of α-XeOF4·XeF2

The mixed oxidation state complexes, α-XeOF₄·XeF₂ and β-XeOF₄·XeF₂, result from the interaction of XeF₂ with excess XeOF₄. The X-ray crystal structure of the more stable α-phase shows that the XeF₂ molecules are symmetrically coordinated through their fluorine ligands to the Xe(VI) atoms of the XeOF₄ molecules which are, in turn, coordinated to four XeF₂ molecules. The high-temperature phase, β-XeOF₄·XeF₂, was identified by low-temperature Raman spectroscopy in admixture with α-XeOF₄·XeF₂; however, the instability of the β-phase precluded its isolation and characterization by single-crystal X-ray diffraction. The Raman spectrum of β-XeOF₄·XeF₂ indicates that the oxygen atom of XeOF₄ interacts less strongly with the XeF₂ molecules in its crystal lattice than in α-XeOF₄·XeF₂. The ¹⁹F and ¹²⁹Xe NMR spectra of XeF₂ in liquid XeOF₄ at −35 °C indicate that any intermolecular interactions that exist between XeF₂ and XeOF₄ are weak and labile on the NMR time scale. Quantum-chemical calculations at the B3LYP and PBE1PBE levels of theory were used to obtain the gas-phase geometries and vibrational frequencies as well as the NBO bond orders, valencies, and NPA charges for the model compounds, 2XeOF₄·XeF₂, and XeOF₄·4XeF₂, which provide approximations of the local XeF₂ and XeOF₄ environments in the crystal structure of α-XeOF₄·XeF₂. The assignments of the Raman spectra (−150 °C) of α- and β-XeOF₄·XeF₂ have been aided by the calculated vibrational frequencies for the model compounds. The fluorine bridge interactions in α- and β-XeOF₄·XeF₂ are among the weakest for known compounds in which XeF₂ functions as a ligand, whereas such fluorine bridge interactions are considerably weaker in β-XeOF₄·XeF₂.     

Electronic energy structure of MBiS2 (M = Li, Na, K) calculated with allowance for the difference between the M-S and Bi-S bond lengths

The modified augmented plane wave method (WIEN2k program) was used to study the electronic energy structure and calculate the SK-absorption spectra of LiBiS₂, NaBiS₂, and KBiS₂. The crystal structures of the compounds were modeled using symmetric structures, in which each sulfur atom was surrounded by three alkali metal atoms and three bismuth atoms in such a way that the alkali metal-sulfur and bismuth-sulfur bond length differed. This difference between bond lengths was calculated from the sum of the ionic radii of the components of compounds and by the geometry optimization of the crystal lattice. The two variants of calculation allowed us to check the applicability of Pauling’s idea about preservation of the bond lengths of elements in compounds for modeling the crystal structures of LiBiS₂, NaBiS₂, and KBiS₂. The SK absorption spectra and optically forbidden bands were calculated.     

Spontaneous reactions of xenon,flourine and antimony pentaflouride

Mixtures of xenon and fluorine gases react spontaneously with liquid antimony pentafluoride in the dark to form solutions of XeF⁺Sb₂F^?₁₁. Dixenon cation, Xe⁺₂, is formed as a labile intermediate product and is oxidized by the fluorine to XeF⁺ cation. The rate of the overall reaction is proportional to the partial pressure of xenon and the partial pressure of fluorine. This direct combination of reagents provides a simple method for the preparation of XeF⁺Sb₂F^?₁₁.     

New class of coordination compounds with noble gas fluorides as ligands to metal ions

A new class of coordination compounds of the type [Mⁿ⁺(L)_p](AF₆⁻)_n and [Mⁿ⁺(L)_r](BF₄⁻)_n, where M is Mg, Ca, Sr, Ba, Cd, Pb, lanthanides, A is P, As, Sb, Bi and L is XeF₂, XeF₄, XeF₆, KrF₂, was studied. A review of all known coordination compounds with L is XeF₂ is given: (a) synthetic routes for the preparation of these compounds; (b) analysis of their crystal structures (molecular, dimer, chain, double chain, layer, strongly interconnected double layers and three-dimensional network); (c) the influence of the ligand XeF₂ (small formula volume, linear, semi-ionic, charge of −0.5e on each F ligand); (d) the influence of the central metal ion; (e) the influence of the anions: AF₆⁻ and BF₄⁻ (the formula volume, Lewis basicity). On the basis of all properties of the metal ions, ligand and anions the obtained variety of the structures is analyzed.     

VUV spectra of the xenon fluorides

The absorption spectra of gaseous XeF₂, XeF₄, and XeF₆ have been accurately measured in the photon energy range from 6 to 35 eV with the use of the synchrotron radiation of DESY. The vibrational structure of several Rydberg transitions could be resolved. The spectra are interpreted and most of the structures could be assigned. From these data, information about the ionized species is obtained. The assignment of the first two IP's of XeF₄ is corrected.     

DVM-Xα calculations on the electronic structure of the xenon fluorides XeFn : n = 2, 4, 6

The ionization potentials of the XeF₂, XeF₄ and XeF₆ molecules are calculated by the discrete variational Xα-method. The results of the calculations are used for an interpretation of the experitnental PES and XPS of these compounds. Reasonable agreement is found between the theoretical estimates and data obtained from absorption spectroscopy.     

Zur Hochdruckpolymorphie der Dihalogenide MX2 (M: Ca,Sr, Eu; X: F,Cl, Br)

High Pressure Polymorphy of Dihalides MX₂ (M: Ca, Sr, Eu; X: F, Cl, Br) High pressure investigations of alkaline and rare earth dihalides yielded new polymorphs of CaBr₂, SrCl₂, SrBr₂ und EuBr₂, which could be quenched and characterized by x-ray methods. The polymorphic transitions can be understood as single steps in a sequence of structures given by the coordination numbers. We discuss the thermodynamic stability of the high pressure phases in terms of the Madelung part of lattice energy of all polymorphic forms of these compounds.     

Edelgasverbindungen mit dem Liganden –OTeF5

Noble Gas Compounds Containing the Ligand —OTeF₅ Xe(OTeF₅)₄, Xe(OTeF₅)₆, O?Xe(OTeF₅)₄ as well as mixed substituted derivatives O?XeF_x(OTeF₅)_4?x are described and discussed in context with the known compounds Xe(OTeF₅)₂, and Xe(OSeF₅)₂. The ligand —OTeF₅ is the best stabilizer for noble gas compounds, exceeded only by fluorine itself. Whereas the structures of Xe(OTeF₅)₄ and O?Xe(OTeF₅)₄ are analogous to XeF₄ and XeOF₄, Xe(OTeF₅)₆ is found to be structurally comparable to monomeric (gaseous) XeF₆. Attempts to isolate krypton compounds of the same type were not successful.     

First-principles investigation of the ternary scandium based inverse-perovskite carbides Sc3AC (A = Al,Ga, In and Tl)

Based on first-principles approach, we present a comparative study of structural, electronic, elastic and thermo-dynamical properties of the series of inverse-perovskites Sc₃AC, with A = Al, Ga, In and Tl. The calculated equilibrium lattice constants are in excellent agreement with the experimental and available theoretical data. The electronic band structures and densities of states profiles show that the studied compounds are conductors. Analysis of atomic site projected local density of states and charge densities reveals that a mixture of covalent–ionic–metallic characterizes the chemical bonding of the considered inverse-perovskites. Pressure dependence up to 40 GPa of the single-crystal and polycrystalline elastic constants has been investigated in details. The computed B/G ratios show that all Sc₃AC compounds are brittle. We have estimated the sound velocities in the principal directions. Through the quasi-harmonic Debye model, in which the phononic effects are taken into account, the temperature and pressure effects on the lattice constant, bulk modulus, heat capacity and Debye temperature are performed.     

The enthalpies of formation of XeF6(c), XeF4(c), XeF2(c), and PF3(g)

The energies of reaction of XeF₆(c), XeF₄(c), and XeF₂(c) with PF₃(g) were measured in a bomb calorimeter. These results were combined with the enthalpy of fluorination of PF₃(g), which was redetermined to be −(151.98 ± 0.07) kcal_th mol⁻¹, to derive (at 298.15 K) ΔH_f^o(XeF₆, c, I) = −(80.82 ± 0.53) kcal_th mol⁻¹, ΔH_f^o(XeF₄, c) = −(63.84 ± 0.21) kcal_th mol⁻¹, and ΔH_f^o(XeF₂, c) = −(38.90 ± 0.21) kcal_th mol⁻¹. The enthalpies of formation of the solid xenon fluorides were combined with reported enthalpies of sublimation to derive (at 298.15 K) ΔH_f^o(XeF₆, g) = −(66.69 ± 0.61) kcal_th mol⁻¹, ΔH_f^o(XeF₄, g) = −(49.28 ± 0.22) kcal_th mol⁻¹, and ΔH_f^o(XeF₂, g) = −(25.58 ± 0.21) kcal_th mol⁻¹. The average bond dissociation enthalpies,〈D^o〉(XeF, 298.15 K), are (29.94 ± 0.16), (31.15 ± 0.13), and (31.62 ± 0.16) kcal_th mol⁻¹ in XeF₆(g), XeF₄(g), and XeF₂(g), respectively. The enthalpy of formation of PF₃(g) was determined to be −(228.8 ± 0.3) kcal_th mol⁻¹.     

The “Base-catalysed” fluorination of SO2 by XeF2

The fluorination of SO₂ by XeF₂ in the presence of compounds of the type MX (M = NMe₄, Cs, K; X = F, Cl) is described.Reaction mechanisms are proposed in which the XeF₂ functions as a weak Lewis acid.     

Vibrational spectra and structural features of noble gas fluorides in cryogenic and nonaqueous solutions

Data on the vibrational spectra of noble gas fluorides in the gas phase and in cryogenic and nonaqueous solutions are considered in detail. Based on analysis of the IR spectra of xenon fluorides dissolved in liquid Kr and Xe, it is concluded that the XeF₆ molecule possesses the geometry of a distorted octahedron withC _3v symmetry. The contours of spectral lines of totally symmetric stretching modes in the Raman spectra of noble gas fluorides in nonaqueous solutions are considered; the mechanisms of formation contours of these lines, the dynamic parameters of XeF _n (n=2, 4, 6) and KrF₂, and the characteristic times of intramolecular rearrangements in the nonrigid XeF₆ molecule are analyzed. It is concluded that in the XeF₂-HF and XeF₆-HF systems, a number of associates and ionic clusters are formed due to the donor-acceptor interaction of the Lewis bases and acids. Translated fromIzvestiya Akademii Nauk. Seriya Khimicheskaya, No. 4, pp. 560–582, April, 1998.     

Electronic,elastic and thermal properties of lutetium intermetallic compounds

The electronic, structural, elastic, thermal and mechanical properties of Lutetium intermetallic compounds LuX (X = Mg, Cu, Ag, Au, Zn, Cd and Hg) have been studied using ab-initio full potential linear augmented plane wave (FP-LAPW) with the generalized gradient approximation (GGA) in their non magnetic phase. The ground state properties such as lattice constant, bulk modulus, pressure derivatives of bulk modulus are reported in CsCl-(B₂ phase) structure. We also report the band structure and density of states at equilibrium lattice constant. The calculated band structures indicate that these intermetallics are metallic in nature. The second order elastic constants of these compounds are also predicted for the first time. The ductility of these compounds is determined by calculating the bulk to shear ratio B/G_H.     

Solid Ionic Conductors: Principles and Applications

Solid ionic conductors, also called solid electrolytes, transport electric current by means of ions. The best known examples of these usually crystalline compounds include doped ZrO₂, as well as AgI, β-Al₂O₃, and CaF₂. Ionic conduction in solid electrolytes reaches its maximum value if a partial lattice of a solid compound undergoes transition at elevated temperature to a quasimolten state. The ionic conductivity in such solid compounds is then as high as in molten salts. Solid electrolytes have found many scientific and technological applications; thus, they can be used to study thermodynamic and kinetic problems, and to build fuel cells, batteries, sensors, and chemotronic components.     

Syntheses and Structures of F6XeNCCH3 and F6Xe(NCCH3)2

Acetonitrile and the potent oxidative fluorinating agent XeF₆ react at ?40 °C in Freon‐114 to form the highly energetic, shock‐sensitive compounds F₆XeNCCH₃ ( 1 ) and F₆Xe(NCCH₃)₂?CH₃CN ( 2 ?CH₃CN). Their low‐temperature single‐crystal X‐ray structures show that the adducted XeF₆ molecules of these compounds are the most isolated XeF₆ moieties thus far encountered in the solid state and also provide the first examples of Xe^VI? N bonds. The geometry of the XeF₆ moiety in 1 is nearly identical to the calculated distorted octahedral (C_3v) geometry of gas‐phase XeF₆. The C_2v geometry of the XeF₆ moiety in 2 resembles the transition state proposed to account for the fluxionality of gas‐phase XeF₆. The energy‐minimized gas‐phase geometries and vibrational frequencies were calculated for 1 and 2 , and their respective binding energies with CH₃CN were determined. The Raman spectra of 1 and 2 ?CH₃CN were assigned by comparison with their calculated vibrational frequencies and intensities.     

Tutorial review: Bohr circular orbit diagrams for some fluorine-containing molecules

Examples are provided of Bohr circular orbit diagrams to represent the electronic structures of some fluorine-containing molecules. The orbit diagrams are constructed from a 2n × n factorisation of the atomic shell-structure formula 2n², with n = 1, 2, 3, … Particular attention is given to orbit diagrams and the associated valence bond structures for the hypercoordinate molecules and ions PF₅ and NF₅, F₃⁻ and XeF₂, IF₅ and XeF₅⁺, XeF₅⁻, IF₈⁻, XeF₈²⁻, ReF₈⁻ and TaF₈³⁻, ZrF₈⁴⁻, ZrF₇³⁻, Re₂F₈²⁻, and high-spin CoF₆³⁻.Aspects of the electronic structures of D_3h-symmetry PF₅ and NF₅ are contrasted via the use of orbital valence bond considerations, and the results of STO-3G valence bond calculations are reported for these species.