Die Kristallstruktur von (CH3)2GaC5H5

Dimethyl(cyclopentadienyl gallium, (CH₃)₂GaC₅H₅, crystallizes with monoclinic symmetry in space group P2₁/c; the cell dimensions are a = 6.587(3), b = 9.154(3), c = 12.756(5) Å and β = 113.20(3)^o with Z = 4. The structure was solved using heavy atom techniques and refined by least-squares techniques to give a value of R = 0.046 for the 1719 observed reflections. The structure consists of chains of dimethylgallium-groups bridged by cyclopentadienyl rings along the b-axis. Each gallium atom has a distorted tetrahedral environment with Ga-methyl distances of 1.965 Å and Ga-Cp distances of 2.215 and 2.314 Å, respectively.     

The crystal and molecular structure of Rh2(CH3CO2)4[HCON(CH3)]2—effect of ligands on metalmetal bonding

The structure of Rh₂(CH₃CO₂)₄(DMF)₂ {DMF = HCON(CH₃)₂} has been determined by single crystal X-ray methods. The compound crystallizes with eight formula units in a cell of dimensions: a = 29.438(7) Å, b = 7.978(2) Å, c = 20.279(5) Å, β = 113.20(4)°, V = 4377.5 ų, space group C2/c. The structure has been refined by full-matrix least-squares method to a final R = 0.030 for the 4156 observed data. Two Rh(II) atoms are linked by four acetate groups forming a dimeric unit, where the RhRh distance is 2.383(1) Å. The coordination sphere about each Rh atom is completed by a DMF molecule; the average RhO(DMF) distance is 2.296(3) Å.     

Synthesis of 1,1′-di-t-butylstannocene and its reaction with trifluoroborane. The crystal and molecular structure of η5-(CH3)3CC5H4Sn+BF4−

The reaction of Li(CH₃)₃CC₅H₄ with SnCl₂ in THF affords 1,1′-di-t-butylstannocene in 78% yield as an air-sensitive oil. ¹H and ¹³C NMR spectra are consistent with a pentahapto-structure. Mössbauer parameters of the stannocene and its trimethylsilyl counterpart match closely those of known stannocenes and neither compound appears to undergo oligomerization. The reaction of 1,1′-di-t-butylstannocene with BF₃ in CH₂Cl₂ affords η⁵-(CH₃)₃CC₅H₄Sn⁺ BF₄^? and other uncharacterized product(s) thought to involve tetracoordinate tin. The structure of η⁵-(CH₃)₃CC₅H₄Sn⁺ BF₄^? was determined by single crystal X-ray diffraction (orthorhombic,Pbcn, (T 25°C), a 18.423(3), b 11.723(1), c 11.044(2) Å, Z Å, m.p. 95–96°C, colorless, Mo-K_α, R = 0.043).     

X-ray crystal analysis of tricyclohexyltin trifluoroacetate and Mössbauer data for (cyclo-C6H11)3SnO2CR′ (R′ = CH3, CH2CL,CHCL2, CCl3 and CF3)

The halogenocarboxylates (cyclo-C₆H₁₁)₃SnO₂CR′, (R′ = CH₃, CH₂Cl, CHCl₂, CCl₃ and CF₃) have been prepared, and characterized by Mössbauer and IR spectroscopy. The crystal structure of (cyclo-C₆H₁₁)₃SnO₂CCF₃ has been determined by X-ray analysis. The crystals are orthorhombic, space group Pcmn, with unit cell parameters a 14.390 ± 0.004, b, 13.427 ± 0.004, c 11.516 ± 0.003 Å. The structure was resolved by Patterson methods and refined to an R value of 0.147. The coordination about the tin atom can be considered distorted trigonal-pyramidal or distorted tetrahedral. Mössbauer data are explained in terms of distortions of bond angles about the tin atom.     

On the molecular structure of (CH3)2NSO2N(CH3)2 as studied by gas electron diffraction

The following bond lengths and bond angles have been deduced from a vapour phase electron diffraction study of (CH₃)₂NSO₂N(CH₃)₂: r(C-H) 1.114 ± 0.005 Å, r(S-O) 1.432 ± 0.010 Å, r(N-C) 1.475 ± 0.013 Å, r(S-N) 1.651 ± 0.003 Å, ∠N-C-H 109.3 ± 2.0°, ∠C-N-C 118.0 ± 302°, ∠S-N-C 115.2 ± 1.1°, ∠N-S-N 110.5±1.3° and ∠O-S-O 114.7±2.5°. The sulphur bond configuration and the prevailing conformation, which was identical to that in the crystal, are discussed in relation to analogous sulphide and sulphoxide derivatives.     

Valence electronic structure of CH3Br and CH3I: Electron momentum distributions and separation energies

Bromomethane (CH₃Br) and iodomethane (CH₃I) have been studied by binary (e,2e) coincidence spectroscopy at 1200 eV using non-coplanar symmetric kinematics. Separation energy spectra have been determined in the energy range up to 47 eV at azimuthal angles of 0° and 8° for CH₃Br and 0° and 6° for CH₃I. The separation energy spectra and the electron momentum distributions measured for each of the valence orbitals are compared with theoretical predictions employing SCF wavefunctions and outer valence type and extended 2 ph-TDA Green function calculations. Electron density and momentum density maps have been calculated for all the valence orbitals using the SCF wavefunctions, and they are used to explain trends and contrasts in the electronic structure and bonding properties of these halomethanes in both position and momentum space.     

Actinide-centered cyclometalation chemistry. An unusually distorted thorium bishydrocarbyl: Thp[η5-(CH3)5C5]2CH2Si(CH3)3]2

The crystal and molecular structure of the complex Th[η⁵-(CH₃)₅C₅]₂[CH₂-Si(CH₃)₃]₂, which undergoes facile intramolecular cyclometalation to the thoracyclobutane Th[η⁵-(CH₃)₅C₅]₂(CH₂)₂Si(CH₃)₂, is reported. While the Th[η⁵-(CH₃)₅C₅]₂ ligation is unexceptional, the Th[CH₂Si(CH₃)₃]₂ fragment is highly unsymmetrical having Th-C (corresponding angle Th-C-Si) 2.51(1) Å (132.0(6)°) and 2.46(1) Å (148.0(7)°). This conformation, which appears to result from severe intramolecular non-bonded contacts, allows a methyl hydrogen atom of one CH₂Si(CH₃)₃ ligand to approach within ca. 2.3 Å of the α-carbon atom of the other CH₂Si(CH₃)₃ ligand.     

Synthesis and crystal structure of (ThCu3)(Mn3+2Mn4+2)O12, a new ferrimagnetic perovskite-like compound

Single crystals of [ThCu₃](Mn³⁺₂Mn⁴⁺₂]O₁₂, a ferrimagnetic perovskite-like compound, have been synthesized by hydrothermal conditions at 600°C and 2 kbar. They have been found to be cubic, of space group Im3, with a = 7.359 Å, and isostructural with [NaMn₃](Mn³⁺₂Mn⁴⁺₂)O₁₂. The crystal structure has been refined by single-crystal X-ray diffraction data. The Th⁴⁺ cations are surrounded by slightly distorted icosahedra; the ThO distance is 2.556 Å. The Cu²⁺ cations are also surrounded by 12 oxygens, which are arranged as three mutually perpendicular rectangles of different size, the smallest and the largest of which are almost squares. The three sets of CuO distances are 1.973, 2.800, and 3.238 Å. The octahedral MnO distance is 1.950 Å. A test based on neutron diffraction powder data indicated that the square sites are occupied by only the Cu²⁺ cations.     

Microwave spectrum and substitutional structure of CH2DF

Forty-two transitions of the microwave spectrum of CH₂DF have been observed in the region between 75 and 450 GHz. The measurement of both a-type and b-type transitions makes possible the analysis of the spectrum and the accurate calculation of the rotational constants (in MHz): = 119 675.0535 ± 0.074, = 24 043.4415 ± 0.072, ? = 22959.3732 °0.072, °j = 0.049371 ±0.00011, °_jk = 0.34268 ±0.0006, 2_k = 3,3774 ± 0.0035, δ _j = 0.002329 ± 0.000045, δ_k = 0.0687 ± 0.036. These constants, in combination with the results of earlier work on the symmetric speci r_s structure calculation based entirely on high-accuracy microwave data. The structural parameters are r_CH = 1.100 Å, r_CF = 1.383 Å, and ∠HCH = 110° 37'.     

The crystal structure of N-sodiohexamethyldisilazane,Na[N{Si(CH3)3}2]

The crystal structure of Na[N{Si(CH₃)₃}₂] has been determined from single-crystal x-ray diffraction data collected by counter methods. N-sodiohexamethyldisilazane crystallizes in the mono-clinic space group p21/n with unit cell parameters $\text{a}$ = 9.426(3), $\text{b}$ = 6.921(3), c = 17.974(5)Å, β = 93.83(2)°, and ?_calc = 1.04 g cm^?3 for z = 4 formula units. Least-squares refinement gave a final conventional R value of 0.034 for 1244 independent observed reflections. In the solid state the compound exists in a polymeric arrangement with an average Na-N distance of 2.355(4)Å. The methyl group are configured such that the angle of rotation of the trimethylsilyl moiety about the Si-N bond is 30° from the eclipsed position. The Si-N bond length is 1.690(5)Å, and the Si-N-Si bond angle is 125.6(1)°.     

Structure cristalline de l'hexachlorotellurate(IV) d'hydroxydiméthylsoufrediméthylsulfoxyde (12) [(CH3)2SOH]2(TeCl6)· 2(CH3)2SO

[(CH₃)₂SOH]₂(TeCl₆)·2(CH₃)₂SO crystallizes in the triclinic system, space group P$\text{1}$, with a 9.474(5), b 7.952(4), c 10.180(3) Å, α 109.20(3)°, β 95.75(5)° and γ 117.60(4)°, Z = 1. The structure has been determined by a single-crystal X-ray study and refined by full-matrix least squares analysis to R = 0.044 for 1332 independent reflections. The hydrogen atoms of the methyl groups were not located. The structure contains TeCl₆^2? and (CH₃)₂SOH⁺ ions and (CH₃)₂SO molecules which form layers situated along (011) planes. The TeCl₆^2? ion adopts an almost regular octahedron. The (CH₃)₂SOH⁺ cation and the (CH₃)₂SO molecule are linked by a short hydrogen bond. Interatomic distances are in good agreement with previously published values. Cohesion of the structure is due to ionic interactions, hydrogen bonds and Van der Waals interactions.     

The molecular structure of the complex trimethylaluminium dimethyl ether, (CH3)3AlO(CH3)2, determined by gas phase electron diffraction

The molecular structure of (CH₃)₃AlO(CH₃)₂ has been determined by gas phase electron diffraction. The main molecular parameters are AlC = 1.973(11), AlO = 2.014(14), OC = 1.436(3) Å, OAlC = 98.7(1.5), AlOC = 122.6 (0.5) and COC = 114.5(1.7)°. The OC bond distance and the COC valence angle are significantly larger than those in free dimethyl ether. The three valencies of the oxygen atom appear to lie in one plane. It is suggested that the planarity of the oxygen atom is due to across-angle repulsion Al?C(O).     

On the structures and relative energies of CH3F⨥ isomers

Ab initio calculations have identified two isomers in the CH₃F^? potential energy surface, one corresponding to ionized fluoromethane (CH₃L^? and the other to the methylenefluoronium radical cation (CH₂TH^?. The latter is predicted to lie lower in energy to 46 kJ mol^?1. Examination of rearrangement and fragmentation pathways leads to the conclusion that both ions should be stable, observable species. The importantce of electron correlation in satisfactorily describing the structure of CH₃l^? is demonstrated.     

1,2-Hydrogen abstraction: the characterization of [Li(CH3)2N(CH2)2N(CH3)2]2 [C12H8]. A dilithium complex obtained by the 1,2 deprotonation of acenaphthylene

The reaction of n-butyllithium chelated to N,N,N′,N′-tetramethylethylenediamine (TMEDA) with acenaphthene results in 1,2-hydrogen abstraction to give the dilithio complex of acenaphthylene, [Li(CH₃)₂N(CH₂)₂N(CH₃)₂]₂[C₁₂H₈]. This compound was isolated as a crystalline product and characterized by single crystal X-ray crystallography. [Li(CH₃)₂N(CH₂)₂N(CH₃)₂]₂[C₁₂H₈] crystallizes with a unit cell of a = 23.164(10), b = 25.609(10) and c = 8.495(6) Å in the orthorhombice space group Fdd2. The calculated density is 1.04 g cm^?3 for 8 molecules per unit cell. The observed density is 1.03(4) g cm^?3. 1412 unique reflections were measured on a full circle X-ray diffractometer. The light atom, acentric structure was solved by the symbolic addition technique and refined by full matrix least squares to R₁ = 0.058 and R₂ = 0.056.The acenaphthylene fragment is nearly planar. The effect of charge transfer is evidenced in the short C(3)C(4) bond distance of 1.30(3) Å and the lengthening of the C(1)C(2) bond length from the localized olefinic bond distance of 1.34 to 1.42(2) Å. The two LiTMEDA fragments are coordinated to both sides of the five membered carbon atom ring of the acenaphthylene group.     

The gas-phase molecular structure of CF3HgCH3 - an electron diffraction and microwave study

The molecular structure of CF₃HgCH₃ in the gas phase is determined by a joint analysis of electron diffraction and microwave data. The following geometric parameters (r_av values) are derived: r(Hg—CH₃) = 2.052(5) Å, r(Hg—CF₃) = 2.116(4) Å. r(C-F) = 1.354(2) Å. r(C—H) = 1.079(14) Å, ∠.FCF = 105.7(0.2)° and ∠HCH = 107.0(1.5)°. Error limits are twice the standard deviations.     

Synthesis and crystallographic characterization of a dicyclopentadienylvanadium alkynide complex: (C5H5)2VCCC(CH3)3

(C₅H₅)₂VCl reacts with LiCCC(CH₃)₃ to form (C₅H₅)₂VCCC(CH₃)₃ which was characterized by spectroscopic, analytical, and crystallographic methods. The complex crystallizes from pentane at 0°C as a monomer in the orthorhombic space group Pnma with four molecules in a unit cell of dimensions a 9.075(3), b 9.807(3), c 16.444(5) Å. Full-matrix least-squares refinement based upon 1300 nonzero intensity data converged to a final conventional R factor of 0.060. The molecule has a mean VC₅H₅-ring centroid distance of 1.941 Å with 146.6° ring centroid-V-ring centroid angle. The vanadium alkynide carbon distance is 2.075(5) Å.     

The crystal and molecular structure of triphenylphosphoniodithio-carboxylato-ss'-carbonylbis (trikphenylphosphine) iridium(I) tetrafluoroborate [Ir(S2CPPh3) (CO) (PPh3)2]BF4.

Crystal and molecular structures of the title compound have been determined from a three-dimensional X-ray analysis using diffractometer data. The crystals are monoclinic, space group P2₁/c, with Z = 4 in a unit cell of dimensions a = 10.5876(9), b = 31.518(10), c = 16.2164(5) Å, β = 92.521(1)°. The observed and calculated densities are 1.38 and 1.374 g cm^-1 respectively. The crystals decompose under X-rays, and three crystals were required to complete data collection. The structure was solved and refined by convetional methods to final residuals R and R_w of 0.087 and 0.107 respectively.The crystals contain monomeric cations, and BF₄ anions. The iridium atom is in a distorted trigonal bipyramidal environment consisting of the two sulphur atoms (one axial, one equatorial) of a bidentate triphenylphosphoniodi-thiocarboxylate ligand, two triphenylphosphine groups (equatorial) and the carbonyl ligand (axial). The non-equivalent Ir-s distances are 2.377 and 2.307(5) Å, the Ir-P distances are 2.334, 2.331(5) Å. Within the zwitterion, the C-S distances are 1.66 and 1.70(2) Å, while P-C is 1.78(2) Å. The condensation of PPh₃ and CS₂ to form the PH₃P⁺-CS₂ zwitterion is in contrast to that predicted previously.It is probable that the other complexes of iridium and rhodium prepared in a similar manner [2] should now be reformulated as containing Ph₃P⁺-CS₂^- ligands.     

Structural studies of complexes containing the coordinated methyldisulphido ligand: The crystal structure of [Os (η2-S2CH3) (CO)2 (P (C6H5)3)2] ClO4·12 C6H6.

Crystal and molecular structures of the title compound have been determined from a three-dimentional X-ray analysis usinq diffractometer data. The crystals are triclinic, space group P$\text{1}$, with Z = 2 in a unit cell of dimensions a = 14.23(1), b = 17.30(1), c = 10.44(1) Å, α = 102.1(2), β = 102.7(2), γ = 105.5(2)°. Full matrix least squares refinement has given a final R-factor of 0.060 for 4628 reflections for which I > 3σ(I).The crystal structure consist of discrete cations and anions, together with benzene molecules of crystallisation which are situated about the crystallographic centres of symmetry and serve a purely space-filling role. In the cation coordination about the osmium atom is that of a distorted octahedron, comprising the two triphenylphosphine groups (mutually trans), the two carbonyl groups (mutually cis) and the dihapto S₂Me group. The Os-P distances of 2.420 and 2.419(3) Å are normal. The S₂Me group is nearly symmetrically coordinated with Os-S(l) 2.426(4)Å and Os-S(3) 2.442(4) Å. Other bonds and angles in this ligand are S(1)-S(2) 2.022(7) Å, S(1)-CH₂ 1.81(2) Å, and S(2)-S(1)-CH₃ 105.4(6)°. The observed geometry is similar to that in [Ir(S₂) (Ph₂PCH₂CH₂PPh₂)₂Cl.Ch₃CN.     

Vibrational energy transfer in CH3I

Previous works have reported vibration—vibration and vibration—translation transfer rates in the methyl halides. Using the technique of laser induced infrared fluorescence we have studied energy transfer in the concluding member of this series, CH₃I. Following excitation by resonant lines of a Q-switch CO₂ laser, infrared fluorescence has been observed from the v₂, v₅ as well as the 2v₅, v₁, v₄ vibrational energy levels of CH₃I. All the observed states exhibit a single exponential decay rate of 23 ± 2 ms^?1 torr^?1. Measurements have also been made on deactivation of the various modes by rare gases. The risetime of the v₂, v₅ levels was found to be approximately 101 ± 20 ms^?1 torr^?1, while that of the 2v₅, v₁, v₄ levels was approximately 225 ± 45 ms^?1 torr^?1. Fluorescence was not detected from the v₃ level. These results are discussed in terms of SSH type theoretical calculations, and comparison is made with the results obtained for other members of the methyl halide series, namely CH₃F, CH₃Cl and CH₃Br.     

Photodissociation of CH3Cl+ and CH3Br+ in a tandem quadrupole mass spectrometer

A new tandem quadrupole photodissociation mass spectrometer was used to measure photodissociation cross sections for the reactions, CH₃Cl⁺ → CH₃⁺ + Cl and CH₃Br⁺ → CH₃⁺ + Br in the gas phase using wavelength-selected light. The results on CH₃Cl⁺ are compared with the earlier work of Dunbar. For both reactions we are able to observe photodissociations occurring with small cross sections (≈ 2 × 10^?20 cm²) in the visible region near the thermochemical thresholds.