Pre-resonance Raman effect and vibronic coupling of benzene and benzene-d6

The pre-resonance Raman effect was observed for liquid benzene and benzene-d₆. Great intensity enhancement was found for ν₁₀(e_1g), 2ν₈ and 2ν₁₄. The effect was expained in terms of vibronic couplings between the electronic states of the molecules.     

Synthesis and structure of the silylated benzene radical anion salts [K([18]crown-6){C6H4(SiMe3)2-1,4}] and [K([18]crown-6)(THF)2][C6H2(SiMe3)4-1,2,4,5]

The crystalline compound [K([18]crown-6){C₆H₄(SiMe₃)₂-1,4}] (1) was prepared by the low-temperature reduction of the para-disilylated benzene with K/[18]crown-6 in toluene followed by recrystallisation from the same solvent. Reduction of 1,2,4,5-tetrasilylated benzene with 2(K/[18]crown-6) in toluene produced a hydrocarbon-insoluble powder identified as the dianionic derivative [K([18]crown-6)]₂[C₆H₂(SiMe₃)₄-1,2,4,5)] (2), which upon crystallisation from THF/Et₂O yielded [K([18]crown-6)(THF)₂][C₆H₂(SiMe₃)₄-1,2,4,5] (3). An X-ray diffraction study revealed that 1 comprised a contact ion pair with the crown-encapsulated K cation η⁵-connected to the planar ring of the substituted benzene radical anion, while 3 contained a well separated cation and anion.     

Simulation of vibrational spectra of isotopic benzenes by an extended molecular mechanics method

Vibrational spectra of benzene and benzene-d₆ in the gas and liquid phase have been simulated by a molecular mechanics method including the calculation of equilibrium structures, thermodynamic quantities, normal frequencies and vibrational transition probabilities. The potential parameters have been estimated by referring to the observed frequencies of benzene, benzene-d₆ and 1,3,5-benzene-d₃ and also to results of ab initio calculations. Four and ten independent parameters are required, respectively, for elucidating the infrared absorption and Raman intensities of these compounds in the gas and liquid phase. The infrared absorption spectrum of benzene-d₁ is reproduced well by using the potential and the intensity parameters estimated for benzene and benzene-d₆. The change of relative band intensities on the phase change has been elucidated in terms of the change of various intensity parameters.     

Photochemical studies on η5-cyclopentadienyl(triphenylphosphine)nickelalkyl and -aryl compounds

Photo-induced degradation studies of a series of organonickel complexes of the type (η⁵-C₅H₅)(PPh₃)Ni(R) (R = CH₃, C₂H₅, C₆H₅ and C₆H₄CH₃-p) as well as certain deuterated analogs have been undertaken. Photolysis of the methyl compounds in benzene as well as benzene-d₆ gives methane as the major gaseous product, the photogenerated methyl group abstracting hydrogen from either the cyclopentadienyl ring, from the solvent, or from another methyl group. The photo-induced dealkylation of the ethyl compound gives both ethylene and ethane, and is explained by β-hydride elimination followed by subsequent reaction of the hydrido intermediate with additional ethyl compound. The photolysis of the phenyl and p-tolyl complexes in benzene solution leads to biaryl formation, both from the coupling of two coordinated aryl groups as well as interactions with the solvent. Triphenylphosphine is a product in all of these photo-decomposition studies.     

Determination of rotational diffusion constants of liquid benzene from measurements of infrared and raman line widths

Line widths are measured for the Raman v₁, v₁₅ and infrared v₁₂ of C₆ll₆ in C₆D₆ solution. Rotational diffusion constants are determined from the observed line widths, and compared with literature values. A rather anisotropic rotation of benzene molecules is suggested.     

Pd(OAc)2-catalyzed cross-coupling of polyfluoroarenes with simple aromatics in imidazolium ionic liquids (ILs) without oxidant and additive and with recycling/reuse of the IL

Polyfluoroarenes can be cross-coupled with simple aromatics (benzene, toluene, and anisole), in good isolated yields, by using Pd(OAc)₂ dissolved in imidazolium ILs [(bmim)PF₆ and (bmim)BF₄] as solvent, without the need for an oxidant and an additive. The reaction is catalyzed by HOAc and it is subject to a primary isotope effect (K_H/K_D = 4.87). Competitive cross-coupling reactions of 1,2,4,5-tetrafluorobenzene with benzene/toluene, benzene/anisole, and anisole/toluene gave K_B/K_T = 5.1, K_B/K_A = 5.7, and K_A/K_T = 5.0, respectively, indicative of a remote substituent effect on Pd insertion into the phenyl C-H bond. Mild reaction conditions, simple product isolation and recycling/reuse of the IL are additional advantages of this method.     

The interaction of aromatic hydrocarbons with organometallic compounds of the main group elements : III. The crystal structure of K[Al2(CH3)6F]·C6H6

The crystal structure of K[Al₂(CH₃)₆F]·C₆H₆ has been determined from three-dimensional X-ray data measured by counter methods. The compound crystallizes in the orthorhombic space group Pnma with cell dimensions a = 14.071(5), b = 14.404(5), c = 8.862(3) Å and ρ_calc = 1.04 g·cm^-3 for Z = 4. Least squares refinement gave a conventional weighted R factor of 0.037 for 973 independent observed reflections. In the fluorine-bridged anion, the aluminum—fluorine—aluminum bond angle is fixed at 180° by crystallographic symmetry. The aluminum—fluorine bond length of 1.782(2) Å is compared to other halogen-bridged systems. The potassium ion coordination sphere contains six methyl groups at distances from 3.23 to 3.47 Å; the benzene functions as a molecule of crystallization with 3.947(7) Å as the shortest benzene carbon—potassium ion approach.     

Benzene clusters in a supersonic beam

A supersonic beam is employed to produce benzene clusters (C₆H₆) _n up ton=40. Mass analysis is achieved after two-photon ionization in a reflectron mass spectrometer. Photon energy is chosen so that the internal energy of the cluster ions is less than 700 meV and a slow decay on the µs time scale is observed. By an energy analysis with the reflecting field it is found that the elimination of one neutral benzene monomer is the favoured dissociation process of the cluster ions. Information about the dissociation pathways of the cluster ions is essential if one is to obtain neutral cluster abundances from the ion mass spectrum. Furthermore an experimental method is presented to obtain pure intermediate state (S ₁←S₀) spectra of selected clusters without interferences from the other clusters present in the molecular beam. This method is based on the observation of the metastable decay of the corresponding cluster ion. When the metastable signal is recorded as a function of photon energy it reflects theS ₁←S ₀ intermediate state spectrum. Spectra are presented for the benzene dimer, trimer, tetramer and pentamer.     

New N-heterocyclic carbene mercury(II) complexes: Close mercury-arene interaction

Mononuclear mercury complexes (1, 2, and 3) bearing bis-N-heterocyclic carbene (NHC) ligands of the form [(NHC)₂-μ-Hg]⁺² have been prepared and structurally characterised. The complexes were derived from three bis-imidazolium salts as precursors to NHC; either 1,3-bis(N-methylimidazolium-1-ylmethyl)benzene bis(hexafluorophosphate) (I·2PF₆), 1,3-bis(N-butylimidazolium-1-ylmethyl)benzene bis(hexafluorophosphate) (II·2PF₆) or 3,5-bis(N-butylimidazolium-1-ylmethyl)toluene bis(hexafluorophosphate) (III·2PF₆) treated with mercury(II) acetate. Interestingly X-ray crystal structure analysis revealed a close interaction between the Hg metal centre with one carbon atom of the aryl linker in addition to coordination with two NHCs.     

Isolierung und struktur des dreikernigen hexamethylbenzolzirkonium-komplexes [(Me6C6)3Zr3Cl6]2+ [(Al2Cl7)−]2

Crystals of the trinuclear complex [(Me₆C₆)₃Zr₃Cl₆][Al₂Cl₇]₂ have been obtained from the reaction of ZrCl₄, hexamethylbenzene, AlCl₃, and Al in benzene. They are monoclinic, space group C2/2, with Z  4 and lattice parameters a 14.167(3), b 27.779(7), c 15.721(3) Å and β 94.27(4)°. The Zr atoms form a regular triangle. Each pair of Zr atoms is bridged by two Cl atoms. The fifth coordination site of each Zr atom is occupied by a h⁶-Me₆C₆ group. The cation is almost isostructural with the known trinuclear cation [(Me₆C₆)₃Nb₃Cl₆]²⁺. Important distances are: ZrZr 3.35, ZrCl 2.56, and Zrcenter of C₆ ring 2.17 Å. One of the two independent [Al₂Cl₇]^? anions occurs in a staggered conformation and one occurs in an eclipsed conformation.     

The crystal structure of bis(N-pentafluorophenyl)tetraphenyl-cyclodisilazane-tetrabenzene, (Ph2SiNC6F5)2 · 4C6H6

The disilazane (Ph₂SiNC₆F₅)₂ crystallises from benzene solution with four molecules of solvent in the orthorhombic space group Pnna with a 18.182(6), b 21.480(8) and c 13.631(5) Å, Z = 4. The structure was solved by direct methods and refined by least-squares to R 0.069 for 937 observed reflections. The Si₂N₂ ring is planar with NSiN and SiNSi angles of 85.2 and 95.5° respectively; the mean SiN distance is 1.755 Å. The C₆F₅ groups are twisted by ca. 16° from the Si₂N₂ plane and the benzene molecules are arranged face-on above and below each of the C₆F₅ groups. There are, in addition, short intermolecular contacts between four fluorines of each C₆F₅ group and hydrogen atoms from both solvate benzene and the phenyl groups of a symmetry related silazane. Attempts to refine the related (Me₂SiNC₆F₅)₂ structure were not successful, probably due to disorder.     

Naphthalene complexes: V. Arene exchange reactions in naphthalenechromium complexes

Di-η⁶-naphthalenechromium(0) (1) reacts at 150°C with benzene to yield (η⁶-naphthalene)(η⁶-benzene)chromium(0) (3) in 76% yield. In the presence of THF, 1 undergoes Lewis base catalyzed arene exchange at 80°C. Reactions of 1 with substituted arenes yield the mixed sandwich complexes 4 and 6–10 (arene = 1,4-C₆H₄Me₂, 1,3,5-C₆H₃Me₃, C₆Me₆, 1,4-C₆H₄(OMe)₂, 1,4-C₆H₄F₂ and 1,4-C₁₀H₆Me₂). In all but one case (with 1,4-dimethylnaphthalene) exchange of a single naphthalene ligand is observed. In marked contrast to the lability of 1, dimesitylenechromium(0) (5) is inert to arene displacement in benzene up to 240°C. The molecular structure of 3 has been determined by X-ray crystallography. The crystal data are as follows: a 7.784(1), b 13.411(2), c 22.772(5) Å, Z = 8, space group Pbca. The structure was refined to a R_w value of 0.043. The naphthalene ligand in 3 is nearly planar and parallel to the approximately eclipsed benzene ring. Metal atom-ring distances are 1.631(9) and 1.611(4) Å for naphthalene and benzene, respectively. Catalyzed and uncatalyzed naphthalene exchanges in the sandwich complex are compared to the analogous reactions with the Cr(CO)₃ complex 2. Naphthalene exchange in 2 in benzene is 10³ to 10⁴ times faster than arene exchange in other arenetricarbonylchromium compounds. The mild conditions for Lewis base catalyzed naphthalene exchange make 2 a good precursor of other arenetricarbonylchromium compounds. Examples include the Cr(CO)₃ complexes of styrene, benzocyclobutene, 1-ethoxybenzocyclobutene, 1,8-dimethoxy-9,10-dihydroanthracene and 1,4-dimethylnaphthalene.     

A CNDO/S study of the importance of electron repulsion parameters and charge density changes on the weakness of the v8(e2g) vibronic activity in the benzene 260 nm band

We investigate the disparity between the large observed ratio ( ≈100:1 ) of v₆ to v₈ vibrationally induced intensity in the 260 nm ( ¹B_2u–¹A_1g) absorption band of benzene and that computed from CNDO/S and INDO/S (typically 4:1). The calculated v₈ intensity is relatively insensitive to small admixtures of the v₆ mode, but is found to be quite sensitive to the nature of the semiempirical electron repulsion integral (γ) distance dependence. A new perturbation theory is applied successfully which relates the vibronic coupling directly to changes in the Fock matrix and the simple first-order transition density.     

Preparation and photochemical properties of polymethacrylic esters of para-acylated 2-phenoxyethanols

For studying the photochemistry of carbonyl chromophores in the side-chain, methacrylic esters of para-acylated 2-phenoxyethanols (CH₂ = C(CH₃) · CO · O · CH₂ · CH₂O · C₆H₄ · CO · R), soluble copolymers with styrene and soluble homopolymers were prepared. Comparison of low temperature emission spectra of model compounds, homopolymers and copolymers doped in polystyrene film indicated some interaction between the excited and the ground state structural units in homopolymers. Quantum yield of main chain scission of copolymers of styrene with monomers 1–3 (R = CH₃, C₂H₅, C₆H₅) at 313 nm radiation in benzene were about 10^?4; the cross-linking was the main reaction for copolymer styrene/monomer 4 (R = C₆H₅CH₂). On exposure of copolymers styrene/monomers 1–4 and polystyrene doped with model compounds in film to 313 nm radiation in air, accelerated photo-oxidation occurs as well as cross-linking. Only chromophores of monomers 3 and 4 were effective as sensitizers of photochemical addition of maleic anhydride to benzene by radiation with γ > 340 nm. The difference in the efficiency between model compounds and copolymers on the one hand and a homopolymer on the other hand is due to self-quenching.     

A tert-butyl/cyano substituted (1,2,3,5-dithiadiazolyl)benzene and η π complexes with CpCr(CO)2

A rational synthesis for 5-tert-butyl-3-cyano-1-(1,2,3,5-dithiadiazolyl)benzene, which was first observed from thermal cleavage of the bis-dithiadiazolyl, has been developed. Voltammetry and electron paramagnetic resonance (EPR) spectra for this radical are reported and its X-ray structure is described. Despite the bulky ^tBu substituent, the cyano supramolecular synthon is still able to maintain links to a single neighbouring sulfur atom of the S₂ unit, as previously observed in cyano-substituted dithiadiazolyls. In the η² complex with CpCr(CO)₂, no such interactions are observed; the nitrile group forms a centrosymmetric dimer through weak contacts with the para H atom on the aryl ring of the partner molecule. This behaviour is contrasted to similar complexes of less bulky dithiadiazolyls, where intermolecular interactions are retained in the crystalline lattice.     

Unperturbed dimensions of poly-p-chlorostyrene

Viscosity measurements on poly-p-chlorostyrene (PPCS) in benzene-methanol mixtures have been carried out at their corresponding theta temperatures determined by the phase separation method. Viscosity measurements were also run in benzene at the same temperatures. The Stockmayer-Fixman extrapolation method was applied to the data to obtain the chain unperturbed dimensions. K_θ. It was found that these, for PPCS in benzene, decrease with increasing temperature and that, both in benzene and in binary mixtures, they decrease with increasing values of the parameter a from the relationship [η] = KM^α. PPCS theta temperature in benzene was 8.     

Reactions of bis(tetrazole)phenylenes. Surprising formation of vinyl compounds from alkyl halides

The reactions of 1,2-bis(tetrazol-5-yl)benzene (1), 1,3-bis(tetrazol-5-yl)benzene (2), 1,4-bis(tetrazol-5-yl)benzene (3), 1,2-(Bu₃SnN₄C)₂C₆H₄ (4), 1,3-(Bu₃SnN₄C)₂C₆H₄ (5) and 1,4-(Bu₃SnN₄C)₂C₆H₄ (6) with 1,2-dibromoethane were carried out by two different methods in order to synthesise pendant alkyl halide derivatives of the parent bis-tetrazoles. This lead to the formation of several alkyl halide derivatives, substituted at either N1 or N2 on the tetrazole ring, as well as the surprising formation of several vinyl derivatives. The crystal structures of both 1,2-[(2-vinyl)tetrazol-5-yl)]benzene (1-N,2-N′) (1b) and 1,3-bis[(2-bromoethyl)tetrazol-5-yl]benzene (2-N,2-N′) (5d) are discussed.     

Arenetitatnium(II) complexes of formula Ar-TiCl2-Al2Cl6

The synthesis and properties of Ar-TiCl₂-Al₂Cl₆(Ar=benzene or a methylbenzene) complexes have been studied, and the results indicate an increase in stability of the arenetitanium π-bond in the order: benzene < toluene < xylenes < mesitylene < durene < hexamethylbenzene.An exchange reaction of the aromatic ligands was observed. On the basis of conductivity measurements it was ascertained that the complexes are partialy ionize in solution.     

Studies on bis(1′-ortho-carboranyl)benzenes and bis(1′-ortho-carboranyl)biphenyls

Reactions between the C,C′-dicopper(I) derivative of ortho-carborane and ortho-, meta- and para-diiodobenzene are reported. The reaction with 1,2-C₆H₄I₂ unexpectedly afforded 2,2′-bis(1′-ortho-carboranyl)biphenyl, [HCB₁₀H₁₀CC₆H₄]₂2, whereas reactions with 1,3- or 1,4-C₆H₄I₂ provided alternative routes to 1,3-bis(1′-ortho-carboranyl)benzene 3 and 1,4-bis(1′-ortho-carboranyl)benzene 4, respectively. The crystal structure of the biphenyl derivative 2 revealed significant distortions in the biphenylene framework attributable to the proximity of the two bulky carborane cages. UV absorption spectra and electrochemical data on 2 and 3 showed little electronic communication between the two carborane cages in either, and negligible π-conjugation between the two ortho-phenylene rings in 2. However, substantial evidence was found of electronic communication between the carborane cages via the para-phenylene bridge in 4. B3LYP/6-31G^∗ computations have been carried out on compounds 2 and 4, on 4,4′-bis(ortho-carboranyl)biphenyl 6 and on 1,2-bis(1′-ortho-carboranyl)benzene 7. Those on 2, 4 and 6 show the computed geometries to be in very good agreement with the experimental geometries: those on 7 allowed the reported molecular geometry of this compound to be revised and revealed a long cage C–C bond of 1.725(3) Å.     

Enthalphy of mixing of bromobenzene with n-alkanes,with cyclohexane,and with benzene

A dynamic flow microcalorimeter of the Picker design was used to measure enthalpies of mixing at 298.15 K and atmospheric pressure of the six binary systems bromobenzene + n-hexane, + n-heptane, + n-nonane, + n-tetradecane, + cyclohexane, and + benzene. Within the homologous series of n-alkane systems, the interaction parameter, h₁₂, calculated from rigid-lattice group contribution theory, decreases weakly with increasing chain length of the alkane. This behavior is quite analogous to that observed with chloro-derivatives of benzene + n-alkane.