Die konjugative Wechselwirkung zwischen π- und Walsh-Orbitalen: Das Photoelektron-Spektrum des Homofulvens

Analysis of the photoelectron spectrum of homofulvene ( 1 ) (spiro [2.4] hepta-4,6-diene) confirms the conclusions previously drawn concerning the direct conjugation between π-and Walsh-orbitals. It is shown that the resonance integral (4) appropriate for the semi-quantitative interaction of these orbitals amounts to ?1.9 eV, i.e. nearly the value for conjugating π-orbitals (β = ?2.4 to ?2.5 eV). This explains the close analogy between the photoelectron spectrum of 1 and that of fulvene.     

Photoelectron-spectroscopic Evidence Concerning “Homo-aromaticity”

The first of the two π-bands in the photoelectron spectrum of cis-cis-cis-1, 4, 7-cyclononatriene (I, symmetry C_3v) shows a Jahn-Teller split. This is consistent with the prediction of molecular orbital theory that the top occupied orbitals of I are e (π) and a ₁(π) respectively. From the difference ?( e (π)) - ?( a ₁(π)) = 0.90 to 0.97 eV a value of β_1,3 = ?0.68 eV = 0.27 β (β = -2.5 eV) is obtained for the homoconjugative interaction of two π-orbitals in I. This value represents almost exclusively through-space interaction between the π-orbitals. Through-bond interaction (hyperconjugation) is a minor effect in I. A comparison of the photoelectron data of bicyclo [4.2.1] nonatriene with those of norbornene and cycloheptadiene shows that homoconjugation (homo-aromaticity) can only be detected by photoelectron spectroscopy if the interacting π-bonds (basis orbitals) are symmetry equivalent or have accidentally (almost) degenerate energies.     

The Interaction of π-Orbitals in Barrelene

The photoelectron spectrum (PE. spectrum) of barrelene (bicyclo[2.2.2]octatriene, 4 ) is recorded and the first four bands are correlated with orbitals obtained with the MINDO/2-SCF procedure. The structural changes accompagnying the ionisation process 4 → 4 ⁺ are qualitatively derived from the features of the top-occupied a′₂ (π) MO of 4 , which shows complete σ-π separation. The vibrational pattern of the corresponding PE. band 1. as well as complete energy-minimisation of the geometries of 4 and 4 ⁺ support the conclusion that 4 is a rather strained molecule. The interaction of the three π? bonds in 4 are discussed in terms of ‘through-space’ and ‘through-bond’ interaction with lower lying σ-orbitals. It is found that the latter is far from being negligible.     

The Ionization Potentials of Butadiene,Hexatriene, and their Methyl Derivatives: Evidence for through space interaction between double bond π-orbitals and non-bonded pseudo-π orbitals of methyl groups?

It is shown that the correlation of the π-ionization potentials of ethylene ( 1 ), butadiene ( 2 ) and trans-1,3,5-hexatriene ( 4 ) favours the orbital sequence π, π, σ in butadiene and π, π, σ, π in the hexatriene in excellent agreement with the results of SPINDO calculations. Within the experimental error the π-ionization potentials of cis-1,3,5-hexatriene ( 3 ) and trans-1,3,5-hexatriene ( 4 ) are the same. Methyl-substitution of 2 lowers the π-ionization potentials I₁(π) and I₂(π). For 1 and/or 4 substitution the difference I₂(π)?I₁(π) remains constant (≈ 2.5 eV). On the other hand 2 and/or 3 substitution leads to a smaller gap of I₂(π)–I₁(π) ≈ 1.6 to 2.0 eV without changing the mean π-ionization potential I (π) relative to the corresponding 1,4 substituted derivatives. This result is rationalized in terms of a through space interaction between double bond π-orbitals and non-bonded pseudo-π-orbitals of the substituting methyl groups. The reduced split I₂(π)–I₁(π) in cyclopentadiene is attributed to hyperconjugation across the methylene group.     

Consequences of Substitution in the Photoelectron Spectra of [2, 2]Paracyclophanes: Separation of ‘through-space’ and ‘through-bond’ interactions as a consequence of fluorosubstitution

The PE. spectra of [2, 2]paracyclophane ( 1 ), 4-amino[2, 2]paracyclophane ( 2 ) and 1, 1, 2, 2, 9, 9, 10, 10-octafluoro[2, 2]paracyclophane ( 3 ) are presented. The bands corresponding to ejection of the photoelectron from the five highest occupied π-orbitals have been assigned. The ‘observed’ orbital energies (i.e. the negative ionization potentials) are discussed in terms of ‘through space’ and ‘through-bond’ interactions between the semi-localized π-orbitals ( e_1g ) of the benzene moieties and the C, C-σ-orbitals of the ethylene bridges. The PE. spectrum of 3 shows that the fluorine-induced lowering of the C, C-σ-orbital energy effectively ‘turns-off’ the ‘through-bond’ interaction. The resulting pattern of the first four bands confirms the assignment given for 1 . Finally the band shifts induced by an amino group in position 4 are again in agreement with this assignment. Attention is drawn to the phenomenon of ‘orbital switching’ as a consequence of substitution in loosely coupled systems such as 1 .     

Electronic and Molecular Structure of Simple 3,3′-Bicyclopropenyls. Photoelectron Spectroscopy and Model Calculations

The electronic and molecular structure of 3,3′-bicyclopropenyl ( 1 ) and its alkyl derivatives 3,3′-dirnethyl-3,3′-bicyclopropenyl ( 2 ), dispiro [2.0.2.3]nona-1,5-diene ( 3 ), dispiro[2.0.2.4]deca-1,5-diene ( 4 ), dispiro [2.0.2.5]undeca-1, 5-diene ( 5 ), and dispiro [2.0.2.6]dodeca-1, 5-diene ( 6 ) are studied by means of photoelectron spectroscopy and model calculations. Through-bond' effects in model compound 1 are analyzed in detail, illustrating a general difficulty with NDO models. Low-energy photoelectron bands of 2–6 can be assigned to ejection of electrons from cyclo-propenyl π- and Walsh-orbitals. Strong ‘through-bond’ coupling leads to splitting of the π-bands in the range 1.0–1.5 eV, while the strongly conformation-dependent splitting of the Walsh-bands allows conclusions concerning the preferred torsional angles. The preference of a gauche-conformation is predicted for 2 in the gas phase.     

n→π*-Übergänge in Dicarbonylverbindungen Der Einfluss der n,n- und π*, π*-Wechselwirkung

By CNDO-CI calculations we have found that dicarbonyl compounds exhibit only two n → π* transitions in the visible or near UV. region, instead of four as expected from simpler MO-models. The dominant features of the long-wavelength electronic spectra may be characterized by the relative energy of the two n and the two lowest π* orbitals. In general we distinguish between three cases:

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The π-Orbital Sequence in Norbornadiene and Related Hydrocarbons

A method outlined previously [1] is used to show that in norbornadiene ( 3 ) the b ₂(π) orbital lies above a ₁(π), as predicted by theory. This indicates that in 3 through-space interaction between the two basis π-orbitals π_a and π_b is more important than through-bond interaction. Analysis of the PE.-spectra of 8-isopropylidene-tricyclo[3.2.1.0^2,4]-octane ( 13 ) and the corresponding octene ( 15 ) confirms that the π-orbital π_c of the exocyclic double bond conjugates more strongly with the symmetric Walsh-orbital e _s of the cyclopropano moiety than with the π-orbital π_a of a double bond in the same position.     

Quadricyclanes. Part I: Photoelectron spectra and electronic structure

The photoelectron spectra of quadricyclane ( 3 ) and 3-methylidene quadricyclane ( 4 ) have been measured. The results served as a basis for the elucidation of the electronic structure of these compounds, which agreed with theoretical calculations. It is found that the symmetry of the HOMO of 3 is different when compared to that of its valence isomer norbornadiene ( 1 ). The results also indicate that the structure of the highest occupied orbitals cannot be derived by only considering the Walsh-orbitals of the two three-membered rings. In addition one of the Walsh-components of the four-memebered ring has to be taken into account.     

σ, π-Isomerisierungen von Monohetero-σ-bishomobenzol-Derivaten. Vorläufige Mitteilung

The cis-oxa- ( 13a-d ) and -aza-σ-bishomobenzene ( 13 e ) derivatives have been synthesized; they are sufficiently stable to be isolated in pure form. On heating, 13a-e are easily isomerized into the π-bishomobenzene analogues 14a-e , the processes 13 a ? 14 a , 13 b ? 14b and 13d ? 14d being reversible. Some kinetic and thermodynamic data for these σ, π,bishomobenzene transformations are presented.     

The Electronic Spectrum of Tricyclo[3.3.0.0.2,6]octa-3,7-diene

The unusual electronic spectrum of the title compound is shown to be due to the strong interaction between the π-orbitals of the double bonds and the Walsh-orbitals of the fourmembered ring.     

Die Wechselwirkung zwischen Walsh- und π-Orbitalen im 7-Cyclopropyliden-norbornadien

The qualitative analysis of the PE.-spectrum of 7-cyclopropylidene-norbornadiene ( 3 ) shows that the ‘through-space’ interaction of the e _A-Walsh orbital with the antisymmetric linear combination \documentclass{article}\pagestyle{empty}\begin{document}$ {{\pi _ - = (\pi _a - \pi _b)} \mathord{\left/ {\vphantom {{\pi _ - = (\pi _a - \pi _b)} {\sqrt 2}}} \right. \kern-\nulldelimiterspace} {\sqrt 2}} $\end{document} of the two π-orbitals in 3 is of the same order as the analogous interaction between π- and the π-orbital of the exocyclic double bond in 7-isopropylidene-norbornadiene ( 2 ).     

Triplet states of fluorocarbonyl compounds determined by trapped electron spectroscopy

Ion cyclotron resonance trapped electron spectra for carbonylfluoride, trifluoroacetyl fluoride, hexafluoroacetone, acetyl fluoride and I,I.I-trifluoroacetone are reported. Comparisons of data obtained for ³(π → π^*) vertical excitation energies are used in conjunction with photoelectron spectroscopic data to deduce the effects of fluorine and trifluoromethyl groups on the energies of σ, π and π^* orbitals associated with the carbonyl group.     

Photoelektron-Spektren von Cycloalkenen und Cycloalkadienen. Vorläufige Mitteilung

The photoelectron spectra of cis-cycloalkenes (with three to ten carbon atoms in the ring), of three isomeric, non-conjugated cyclodecadienes, and of cis, cis, -1, 3-cycloalkadienes (with five to eight carbon atoms in the ring) have been recorded. The essential features of their π-bands and of the first σ-bands are briefly discussed.     

The Interaction of Walsh-Orbitols in Diademane and Related Hydrocarbons

To obtain further information concerning the interaction between Walsh-orbitols of ‘conjugated’ cyclopropane rings, the photoelectron spectra of the following compounds have been recorded: bicyclo[4.1.0]heptane 1 , cis- and trans-tricyclo[5.1.0^{3, 5}]octane 2, 3 , diademane 4 , trans-pentacyclo[3.3.2.0^{2, 9}.0^{4, 10}, 0^{6, 8}]decan 5 and bicyclo[4.1.0]heptene-2 6 . The first bands in the PE.-spectra of these compounds have been assigned on the basis of a ZDO HMO-approximation. For 2 and 4 the value for resonance integral between linked 2p atomic orbitals of two adjacent eclipsed cyclopropane rings is found to be ?1.73 eV.     

The Electronic Structure of Phenylene and Naphthylene Bicyclobutanes. Photoelectron spectroscopy and model calculations

The photoelectron (PE.) spectra of 1,2,3-methenoindane ( 2 ), 1,2,3-metheno-2,3-dihydro-1H-cyclopenta [b]naphthalene ( 3 ) and 1,2,3-metheno-2,3-dihydro-1H-phenalene ( 4 ) are investigated. The PE. spectrum of 1,3-methano-2,3-dihydrophenalene ( 7 ) is reported and compared with that of 4 . The experimental results are analyzed in terms of empirical correlation diagrams and the results of semiempirical MINDO/3 and CNDO/S calculations. The analysis indicates that the strong impact of the bicyclobutylene group on the spectroscopic properties of the aromatic π-systems in 2 , 3 and 4 is due to hyperconjugative interactions involving bicyclobutane Walsh orbitals.     

The application of the density matrix method for the investigation of the trans-effect of heteroatom in σ-electron systems

The dependence of the intramolecular charge transfer through the σ-electron systems of substituted hydrocarbons on the spatial arrangement of the X(SINGLE BOND)C_α and C_β(SINGLE BOND)C_γ bonds has been studied using the perturbation theory for the one-electron density matrix (DM). Analytical expressions for the populations of the orbitals pertinent to the cis- and trans-bonds with respect to the X(SINGLE BOND)C_α bond have been obtained and analyzed. The Hamiltonian matrix elements determining the predominant direction of the above-defined charge transfer (cis or trans) have been revealed. The electron-accepting and electron-donating substituents (X) have been considered separately and the dependence of the resulting charge-transfer direction on the properties of substituent has been established. © 1996 John Wiley & Sons, Inc.     

Platin(II)-Chromophore mit σ-gebundenen Ligatoratomen

Platinum(II) Chromophores with σ-Bonded Ligating Atoms The absorption spectra of the platinum(II) complexes PtL_xL′_4?x (L = NH₃, amine, hydride, alkyl; L′ = trialkylphosphine) consist of three band systems: (i) ligand-field bands, partially of fully screened by more intensive absorptions; (ii) at least three comparatively sharp bands of low to intermediate intensity (? = 400–10000), which are assigned to Rydberg transitions from 5d(Pt) to a linear combination of the (n+1)s-orbitals of the ligands (with a contribution of metal 6s- or 6p-orbitals, respectively); (iii) (only in the case of chromophores with two phosphorus ligands in trans-position) one high intensity band (? = 20000–50000), presumably due to a transition from the asymmetric linear combination of the trans-lying phosphorus lone-pairs to 5d_x2?y2(Pt). There is no evidence of low-lying π-combinations of phorphorus 3d-orbitals in the absorption spectra.     

Hexacoordinated Tetrel-Bonded Complexes between TF4 (T=Si,Ge, Sn,Pb) and NCH: Competition between σ- and π-Holes

In order to accommodate the approach of two NCH bases, a tetrahedral TF₄ molecule (T=Si, Ge, Sn, Pb) distorts into an octahedral structure in which the two bases can be situated either cis or trans to one another. The square planar geometry of TF₄, associated with the trans arrangement of the bases, is higher in energy than its see-saw structure that corresponds to the cis trimer. On the other hand, the square geometry offers an unobstructed path of the bases to the π-holes above and below the tetrel atom and hence enjoys a higher interaction energy than is the case for the σ-holes approached by the bases in the cis arrangement. When these two effects are combined, the total binding energies are more exothermic for the cis than for the trans complexes. This preference amounts to some 3 kcal mol⁻¹ for Sn and Pb, but is amplified for the smaller tetrel atoms.     

π-Allyl nickel halide–oxygen system as a catalyst for polymerization of butadiene

The π-allyl nickel halide-oxygen system was found to be active as catalyst for stereospecific polymerization of butadiene. The catalyst from π-allyl nickel chloride or π-allyl nickel bromide yields the polymer of 90% cis-1,4 content with high activity, whereas the catalyst from π-allyl nickel iodide affords a polymer of 70% or less cis-1,4 content. The catalyst systems can be fractionated into two parts on the basis of solubility in benzene. It is concluded that the catalyst activity originates essentially from the benzene-insoluble nickel complex which is composed of oxygen, halogen, σ-allyl group, and nickel. The structure of growing polymer terminal is discussed in relation to the mechanism of the stereospecific polymerization.