The Electronic Structure of Azuleno[1,2,3-cd]phenalene and Azuleno[5,6,7-cd]phenalene,a Comparison

The photoelectron (PE.) spectra of azuleno[l, 2, 3-cd]phenalene ( 1 ) and azuleno- [5,6,7-cd]phenalene( 2 ) have been recorded. The first five bands of both compounds could be assigned to transitions corresponding to removal of electrons from 4a₂, 6b₁, 5b₁, 3a₂ and 4b_l orbitals. This assignment is based mainly on a comparison between the observed ionization potentials and orbital energies calculated in a HMO and a PPP model. The UV./VIS. polarized absorption spectrum of 1 in the region 10000–45000 cm^?1 has been measured by means of the stretched film technique. The measurements were performed in polyethylene sheets at 77°K. Several bands could be assigned to π* ← π transitions calculated by a PPP-CI method. A comparison between the electronic structures of 1 and 2 is made by means of a simple HMO diagram.     

VUV and photoelectronic spectra of methylstannane. Theoretical and experimental approach

The vacuum ultraviolet (VUV) and photoelectron spectra of SnH₃CH₃ were recorded between 6.20 and 11.28 eV and between 8 and 17 eV, respectively. Spectra were interpreted using ab initio CI calculations. The photoelectron spectrum confirmed the low SnC bond energy. The first two ionization potentials (IP) observed were attributed to the ionization of the a₁ (10.65 eV) and e orbitals (11.15 and 11.60 eV, split by the Jahn-Teller effect), thereby showing an inversion of IPs compared with ethane. Similarly, the first two bands of the VUV spectrum (at 7.04 and 7.72–8.16 eV) were attributed to a₁ and e transitions towards the Rydberg s orbital. A splitting of the same order of magnitude as that of the photoelectron spectrum could be noted in the E state. Observed transitions between 8.65 and 10 eV showed a strong interaction between the Rydberg p MO and the σ^*_SnC antibonding orbital. Primarilyvalence transitions were encountered beyond 10 eV.     

Xanes of the Pd and Pt atoms in square and octahedral chloride complexes

The fine structure near the ionization threshold in metal X-ray L-absorption spectra of the clusters PdCl²⁻₄, PtCl²⁻₄, PdCl²⁻₆ and PtCl²⁻₆ simulating solid complex compounds of the type K₂PdCl₄ and so on has been calculated using the SCF Xα SW method. Pt L₃ absorption spectra for the complexes K₂PtCl₄ and K₂PtCl₆ have been obtained using synchrotron radiation. The pre-edge white line and the near-edge fine structure (XANES) in Pd and Pt spectra of these square and octahedral chloride complexes have been shown to arise, respectively, from electron excitation to a vacant bound molecular orbital (e_g for octahedral and b_1g for square complexes) and from photoelectron resonance elastic scattering by the metal atom and its first coordination sphere. The calculations indicated no intense pre-edge transitions for the metal L₁ spectra of these complexes and the XANES was shown to be due to several intense narrow shape resonances of the t_1u and a_2u, e_u for octahedral and square complexes, respectively.     

Trans-N2F2 and cis-N2F2: A green's function calculation on their photoelectron spectra

The vertical valence ionization potentials of trans-N₂F₂ and cis-N₂F₂ have been computed by a many-body Green function method. For trans-N₂F₂ the agreement with experiment is very satisfactory in general and the calculations permit an analysis and assignment of the experimental photoelectron spectrum. The ionization potentials of cis-N₂F₂ are predictions. The ordering of the ionization potential is for trans-N₂F₂ 5ag(n₊), 2a_u(π), 4b_u(n_?), 4ag, 1b_g(π), 1a_u(π), 3b_u, 3a_g, 2b_u and for cis-N₂F₂ 4b₂ (n_?), 2b₁ (π) + 5a₁(n+), 3b₂, 1a₂ (π), 1b₁(π), 4a₁, 3a₁, 2b2, n₊ and n_? denote lone pairs on the N atoms except for the 4b_u(n_?) orbital which has the largest contribution from the F atoms.     

Studies on the pitting corrosion of zinc in aqueous solutions II. Measurement of pitting corrosion currents operating under natural conditions

A simple experimental arrangement was applied for the measurement and the evaluation of pitting corrosion currents operating under natural conditions. The feasibility of the procedure was examined by using Zn as a test metal, K₂CrO₄, Na₂HPO₄ and Na₂WO₄ as inhibitors, and Cl^?, Br^? and I^? as pitting corrosion agents. Both the type and concentration of the inhibiting and corroding agents were varied in a programmed manner. In CrO₄^2? and HPO₄^2? solutions, the pitting corrosion currents started to flow after an induction period, which decreased with increase in the concentration of the attacking agent. In WO₄^2? solutions, on the other hand, initially high currents were recorded due to the reduction of the agent to soluble, non-inhibiting species.In all solutions tested the corrosion current reached steady-state values which depended on the type and concentration of both the inhibiting and the aggressive anions. When keeping the inhibitor concentration constant, the corrosion current varied with the concentration of the aggressor according to: log i_corr = a₁ + b₁ log c_agg On the other hand, in solutions of constant aggressor concentration, with varying inhibitor amounts, the relation was: log i_corr = a₂ ? b₂ log c_inh where a₁(a₂) and b₁(b₂) are constants.The two equations were derived theoretically on the basis of competitive adsorption of the two counteracting agents on the surface of the metal. Comparison between the experimental values of a and b, with the corresponding terms of the theoretical equations was made.The aggressivity of the three tested anions decreases in the order Cl^? > Br^? > I^?, whilst inhibition varied as CrO₄^2? > HPO₄^2? > WO₄^2?.     

Mass-analyzed threshold ionization spectroscopy of pyrimidine: determining the geometry in the first excited and the ionic ground states

Vibrational spectra of the pyrimidine cation in the electronic ground state were measured via several intermediate states of the first excited state (0⁰,16a¹, 16a², 16a⁴, 16b¹, 10b¹, 6b², 6a¹, 1¹, 4¹, 4² and 12¹) by mass-analyzed threshold ionization spectroscopy. For the first time, several vibrational modes could be assigned in the first excited and the ionic ground states. Anharmonic coupling is shown to occur in the first excited state due to Fermi resonance between the 1¹ and the 16a⁴ vibrations. From the results of the measurements and calculations presented here, pyrimidine is predicted to be planar in the first excited and the ionic ground states, and it belongs to the C_2V point group.     

Picosecond reversible reaction kinetics of excited p-dimethylaminoacetophenone and m-methyl-p-cyanodimethylaniline studied by oxygen quenching technique

Double fluorescence of p-dimethylacetophenone (DMAPh) in CH₃CN and m-methyl-p-cyanodimethylaniline (MCDMA) in CH₂Cl₂ has been observed and analyzed in terms of reversible excited state isomerisation of the primary excited form b^* to the strongly polar rotamer a^*. Using the oxygen quenching technique, the kinetics of the reactions have been solved and all rate constants separated. The “formal” lifetimes of the species b^*, τ_b ≡ (k_bf + k_bd + k_ba)^?1, are 1 ps and 2.2 ps for DMAPh and MCDMA, respectively. The first value fits well to the reorientation relaxation time of acetonitrile.     

Theoretical studies of photoexcitation and ionization in hydrogen sulfide

Computational studies are reported of photoexcitation and partial-channel photoionization processes in the valence shell of H₂S employing single- and coupled-channel, vertical-electronic, static-exchange approximations. Detailed assignments are provided on the basis of the calculations of all prominent features observed below the first ionization threshold in recent photoabsorption studies. Comparisons are also made with experimental partial-channel photoionization cross sections obtained from electron-impact measurements in the dipole limit, and with branching ratios obtained from synchrotron-radiation photoelectron spectroscopy studies. The calculated discrete valence-shell excitation series are in generally good agreement with recent high-resolution VUV spectral measurements, although some of the present assignments are not in accord with those suggested on basis of the experimental data alone, nor with those based on earlier computational studies. The origins of these discrepancies are indicated and clarified. Configuration mixing is seen to influence the absorption intensities in the H₂S valence-shell spectrum, particularly in ¹A₁ → ¹A₁ and ¹A₁ → ¹B₂ symmetries due to the presence of intravelence excitations in these cases. The calculated valence-shell partial-channel photoionization cross sections are in good accord with the recent electron-impact study, and with branching ratios obtained from synchrotron-radiation measurements. Agreement with previous computational studies is not entirely satisfactory, however. The discrepancies are attributed to use of Coulomb and local-potential approximations in the earlier calculations. As in previous reports in this series on molecular photoabsorption and photoionization in polyatomic molecules, the general natures of the excitation and ionization spectra in H₂S are clarified on basis of the presence of valence-like (3b₂(σ^*), 6a₁(γ^*)) and diffuse orbital contributions to both discrete and continuum states.     

The Electronic Structure and Bonding of the First p-Block Paddlewheel Complex,Bi<Subscript>2</Subscript>(trifluoroacetate)<Subscript>4</Subscript>, and Comparison to d-Block Transition Metal Paddlewheel Complexes: A Photoelectron and Density Functional Theory Study

The photoelectron spectrum and a density functional computational analysis of the first p-block paddlewheel complex, Bi₂(tfa)₄, where tfa = (O₂CCF₃)⁻, are reported. The photoelectron spectrum of Bi₂(tfa)₄ contains an ionization band between the region of metal-based ionizations and the region of overlapping ligand ionizations that is not seen in the photoelectron spectra of d-block paddlewheel complexes. This additional ionization arises from an a_1g symmetry combination of the tfa ligand orbitals that is directed for σ bonding with the metals, and the unusual energy of this ionization follows from the different interaction of this orbital with the valence s and p orbitals of Bi compared to the valence d orbitals of transition metals. There is significant mixing between the Bi–Bi σ bond and this a_1g M–L σ orbital. This observation led to a re-examination of the ionization differences between Mo₂(tfa)₄ and W₂(tfa)₄, where the metal–metal σ and π ionizations are overlapping for the Mo₂ molecule but a separate and sharp σ ionization is observed for the W₂ molecule. The coalescing of the σ and π bond ionizations of Mo₂(tfa)₄ is due to greater ligand orbital character in the Mo–Mo σ bond (∼7%) versus the W–W σ bond (∼1%). In tribute to F. Albert Cotton for sharing the beauty of symmetry and the joy and excitement in the exploration of metal–metal bonds.     

Highly Kinked Uranyl Chromate Nitrate Layers in the Crystal Structures of A[(UO2)(CrO4)(NO3)] (A = K,Rb)

Two first uranyl chromate nitrates, K[(UO₂)(CrO₄)(NO₃)] ( 1 ) and Rb[(UO₂)(CrO₄)(NO₃)] ( 2 ), were prepared by solid‐state reactions and characterized by electron microprobe analysis and single‐crystal X‐ray diffraction. The compounds are isotypic [ 1 : monoclinic, P2₁/c, a = 9.881(5), b = 7.215(4), c = 14.226(6) Å, β = 124.85(3)°, V = 832.3(7) ų; 2 : monoclinic, P2₁/c, a = 9.804(1), b = 7.359(1), c = 14.269(1) Å, β = 122.048(4), V = 872.6(1) ų]. The structures of 1 and 2 are based upon the complex [(UO₂)(CrO₄)(NO₃)]^– layers with unprecedented structural topology, which consist of the UrO₃NO₃ units linked through CrO₄ tetrahedra. The resulted kinked layer can be divided into chains arranged in the ladder fashion. The layers are parallel to (100) and are linked by A⁺ (A = K, Rb) cations located between the layers.     

Crystal Structures of the Europium and Yttrium Hydroxychromates Eu(OH)(CrO4) and Y(OH)(CrO4); Structural Evolution as a Function of the Ln3+ Ionic Radius

The compounds Eu(OH)(CrO₄) and Y(OH)(CrO₄) were obtained under hydrothermal conditions and characterized by single‐crystal X‐ray diffraction analysis. They are isostructural and crystallize in the monoclinic system, space group P2₁/n (no. 14) with lattice parameters a = 8.278(1) Å, b = 11.400(2) Å, c = 8.393(1) Å, β = 93.76(2)°, V = 790.3(2) Å³, Z = 4, d = 4.79 g · cm^–3 for Eu(OH)(CrO₄) and a = 8.151(1) Å, b = 11.362(2) Å, c = 8.285(1) Å, β = 94.23(1)°, V = 765.2(2) Å³, Z = 4, d = 3.85 g · cm^–3 for Y(OH)(CrO₄). The [EuO₈] polyhedra form infinite double chains along the a direction, which are connected by common edges and corners. These double chains are related together in the two other directions by the [CrO₄]^2– tetrahedra to form a three‐dimensional network in which channels appear parallel to the [100] direction. We examine the structural evolution, as a function of the Ln³⁺ ionic radius, in the series Ln(OH)(CrO₄) compounds (with Ln = Nd, Eu, Gd, Tb, Er, Yb) and Y(OH)(CrO₄). To determine the best coordination number of each lanthanide and yttrium ions, different calculations of bond valence sum were realized.     

Substituted 5-Antipyrinylazo-4-phenyl-2-aminothiazoles as Disperse Dyes for Dyeing Polyester Fabrics

Summary. A series of some new substituted 5-antipyrinylazo-4-phenyl-2-aminothiazole disperse dyes was synthesized by diazocoupling of 4-antipyrinyldiazonium chloride with aminothiazole derivatives. The synthesized dyes were characterized by UV-Vis absorption, IR, ¹H NMR, and MS spectroscopy. The dyes gave orange to reddish-violet shades with very good depth and levelness when applied to polyester fabrics as disperse dyes and their fastness properties were evaluated on polyester fibers. Also the position of color in CIELAB coordinates (L^*, a^*, b^*, H^*, and C^*) was assessed.     

Substituted 5-Antipyrinylazo-4-phenyl-2-aminothiazoles as Disperse Dyes for Dyeing Polyester Fabrics

A series of some new substituted 5-antipyrinylazo-4-phenyl-2-aminothiazole disperse dyes was synthesized by diazocoupling of 4-antipyrinyldiazonium chloride with aminothiazole derivatives. The synthesized dyes were characterized by UV-Vis absorption, IR, ¹H NMR, and MS spectroscopy. The dyes gave orange to reddish-violet shades with very good depth and levelness when applied to polyester fabrics as disperse dyes and their fastness properties were evaluated on polyester fibers. Also the position of color in CIELAB coordinates (L^*, a^*, b^*, H^*, and C^*) was assessed.     

The ionization energies of bridged [14]annulenes and of dicyclohepta[cd,gh] pentalene

The ionization energies J_J, of 1,6;8,13-alkanediylidene-[14]annulenes ( 2 to 5 ) and of dicyclohepta[cd,gh]pentalene ( 1 ) have been determined by photoelectron spectroscopy, using HeI radiation. The data are interpreted in terms of Koopmans' theorem (J_J = ?ε_J) on the basis of correlation diagrams and with the help of simple molecular orbital models. If the bridge is an ethane-, propane- or butane-diylidene group, the π-orbital sequence, in descending order of orbital energies, is (in C_2v): b₁, b₂, a₂, a₁. The sequence is due to a complicated and not uniquely definable interplay of inductive, conjugative and homoconjugative effects. A detailed analysis of these effects suggests that the effective angle of twist between two consecutive basis-AOs 2p_μ, 2p_ν of the peripheral π-system should be smaller than the twist angles θ_μν determined by X-ray analysis, i.e. that the pi;-ribbon adjusts elastically and is no longer locally orthogonal to the σ-frame. In the non-alternant hydrocarbon 1 of symmetry D_2h, the sequence is 2b_2g, 3b_1u, 2b_3g, 1a_u, 2b_1u. The sequence 3b_1u above 2b_3g, _i.e. the reverse of b₂ above a₁ in the bridged [14]annulenes, is explained as being due to the interaction of the semilocalized perimeter orbitals b_1u and b_3g with the bonding (π(B_1u))and antibonding (π*(B_3g)) orbital of the central double bond. In 2 the replacement of the two latter orbitals by the Walsh-orbitals of the cyclopropane moiety leads to the sequence b₁, b₂, a₁, a₂. From the data observed for 1 to 5 and for 1,6-methano-[10]annulene [11], a crude estimate for the orbital energies of the hypothetical all-cis D_10h-[10]- and D_14h-[14]annulenes can be derived.     

Kinetics and mechanisms of oxidation of 1-octene and heptanal by crown ether-solubilized potassium permanganate in non-aqueous solvents

The kinetics of oxidation of 1-octene and heptanal by 18-crown-6-ether-solubilized KMnO₄ in benzene and CH₂Cl₂ have been investigated. In benzene, the oxidation of 1-octene is first order with respect to the oxidant and zero order with respect to the substrate, whereas in CH₂Cl₂ the reaction is first order with respect to both substrate and oxidant. The reaction of heptanal followed different kinetics being first order with respect to both substrate and oxidant, regardless of whether benzene or CH₂Cl₂ was employed as the solvent. The values of activation energy E _a, standard enthalpy H ^*, standard entropy change S ^*, and standard free energy G ^*, for the reaction, are reported. Mechanistic pathways for the studied reactions are also proposed.     

Solvent-dependent reactivities of acyclic nitrones with β-diketones: catalyst-free syntheses of endiones and enones

Reactions of the nitrones ^?O⁺N(Me)C(H)Ar 1 (Ar=phenyl 1a, 4-methylphenyl 1b, 2,4,6-trimethylphenyl 1c, and anthracen-9-yl 1d) with the cyclic β-diketones 1,3-indandione 2 or barbituric acid 3 in CH₂Cl₂, afford the corresponding endiones 2′a–2′d or 3′a–3′d. In contrast, dimedone 4 reacts with 1a or 1b to give the endione 4′a or 4′b and the bis-adduct 4″a or 4″b. Nevertheless, reaction of 4 with 1c or 1d in CH₂Cl₂ furnishes only the endione adducts 4′c or 4′d. However, the reaction of 4 with 1a or 1b in methanol gives only 4″a or 4″b, respectively. Among acyclic β-diketones only malonic acid 7 reacts with 1a–1c. Reaction of 7 with 1a in CH₂Cl₂ forms cinnamic acid 7″a, whereas in the case of 1b, the endione 7′b and (E)-3-p-tolylacrylic acid 7″b are obtained. The nitrone 1c reacts with 7 in CH₂Cl₂ to afford the endione 7′c or with acetone yielding (E)-4-mesitylbut-3-en-2-one 8. X-ray analyses are reported for 4′c, 5, and 7″b. In addition, the calculated acidity of the hydrogen at the α-C atom is shown to correlate with the reactivity of the β-diketones with nitrones.     

The chemistry of chromium(V) oxide trichloride

Summary The recent upsurge of interest in chromium(V)^(1–8) has highlighted two features of especial interest in its chemistry. Firstly, the complexes of chromium(V) are considerably more stable than has generally been assumed in the past, as exemplified by the recent characterisation of a water soluble complex, potassium bis(2-hydroxy-2-methylbutyrato)oxochromate(V)⁽¹⁾. Secondly, the d1 electronic configuration of the complexes makes them ideal model systems for study by such techniques as electron paramagnetic resonance (²) and electronic absorption spectroscopy^(3,4) . Although chromium(V) oxide trichloride was first prepared in 1962, by the reaction between chromium(VI) oxide and SOCl₂ or SO₂Cl₂ ^{(9 10)}, and subsequently by the reaction between CrO₂Cl₂ and BCl₃ ⁽¹¹⁾, its chemistry and physical properties have remained virtually unstudied. We report here the first series of reactions of CrOCl₃, along with details of its i.r. and photoelectron spectra.     

1H NMR,IR and UV/VIS Spectroscopic Studies of Some Schiff Bases Derived from 2‐Aminobenzothiazole and 2‐Amino‐3‐Hydroxypyridine

By condensing 2‐aminobenzothiazole with 2‐hydroxy‐1‐naphthaldehyde, 2‐hydroxybenzaldehyde, 4‐methoxybenzaldehyde, 4‐hydroxybenzal‐dehyde, benzaldehyde and 4‐dimethylaminobenzaldehyde, and five Schiff bases Ia‐Ie are prepared. Also, two Schiff bases IIa and IIb are prepared by condensation of 2‐amino‐3‐hydroxypyridine with 2‐hydroxy‐1‐naphthaldehyde and 2‐hydroxybenzaldehyde. The ¹H NMR, IR and UV/Vis spectra of these seven Schiff bases are investigated. The signals of the ¹H NMR spectra as well as the important bands in the IR spectra are considered and discussed in relation to molecular structure. The UV/Vis absorption bands in ethanol are assigned to the corresponding electronic transitions and the electronic absorption spectra of Schiff bases Ib and IIb are studied in organic solvents of different polarities. The UV/Vis absorption spectra of 2‐amino‐3‐hydroxypyridine Schiff bases IIa and IIb are investigated in buffer solutions of different pH values containing 5% (v/v) methanol, and the results are utilized for the determination of pK_a and ΔG^* of the ionization of the phenolic OH‐groups. The fluorescence spectra of IIa and IIb are studied in organic solvents of different polarities. The obtained spectral results are confirmed by some molecular calculations using the atom super position and electron delocalization molecular orbital theory for the Schiff base IIb.     

AB initio and configuration interaction calculations for some σ → π* superexcited states of the trans-1,3-butadiene molecule

Some σ → π¹ superexcited states of the trans-1,3-butadiene molcule have been calculated in order to establish them as possible candidates for the 9.52 eV and 11.04 eV transitions observed in the electron impact spectra of this molecule. Four states have been solved self-consistently ( 7a_g→ 2a_u2a_gand 2b_g and 6b_u→ 2a_u, 2bg) and on the basis of extensive CI calculations of transition energies and oscillator strengths, we assign the 11.04 eV transition to the ¹B_g (6b_u→ 2a_u) state. The transition observed at 9.52 eV is more likely to be either a π (la_u) → π1 transition or the first member of a Rydberg series converging to the second ionization potential.     

The electronic structure of molecules by a many-body approach: V. Ionization potentials and one-electron properties of cyclopentadiene and 1-sila-cyclopentadiene-(2,4)

The valence ionization potentials (IP's) of cyclopentadiene and 1-sila-cyclopentadiene-(2,4) are studied by an ab initio many-body approach which includes the effect of electron correlation and reorganization beyond the Hartree-Fock approximation. The Hartree-Fock approximation gives the correct ordering of the IP's for cyclopentadiene but this ordering does not agree with the results of the previous experimental and theoretical studies. The ordering is 1a₂(π), 2b₁(π), 4b₂, 6a₁, 5a₁, 3b₂, 1b₁ (π), 4a₁, 2b₂, 3a₁. For sila-cyclopentadiene the ordering of the IP's is: 1a₂(π), 4b₂, 2b₁(π), 6a₁, 1b₁(π), 5a₁, 3b₂, 4a₁, 3a₁, 2b₂. The Hartree-Fock approximation is found to be incorrect with respect to the ordering of the 4b₂ and 2b₁(π) IP's. A number of one-electron properties are calculated in the one-particle approximation and compared with the available experimental data.