The electronic structure of the SbF2−5 ion and isoelectronic species

The electronic structure of the SbF²⁻₅ion and the isoelectronic species TeF⁻₅, IF₅ and XeF⁺₅ are calculated using the Discrete Variational X_α-method (DVM-X_α). The nature of chemical Bonding is analysed in terms of a Mulliken population scheme. The factors leading to geometrical distortions of the SbF²⁻₅ coordination polyhedron are discussed. The results of calculations cast doubts on the validity of the assumption that the geometry of the anion is influenced by the lone pair.     

On the possibility of existence of η5-π-complexes of C60 fullerene: π-complexes with silicon

Qualitative estimates of possibility of the formation of fullerene ⁵--complexes have been carried out by the MNDO/PM3 method. It was shown, as exemplified by the C₆₀ cluster, that the introduction of five univalent functional groups R (R = H, Cl, Br) to -positions of a separate pentagon of C₆₀ with the formation of [R₅C₆₀]^– anions results in a pronounced increase in the -electron density on the atoms of this five-membered cycle and more favorable conditions for the formation of -bonds with the ⁵-ligand. The nature of the interaction between the atoms of the separate cycle in [R₅C₆₀]^– anion and ⁵-ligand was analyzed by the example of hypothetical sandwich systems R₅C₆₀SiCp. Half-sandwich complexes R₅C₆₀SiX (X = H, Cl) were also investigated. The local energy minima were found on the potential energy surfaces (PES) of systems R₅C₆₀SiCp and R₅C₆₀SiX with C_5p symmetry. These systems transform barrirlessly into q5-7E-complexes with the angular structure if the symmetry restrictions are removed. The most favorable conditions for ⁵--complexes of R₅C₆₀ to form are realized for R = H. The results obtained were compared to those of semiempirical and nonempirical calculations of bis (cyclopentadienyl) silicon.Translated fromIzvestiya Akademii Nauk. Seriya Khimicheskaya, No. 10, pp. 2422–2429, October, 1996.     

Is the FeC cluster linear? Theoretical study of the equilibrium structure and bonding of FeC

Ab initio electron correlation methods and density functional theory are used to investigate the structure, bonding, and stability of FeC. Theoretical calculations show that the ground state of the FeC anion strongly depends on the level of theory. The linear ⁴Σ^? state with an open configuration δ²σ¹ is predicted to be the ground state of FeC at the coupled‐cluster theory restricted to single, double, and noniterative triple excitations (CCSD[T])//CISD and multireference (MR) second‐order Moller–Plesset (MP2)//CAS self‐consistent field (SCF) levels. Next stable conformations are a C_2V ring structure II (⁴B₂) and a C_2V structure III (⁴A₂) in which Fe is bonded to one carbon atom of a triangular C₃. However, CISD and CCSD//CISD calculations show that the C_2V ring structure II and the C_2V structure III are more slightly stable than is the linear structure I of FeC. The harmonic vibrational frequencies and relevant vertical electron binding energies are reported. Possible detachment transitions in the photoelectron spectrum of FeC are discussed on the basis of current calculations. © 2003 Wiley Periodicals, Inc. Int J Quantum Chem 93: 275–279, 2003     

Synthesis,molecular structure and reactivity of new π-conjugated diyne with ferrocenyl and phenyl units

New π-conjugated butadiynyl ligand FcC(CH₃)₂Fc′–CC–CC–Ph (L₁) has been synthesized and its reaction with Co₂(CO)₈ has been studied. New clusters [FcC(CH₃)₂Fc′–CC–CC–Ph][Co₂(CO)₆]_n [(1): n = 1; (2): n = 2] and [Fc–CC–CC–Ph][Co₂(CO)₆]_n [(3): n =  1; (4): n = 2] were obtained by the reaction of ligands FcC(CH₃)₂Fc′–CC–CC–Ph (L₁) and Fc–CC–CC–Ph (L₂) with Co₂(CO)₈ respectively and the composition and structure of the clusters and ligands have been characterized by elemental analysis, FTIR, ¹H and ¹³C NMR and MS. The crystal structures of compounds L₁, L₂, 2 and 4 have been determined by X-ray single crystal analysis.     

Electronic structure and absorption spectra of supramolecular complexes of a fullerene crown ether with a π-extended TTF derivative

The present work is a theoretical investigation on supramolecular complexes of a fullerene crown ether (A and B isomers) with a derivative of π-extended tetrathiafulvalene (T). The geometry and the electronic structure of seven different conformers of the complex of dibenzo-18-crown-6 ether of fullero-N-methylpyrrolidine with a N-benzyl-N-(4-{[9,10-bis(1,3-dithiol-2-ylidene)-9,10-dihydroanthracen-2-yl]ethynyl}benzyl)ammonium cation were determined. We calculated the complexation energies and the absorption spectra, i.e., the lowest 50 excited electronic states of the complexes have been determined at the ground state optimum geometry. All calculations were carried out employing the density functional theory (DFT) and the time-dependent DFT, using the B3LYP, CAM-B3LYP, ωB97X-D, and M06-2X functionals in conjunction with the 6-31G(d,p) basis set. Various types of van der Waals interactions are observed in the complexes. Conformer complexation energies (CE) range from 2.54 to 2.14 eV in the gas phase and from 1.75 to 1.34 eV in CHCl(3) solvent at the ωB97X-D/6-31G(d,p)//M06-2X/6-31G(d,p) level of theory. There are three major features at about 390, 330, and 290 nm in the calculated absorption spectra of all the conformers. The major peaks correspond to T→T, T→T/F (electron density in both T and the fullerene F of B) and to T→F transitions, depending on the particular conformer. Other charge transfer T→F transitions are observed close to the T→T transition, indicating the possibility of photoinduced electron transfer in all these complexes.     

Ab initio MO LCAO SCF simulation of molecular and electronic structure of η5-π-C60H5XCp (X=Fe, Si) complexes

The problem of existence of η⁵-π-complexes of unsubstituted fullereneI _h -C₆₀ and its cyclopentadienyl type derivative C₆₀H₅ ^. is discussed.Ab initio MO LCAO SCF calculations of hypothetical sandwich systems η⁵-π-C₆₀H₅XCp (X=Fe (1a), Si (1b)), the cationic complex C₆₀FeCp⁺ of unsubstituted C₆₀, and the C₆₀H₅ ^. radical were performed in the STO-3G and 3-21G basis sets. In the1a, 1b, and C₆₀H₅ ^. systems, hydrogen atoms are attached to carbon atoms of fullerenei _h -C₆₀ at α-positions relative to the same pentagonal face (pent ^*). In η⁵-complexes, XCp species are also coordinated to this face. According to calculations in the 3-21G basis set, the Fe-pent ^* bond energy in complex1a is much higher than those of similar bonds in1b and in the η⁵-π-C₆₀FECp⁺ cation (117 kcal mol⁻¹ vs. 37 and 64 kcal mol⁻¹, respectively) and is 7 kcal mol⁻¹ higher than the Fe−Cp bond energy in the classical sandwich system FeCp₂. The Fe…C _pent* and Fe…C_Cp distances in complex1a are slightly shorter than the Fe…C distance in the ferrocene molecule. The spin populations in the C₆₀H₅ ^. radical are almost completely localized on the atoms of thepent ^* face, which must favor the formation of η⁵-π-complexes of this radical. Translated fromIzvestiya Akademii Nauk. Seriya Khimicheskaya, No. 9, pp. 1657–1662, September, 1999.     

Synthesis and photophysical properties of heptamethine cyanine–fullerene C60 dyads with non-quenched fluorescence

Two new heptamethine cyanine dye–fullerene C₆₀ covalently- linked dyads, which absorb in far-red and NIR spectral regions, have been synthesized by esterification click reaction and characterized by physicochemical methods. No significant fluorescence quenching was found due to weak electronic coupling between heptamethine moiety and fullerene core, which was confirmed by photophysical and electrochemical methods. Such dyads can be useful for cell imaging and fluorescence diagnostics of various fullerene derivatives.     

Structural and electronic properties of S-doped fullerene C58: where is the S atom situated?

Structural and electronic properties of S-doped fullerene C58 were calculated systematically via Hartree-Fock self-consistent field (SCF) and density functional B3LYP levels of theory with 6-31G(d) basis set. The most stable C58S represents an open cage structure with a nine-member ring orifice, which provides a large hole for large atoms or small molecules to pass through into the cage. The most stable endohedral S@C58 has the S atom seated near the center of the C58 cage. The calculated highest occupied molecular orbital-lowest unoccupied molecular orbital energy gaps of the isomers lie in the range of 1.42-2.50 eV. The electron affinity and the ionization potential were also presented as an indicator of the kinetic stability. Our results may aid in the design of experimental methods for controlling the nature of fullerene cages (for example, doping, opening, and reclosing them).     

Electronic and steric effects controlling efficiencies of photoaddition reactions of fullerene C60 with N-α-trimethylsilyl-N-alkyl-N-benzylamines

Single electron transfer (SET)-promoted photoaddition reactions between fullerene C₆₀ and both various alkyl (Me, Et, i-Pr, t-Bu)- and para-substituted (p-Me, p-OMe, p-F, p-CF₃) arene ring containing, N-α-trimethylsilyl-N-alkyl-N-benzylamines were explored to gain information about photoproduct profiles and how the electronic and steric nature of the amine substrates influence reaction efficiencies. The results show that visible light (λ > 540 nm) irradiation of 10% EtOH-toluene solutions containing C₆₀ and N-α-trimethylsilyl-N-alkyl-N-benzylamines produce 1-aminomethyl-1,2-dihydrofullerenes as a sole photoproduct. In addition, SET-promoted photoaddition reactions of unsubstituted and para-electron donating group substituted arene ring containing N-α-trimethylsilyl-N-alkyl-N-benzylamines take place to give photoproducts more efficiently than those containing para-electron withdrawing group substituted arene rings. Moreover, although steric factors are less significant than the electronic nature of the amine substrates in governing reaction efficiencies, sterics do play a significant role in photoreactions of electron deficient amine substrates.     

Synthesis, crystal structure, and spectral studies of the molecular complex of [60]fullerene with chloro(triphenylphosphine)gold(I), C60·2[(Ph3P)AuCl]

The molecular complex C₆₀·2[(Ph₃P)AuCl] (1) was synthesized. The crystal and molecular structure of1 was established by X-ray diffraction analysis. At room temperature, the [60]fullerene molecules in complex1 are ordered due to π—π interactions between C₆₀ and the phenyl rings of the chloro(triphenylphosphine)gold(1) molecules. The satellite structure, which accompanies the Cls photoelectron peak of complex1, is indicative of a partial suppression of a channel of losses due to π→π transition in the phenyl ring. The 1R spectral data indicate that either a charge is absent or the charge transfer to the fullerene molecule is negligible. Translated fromIzvestiya Akademii Nauk. Seriya Khimicheskaya, No. 2, pp. 365–369, February, 2000.     

Complex formation of 2,4,6-triallyloxy-1,3,5-triazine with copper(I,II) chloride. Synthesis and crystal structure of the Cu3Cl4 · 2C3N3(OC3H5)3 π-complex

The mixed-valence Cu₃Cl₄ · 2C₃N₃(OC₃H₅)₃ π-complex (I) is synthesized from 2,4,6-triallyloxy-1,3,5-triazine (L) and copper(II) chloride by the alternating-current electrochemical method in an ethanolic solution. Single crystals of complex I are studied by X-ray diffraction analysis: space group I4₁/a, a = 25.39(8), c = 10.14(6) Å, V = 6537(48) ų, Z = 8, R = 0.0814. The copper(I) and chlorine atoms form unique cyclic tetramers Cu₄Cl₄. The coordination sphere of each copper(I) atom includes the C=C bond of the allyl group of the ligand molecule L in addition to the two bridging chlorine atoms. Two nearest triazine rings are coordinated through the nitrogen atoms to the copper(II) atoms, whose environment is completed to a square with two chlorine atoms. An intricate three-dimensional structure is formed due to the μ₄-bridging function of the cupro(I) tetramer and the μ₂-bridging function of the ligand molecule L.     

Crystal structure of a new π-complex of AgClO4 with 1-allyl-5-(2-pyridyl)-1H-tetrazole of the composition [Ag2(C9H6N5)2](ClO4)2

By the AgClO₄ interaction with 1-allyl-5-(2-Pyridyl)-1H-tetrazolee (1aPyt) in a methanol solution, an [Ag₂(1aPyt)₂](ClO₄)₂ π-complex is obtained, which is studied using single crystal X-ray diffraction.     

The formation and molecular structure of (η5-C5H5)3Sm · OC4H8

Reaction of 1/2 mole ratio of (η⁵-C₅H₅)SmCl₂ ·3THF and NaCCCH₂OCH₂CHCH₂ in THF solution resulted in the formation of (η⁵-C₅H₅)Sm·OC₄H₈; the complex crystallizes in monoclinic space group P2₁/n with unit cell constants a = 8.254(5), b = 24.63(1), c = 8.339(3) Å, β = 101.33(5)° and D_c = 1.67 g/cm³ for Z = 4. Refinement has led to a final R value of 0.041 based on 2106 independent observed reflections. The THF molecule is coordinated to the samarium atom at a SmO distance of 2.522(6) Å. The SmC(cyclopentadienyl) bond lengths range from 2.70(1) to 2.80(1) Å and average 2.742(1) Å. A comparison of some significant structural parameters along the isostructural series (η⁵-C₅H₅)₃Ln·THF (LnLa, Pr, Nd, Gd, Dy, Lu and Sm) with the ionic radii of Ln³⁺ was made.     

Synthesis and crystal structure of the molecular complex of fullerence C60 with 2-(4-thiono-1,3-dithiolan-5-ylidene)-4,5-dimethyl-1,3-diselenol (C60·2DTDS)

A new molecular complex of fullerene C₆₀ with 2-(4-thiono-1,3-dithiolan-5-ylidene)-4,5-dimethyl-1,3-diselenol (C₆₀·2DTDS) was synthesized for the first time. The crystal and molecular structures of C₆₀·2DTDS were established by X-ray diffraction analysis. The crystal structure of C₆₀·2DTDS is layered: the layers of fullerene C₆₀ molecules alternate with those of DTDS molecules. The molecules of C₆₀ and DTDS are associated by shortened C...Se, C...S, and C...C contacts forming a three-dimensional network of secondary interactions in the crystal. The C₆₀·2DTDS crystals have a specific feature: the absence of shortened C...C contacts between the nearest C₆₀ molecules despite the short distances between their centers, 9.948(2) and 10.054(2) Å. The electrochemical properties of DTDS were studied by cyclic voltammetry in CH₂Cl₂/0.05M Bu₄NPF₆ at room temperature. DTDS undergoes reversible one-electron reduction to a radical anion [E ^o=?1.81 V (Fc^0/+)] and reversible one-electron oxidation to a radical cation [E ^o=+0.37 V (Fc^0/+)]. The degree of charge transfer in C₆₀·2DTDS, ΔN=0.18, calculated from the electrochemical parameters of DTDS and C₆₀ indicates that this compound is a molecular complex with a partial charge transfer.     

Molecular complex of C60 fullerene with an organic π-donor,bis(methylenedithiotetrathiafulvalene): synthesis,crystal structures,and properties

A new molecular complex based on [60]fullerene, namely, (BMDT-TTF)·C₆₀·2CS₂ (1) (where BMDT-TTF is bis(methylenedithiotetrathiafulvalene)) was synthesized. The molecular and crystal structures of 1 were established by X-ray diffraction analysis. Complex 1 has a layered structure, layers of C₆₀ molecules alternating with those formed by BMDT-TTF molecules and CS₂ molecules located between them. In complex 1, there are short contacts between C₆₀ and the donor molecules, which results in a changed BMDT-TTF geometry. The donor molecules in 1 form in addition short S...S contacts. The data of IR spectroscopy indicate that the charge transfer to the fullerene molecule is insignificant if at all present. The conductivity of a single crystal of 1 measured at 20 °C using a four-contact method is 2·10^–5 ( cm)^–1.     

Ab initio study of the molecular vibrations and electronic structure of the X,B, D and F2Σ+ states of AlO

Molecular vibrations and electronic structure of the X²Σ⁺, B²Σ⁺, D²Σ⁺, and F²Σ⁺ states of AlO are studied by carrying out ab initio configuration interaction calculations and molecular vibration calculations using accurate potential energy functions. An avoided crossing between the D²Σ⁺ and F²Σ⁺ potential energy curves occurs in the neighborhood of 4.0 a₀ and results in irregular vibrational levels of the D and F²Σ⁺ states. The vibrational constants for the F²Σ⁺ state are predicted from the vibrational levels not involved in the irregularity. Configuration mixing is important in describing the B, D, and F²Σ⁺ states. The F²Σ⁺ state at and around its well minimum and the D and F²Σ⁺ states in the avoided crossing region are characterized in terms of their main configurations and dipole moment functions.     

Synthesis of some bis(triphenylphosphine)(ethynylferrocenyl) platinum(II) complexes; molecular structure of [PtH(CC-C5H4FeC5H5)(PPh3)2]

Substituted acetylidoplatinum(II) complexes trans-[PtX(CC-C₅H₄FeC₅H₅)(PPh₃) ₂] (X  H, Cl, CCPh or CC-C₅H₄FeC₅H₅) have been prepared. Controlled basicity of the reaction solutions yields the different complexes. A single-crystal X-ray diffraction study of trans-[PtH(CC-C₅H₄FeC₅H₅)(PPh₃)₂] indicates an alternating alignment of the ethynyl ligands between two centrosymmetric platinum atoms, resulting in the formation of a pseudo- polymeric structure.