Nuclear Magnetic Resonance Spectra of Polyhydroxylated Fullerene C60(OH)n

Polyhydroxylated fullerene C₆₀(OH)_n (with an estimated number of hydroxyl groups n = 38–44) synthesized from pure fullerene by mixing a benzene solution of C₆₀ with a NaOH aqueous solution in the presence of a catalyst was studied with ¹H and ¹³C solid-state nuclear magnetic resonance. Possible features of the structure of a molecule shell were revealed from ¹H NMR data. The ¹³C spectrum showed a peak splitting with an increase in temperature, which is probably due to fullerenol isomers.

     

13C NMR and Fukui function analysis on C82 hydroxylated fullerene through density functional theory

Density functional theory calculations were performed on C₈₂ hydroxylated fullerene. B3LYP and PBE0 functionals with 6-31G** basis set were utilised to get chemical shieldings, chemical shifts and the isotropic Fermi contact coupling on each atomic site. A relation between nuclear magnetic resonance (NMR) properties and reactivity of the molecule, obtained through the electronic Fukui function, was observed. Interestingly, the most stable configurations of OH groups adsorbed on C₈₂ surface were obtained when the hydroxyl groups are adsorbed on deshielded (isotropically and anisotropically) sites. For open-shell systems, a relation between isotropic Fermi contact, spin density and average Fukui function was found, that is, sites with a great amount of Fukui function (analytical and the one obtained through finite difference) and spin density have the largest isotropic Fermi contact coupling data. With the adsorption of the first hydroxyl molecules, spin densities and Fukui functions show preferential sites to adsorb the following OH groups close to previously adsorbed. Additionally, theoretical spectra of chemical shifts of C₈₂(OH)_n (n = 1, 2, 3 and 4) were obtained and they were compared with experimental reports, getting a reasonable comparison. For example, regarding ¹³C NMR chemical shifts obtained in C₈₂OH molecule, 80 ppm (B3LYP) and 79 ppm (PBE0) were calculated on hydroxylated carbon, which is in good agreement with experimental results in C₆₀ fullerols.     

Optical spectra of high-symmetry isomers 60(CH3-r 6-H)n at n=3, 6

Earlier, we found the energies of formation and the electron band structures of the fullerene molecule C₆₀ and its methylated and hydrogenated chemical derivatives with saturated r ₆ bonds of the type C₆₀(CH₃-r ₆-H)_n with n from 1 to 6. Based on the self-consistent molecular-orbital method, we found the energies of singlet and triplet excitations for each molecule by the ΔSCF technique. We compared the electron structure of the fullerene molecule with experimental data and other theoretical calculations and showed that the semiempirical quantum-chemical technique used in our work satisfactorily explains the experimental photoluminescence spectra of fullerene-containing star-shaped polystyrenes. Partial or complete removal of the dipole inhibition for the transitions in isomers that are formed upon chemical saturation of double bonds makes it possible to follow changes in the electron structure of the pπ shell of the fullerene molecule by spectroscopic techniques. Specific optical spectra of the first excited singlet states (spectra of absorption, luminescence, and excitation of luminescence) as well as phosphorescence of the first spin-triplet state are described.     

Nanostructural magnetism of polymeric fullerene crystals

The nature of magnetism in all-carbon crystals composed of polymeric layers of covalently bound fullerene (C₆₀) molecules is considered. The results of quantum-chemical calculations performed using the unrestricted Hartree-Fock approximation and the semiempirical AM1 method are presented. It is shown that the exchange integrals J of both a free C₆₀ molecule and a monomer unit of the polymer are too large ensure the required magnetic susceptibility of the fullerene crystal. However, the J value exhibits an approximately n-fold decrease for an oligomer molecule consisting of n C₆₀ units. Therefore, in the case of large n, the exchange integral can be reduced to a low level sufficient to provide for a significant magnetic susceptibility. A nanosize (scaly) model of the observed magnetism is proposed that is consistent with recent experimental data, which are indicative of a nanostructural character of magnetic fullerene samples.     

Theoretical study on the sequential hydroxylation of C82 fullerene based on Fukui function

In the present work semi-empirical PM3 method and ab initio density-functional theory calculations were performed in carbon systems. The condensed Fukui function was calculated and HOMO–LUMO were visualised in order to study the sequence of hydroxylation of two isomers of C₈₂ fullerene for the low coverage regime, with the formula C₈₂(OH) _x where x?=?0???12. It was found that there was a formation of dangling bonds on structures with an odd number of hydroxyl groups on the fullerene surface, which suggests an enhanced reactivity of these molecules. Nevertheless, the coverings with an even number of groups tend to the reconstruction of π bonds, obtaining less reactive molecular structures. With the adsorption of the first group, a narrow HOMO–LUMO gap (1.28?eV) is observed in comparison with the C₈₂(OH)₂ system (1.70?eV), as is found in similar systems, such as C₆₀ fullerenol [E.E. Fileti et al., Nanotechnology 19, 365703 (2008); J.G. Rodríguez-Zavala and R.A. Guirado-López, Phys. Rev. B 69, 075411 (2004)]. Through an analysis of the electronic structure to these coverings, a splitting of electronic energy levels in the structure with one hydroxyl group is observed, which could be one of the factors that causes the narrowing of the energy gap in this structure. On the other hand, with a coverage of 12 hydroxyl groups, the formation of an amphiphilic molecule, where the location of groups in one side of the C₈₂ surface provides an hydrophilic character, is observed, while the uncovered part has an hydrophobic character. This could be important in the formation of Langmuir monolayers. Finally, it is shown that the precise distribution of the OH groups on the fullerene surface plays a crucial role in the electronic structure of the polyhydroxylated fullerenes.     

Small-angle neutron scattering in aqueous solutions of fullerene-containing oligopropylene oxides

Propylene-oxide oligomers in heavy water (their molecular mass is ～500, and the concentration C varies from ～0.6 to 5.0 g/dL) and similar systems with C₆₀ and C₇₀ fullerenes and C₆₀(OH) _x fullerenols (x ～ 20), i.e., functionalized oligopropylene oxides, are studied via small-angle neutron scattering. The initial oligomers are found to create spherical micelles (～40 molecules) in the solution. It is ascertained that, in oligopropylene-oxide solutions, the C₆₀, C₇₀, and C₆₀(OH) _x derivatives (～1 wt % of fullerene relative to the oligomer) modify its molecular organization, acting as physical bonds whereby micelles are joined into large-scale linear, twisted, and branched chain superstructures.     

The oxidation of fullerenes (C<Subscript>60</Subscript>, C<Subscript>70</Subscript>) with various oxidants under ultrasonication

The reaction of C₆₀, under ultrasonication, with various oxidants, such as 3-chloroperoxy benzoic acid (Fluka 99%), 4-methyl morpholine N-oxide (Aldrich 97%), chromium (VI) oxide (Aldrich 99.9%), and the oxone® monopersulfate compound, causes the oxidation of fullerenes at room temperature. The FAB-MS spectra and HPLC profile confirmed that the products of fullerene oxidation were [C₆₀(O)_n] (n=1～3 or n=1). C₇₀ also reacted, under ultrasonication, with various oxidants, but the reaction rate of C₇₀ was lower than that of C₆₀.     

Ab initio calculations of endo-and exohedral C60 fullerene complexes with Li+ ion and the endohedral C60 fullerene complex with Li2 dimer

The results of ab initio Hartree-Fock calculations of endo-and exohedral C₆₀ fullerene complexes with the Li⁺ ion and Li₂ dimer are presented. The coordination of the Li⁺ ion and the Li₂ dimer in the endohedral complexes and the coordination of Li⁺ ion in the exohedral complex of C₆₀ fullerene are determined by the geometry optimization using the 3–21G basis set. In the endohedral Li⁺C₆₀ complex, the Li⁺ ion is displaced from the center of the C₆₀ cage to the centers of carbon hexa-and pentagons by 0.12 nm. In the Li₂ dimer encapsulated inside the C₆₀ cage, the distance between the lithium atoms is 0.02 nm longer than that in the free molecule. The calculated total and partial one-electron densities of states of C₆₀ fullerene are in good agreement with the experimental photoelectron and X-ray emission spectra. Analysis of one-electron density of states of the endohedral Li⁺@C₆₀ complex indicates an ionic bonding between the Li atoms and the C₆₀ fullerene. In the Li⁺C₆₀ and Li⁺@C₆₀ complexes, there is a strong electrostatic interaction between the Li⁺ ion and the fullerene.     

Functionalization of pentagon–pentagon edges of fullerenes by cyclic polysulfides: A DFT study

We have performed a computational study to investigate the cyclosulfurization of the pentagon–pentagon (p–p) junctions in the non-IPR fullerenes C₆₀(D₃) and C₇₀(C_2v), and also Stone-Wales defective C₆₀ fullerene. Our results indicate the exothermic character of cyclosulfurization processes which can be related to the increase of pyramidalization angle (spherical excesses) and p characters of natural hybrid orbitals of C atoms at the p–p junctions. In fact these lead to the structural strain relief and stability of the cyclosulfurization derivatives of the non-IPR fullerenes. Moreover, the cyclosulfurization reaction of p–p bonds on the C₇₀(C_2v) is more energetically favorable than that of C₆₀(D₃), due to the higher curvature of carbon sites and the larger values of the p characters of natural hybrid orbitals in the C₇₀(C_2v). On the other hand, localization of the excess electrons on the C atoms at the p–p junctions leads to the low tendency of the charged non-IPR fullerenes to cyclosulfurization process. The desulfurization pathway of the exohedral derivatives of C₇₀(C_2v) indicates that it is energetically unfavorable for the functionalized fullerenes to break into individual fullerene and sulfur molecules. HOMO–LUMO gaps almost are independent of the number of pentathiepin rings while sensitive to the type of parent fullerene.     

Nanobionics of Pharmacologically Active Derivatives of Fullerene C60

The physical–chemical mechanisms of pharmacologic functioning of amino acid derivatives of fullerene C₆₀ (ADF) have been studied. ADF were shown to penetrate through the lipid bilayer of liposomes without destruction of membrane integrity. ADF are able to carry bivalent metal ions through phospholipid bilayer owing to the formation of complexes. It was shown that stereoisomers of ADF selectively penetrate into phospholipid membranes. In contrast to D-isomers, L-isomers penetrate through the phosphatidylcholine membrane into liposome interior. Stereo-specific effect of ADF enantiomers was also observed in reaction of peroxidation of lipids. Besides that, ADF bring about a substantial increase in the catalytic activity of monoaminoxidases A and B. The directed intraprotein electron transfer was studied by creating a donor–acceptor pair in a water solution in the presence of ADF. To realize the intraprotein electron transfer, the model system was produced on the base of apomyoglobin by incorporating ADF (electron acceptor) into the heme pocket of protein instead of removed heme. It was established that the fullerene C₆₀ and its derivatives did not produce specific anti-C₆₀ antibodies, both IgG and IgE classes, while ADF themselves are efficient adjuvants, i.e. they increased the antibody response to poor antigens. Some ADF were found to inhibit the human immunodeficiency virus and human cytomegalovirus infection.     

Stoichiometric synthesis of fullerene compounds with lithium and sodium and analysis of their IR and EPR spectra

A modified method is proposed for preparing fullerene compounds with alkali metals in a solution. The compounds synthesized have the general formula Me _n C₆₀(THF)_x, where Me = Li or Na; n=1–4, 6, 8, or 12; and THF = tetrahydrofuran. The use of preliminarily synthesized additives MeC₁₀H₈ makes it possible to prepare fullerene compounds with an exact stoichiometric ratio between C ₆₀ ^n? and Me ⁺. The IR and EPR spectra of the compounds prepared are analyzed and compared with the spectra of their analogs available in the literature. The intramolecular modes T _u (1)-T _u (4) for the C ₆₀ ^n? anion are assigned. The splitting of the T _u (1) mode into a doublet at room temperature for Me _n C₆₀(THF)_x (n=1, 2, 4) compounds indicates that the fullerene anion has a distorted structure. An increase in the intensity of the T _u (2) mode, a noticeable shift of the T _u (4) mode toward the long-wavelength range, and an anomalous increase in the intensity of the latter mode for the Li₃C₆₀(THF)_x complex suggest that, in the fullerene anion, the coupling of vibrational modes occurs through the charge-phonon mechanism. The measured EPR spectra of lithium-and sodium-containing fullerene compounds are characteristic of C ₆₀ ^? anions. The g factors for these compounds are almost identical and do not depend on temperature. The g factor for the C ₆₀ ^n? anion depends on the nature of the metal and differs from the g factor for the C ₆₀ ^? anion.     

C<Subscript>60</Subscript> fullerene as an η<Superscript>6</Superscript> ligand in π complexes of transition metals

The possible existence of complexes formed by the C₆₀ fullerene or its derivatives with transition metals interacting with the carbon cage via η⁶−π type bonding is discussed. The derivatives C₆₀ R ₆ of the C₆₀ fullerene (R = −, H, F, Cl, Br, CN) are analyzed using the density functional method within the Perdew-Burke-Ernzerhof approximation. In these molecules, the R groups are attached to carbon atoms located in the α positions with respect to the common hexagon of the C₆₀ fullerene. The structure and electron configuration of complexes formed by these molecules with Cr(C₆H₆), Cr(CO)₃, MoC₆H₆, and Mo(CO)₃ particles are modeled. The “dimer” systems C₆₀R₆-M-R ₆C₆₀ (M = Cr, Mo, R =-, H, F) are investigated in which two fullerene molecules interact via a transition-metal atom. It is found that the introduction of six R groups in the α sites with respect to the common hexagon of C₆₀ favors the formation of complexes of these derivatives of the C₆₀ fullerene with the Cr(C₆H₆), Cr(CO), Mo(C₆H₆), and Mo(CO)₃ particles in which η⁶-π type bonds arise between the metal and the atoms of the hexagon fringed with the R groups. It is also demonstrated that analogous complexes with a “bare” C₆₀ fullerene are possible, but they are significantly less stable. The (C₆H₆) M-R ₆C₆₀ R ₆-M (C₆H₆) complexes of particles M(C₆H₆) (M= Cr, Mo) and derivatives R ₆C₆₀ R ₆ (R =-, H, F, Cl, Br) are studied. In the R ₆C₆₀ R ₆ molecule, six R groups are located in the α sites with respect to the common hexagon of the C₆₀ fullerene and six other groups fringe the opposite hexagon. The obtained results can be applied to planning synthesis of new complexes that C₆₀ fullerene derivatives can form with transition metals. Original Russian Text ￠ E.G. Gal’pern, A.R. Sabirov, I.V. Stankevich, 2007, published in Fizika Tverdogo Tela, 2007, Vol. 49, No. 12, pp. 2220–2223.     

Negative ions of hydrogenated and deuterated C60 fullerenes

This paper reports on the results of mass spectrometric and theoretical investigations of hydrogenated and deuterated fullerene derivatives C₆₀H(D)_x. The formation and decay (through electron autodetachment) of negative molecular ions of the C₆₀H₁₈ and C₆₀D₁₈ hydrofullerenes are discussed. A comparative analysis of these processes is performed for different fullerene derivatives.     

内掺氮富勒烯N_2@C_(60)的几何结构和电子性质的密度泛函计算研究

采用密度泛函理论中的广义梯度近似对内掺氮富勒烯N2@C60的几何结构和电子性质进行计算研究.发现在N2@C60中,氮倾向以分子形式存在于C60中心处.键长分析、能级图、态密度图和电荷分析表明内掺氮分子对C60几何结构和电子结构带来的影响甚微.     

The compressive mechanical properties of Cn (n=20, 60, 80, 180) and endohedral M@C60 (M=Na,Al, Fe) fullerene molecules

The compressive mechanical properties of C_n (n = 20, 60, 80, 180) and endohedral M@C₆₀ (M = Na, Al, Fe) fullerene molecules are investigated using a quantum molecular dynamics (QMD) technique. Energy–strain curves, force–strain curves, endurance load, failure strain corresponding to the endurance load, and compressive stiffness of the fullerene molecules are obtained. The compressive mechanical properties of C₂₀, C₆₀, C₈₀, C₁₈₀ and M@C₆₀ (M = Na, Al, Fe) are discussed. The results show that the larger the magic number n of an empty fullerene, the higher its endurance load and compressive stiffness, but the lower its failure strain, and comparing to the empty C₆₀ fullerene, all the M@C60 molecules have greater endurance capability and failure strain.     

Electronic structure of graphite nanopipes

A recursion method is used for calculating the electron-state density n(E) of carbon in diamond, graphite, C₆₀ fullerene, and graphite nanopipes of various structures and diameters. The calculated n(E) for diamond, graphite, and fullerene are compared with experimental data. The distinctive features of the electron-state density n(E) in graphite nanopipes are discussed. Fiz. Tverd. Tela (St. Petersburg) 39, 1118–1121 (June 1997)     

密度泛函理论计算内掺氢分子富勒烯H2＠C60及其二聚体的几何结构和电子结构

采用密度泛函理论中的广义梯度近似(generalized gradient approximation,简称GGA),对内掺氢分子富勒烯H₂＠C₆₀及其二聚体的几何结构和电子结构进行了计算研究.发现无论是在H₂＠C₆₀单体,还是在其二聚体中,氢倾向以分子形式存在于碳笼中心处,且在室温下氢分子可以做自由旋转.电子结构分析表明,氢分子掺入到C₆₀和C₁₂₀中,仅对距离费米能级以下-8eV至-5eV能级处有一定的贡献,其他能级的分布和能隙几乎没有变化. 关键词： 几何结构 电子结构 密度泛函     

Amino-acid derivatives of fullerene C60 behave as lipophilic ions penetrating through biomembranes

It was found using potential-sensitive probes that the water-soluble amino-acid derivatives of fullerene C₆₀, such as C₆₀-Pro, C₆₀-? aminocapronic acid, and C₆₀-Arg, possess a pronounced membranotropic activity. The first two cause concentration-dependent dissipation of the membrane potential (Δψ) of the symbiosomes of the nodules of the yellow lupine generated in the presence of ATP and Mg²⁺ ions. In contrast to the first two derivatives, C₆₀-Arg, which carries a strong positive charge at the physiological pH, has no effect on the dissipation of Δψ in this model. On the contrary, this derivative caused a noticeable dissipation of the K⁺ diffusion potential (“minus” inside) generated on the membrane of human erythrocytes with the help of the K⁺ ionophore of valinomycin. The regularities obtained indicate that the derivatives of C₆₀ are transported across biological membranes as lipophil ions, thus causing depolarization of the membranes.     

Photopolymerization in the Fullerene Layers of the Molecular Donor–Acceptor Complex {Pt(nPr2dtc)2} · (C60)2

We measured Raman spectra in crystals of molecular donor–acceptor fullerene complexes {Me(nPr₂dtc)₂} · (C₆₀)₂ (Me = Ni, Cu, Pt). In the spectra of the {Pt(nPr₂dtc)₂} · (C₆₀)₂ complex under prolonged irradiation with a laser with λ = 532 nm, characteristic changes in the photopolymerization of fullerene are observed, associated with the splitting of degenerate phonon Hg modes and softening of Ag modes of the C₆₀ molecule. The kinetics of photopolymerization under conditions of weak irradiation at room temperature is studied. It was found that thermal destruction of the photopolymer with increasing temperature leads to a decrease in its concentration in the final photopolymerization product. The kinetics of thermal destruction is described by the Arrhenius equation, with the activation energy E_A of (0.68 ± 0.03) eV; the dimers are destructed to a concentration of 1% within 15 min at ~114°C.

     

Valence state of paramagnetic centers in fullerenes

Charge distribution on individual carbon atoms of a fullerene molecule C_n depends on the number of atoms it comprises,n. Only C₆₀ has the same charge on all its carbon atoms while other molecules containing fromn=32 ton=84 molecules are characterized by a variety of charge distributions. A neutral C₆₀ molecule is diamagnetic and does not show EPR signal. Charged C₆₀ ^v molecules, wherev is the valence taking values fromv=-6 tov=+1, show EPR signals for oddv and forv=2 when a fullerene molecule is in the triple state. EPR lines of isolated fullerene ions are narrow in the whole temperature range whereas EPR lines of Me_xC₆₀ ^v in ionic compounds Me_xC₆₀ are wide and their width decreases with temperature. A model of paramagnetic centers and an empirical formula relatingg-factor to valence have been given.