Electronic properties of charged fullerenes characterized by EPR and Vis-NIR spectroscopy

EPR and Vis-NIR absorption spectra have both been measured for clarification of contradictory statements about the para-and diamagnetic states of fullerenes. Thereby identification of one sharp EPR signal in solution at room temperature to C ₆₀ ^? (g=2.000±4.0001; ΔB=0.07±0.01 mT) could be made upon using different fullerene sources (TechnoCarbo, Hoechst) and methods of anion generation (chemically, electrochemically, and photochemically). This fact is also supported by the similar observation for a monosubstituted derivative (g=1.9999; ΔB=0.10 mT), in which a small broadening of this sharp signal is found originating from additional¹H hyperfine interactions. Furthermore theg-values of the radical anions of C₆₀ increase with charge (g(C ₆₀ ^? <g(C ₆₀ ^2? ) < <g(C ₆₀ ^3? ) <g(C ₆₀ ^5? )) indicating largest contributions from spin-orbit coupling for the monoanion. No diamagnetic states for the dianions of [60]- and [70]- fullerenes could be found so far but biradical species with largest zero field splittingsD=2.7 mT (C ₆₀ ^2? ), andD=3.1 mT (C ₇₀ ^2? ), respectively. The cation formation of C₆₀ (g=2.0023-2.0029; ΔB=0.15-0.20 mT) with antimony pentachloride was controlled by mass spectrometry. Stable cations were found only in methylenechloride. In other solvents like toluene addition reactions seem to occur.     

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.     

Simultaneous electrochemical and electron paramagnetic resonance studies of fullerene anion radicals C 60 1− and C 60 3−

Simultaneous electrochemical and electron paramagnetic resonance experiments have been carried out on the reduced C₆₀ fullerene to examine theg-factor assignment of the radical species. C ₆₀ ^1? and C ₆₀ ^3? show the following EPR characteristics at room temperature: C ₆₀ ^1? :g _1?=2.0002±0.0001, 2ΔB _1s=0.17 mT, and C ₆₀ ^3? :g _{3?=2.0008±0.0002}, 2ΔB _1s=0.07 mT. EPR linewidths are apparently narrower compared to those in most of the spectra previously reported. Variable temperature EPR study on solution containing C ₆₀ ^1? has shown thatg _1? value is not while the linewidth is only slightly temperature dependent.     

A solid-state (CP-MAS)13C nuclear magnetic resonance study of selected photo(thermo)chromic spiro-(indolinonaphthoxazine)s

Liquid and solid-state¹³C NMR data are reported for three photo(thermo)chromic spiro-(indolinonaphthoxazine)s,1–3. The isotropic¹³C chemical shifts are almost identical in the solid state and in solution. Therefore, the structures in the solid state are fully retained in solution. Quantitative analysis of the spinning side-band pattern of¹³C CP-MAS NMR spectra gave shielding anisotropies and asymmetry parameters different for1–3 and related to the substitution pattern. For3 the tensor componentσ ₃₃, assumed to be perpendicular to the aromatic ring, is more shielded than the corresponding components of1 and2 probably because of the near orthogonality between the substituent piperidinyl ring and the naphthoxazinic system. A correlation between shielding anisotropy and thermochromic activity is suggested.     

EPR of a fullerene-molecule-derived paramagnetic center as a mesoscopic conducting object

Discussion of theg-factor value of fullerene is based on the model of itinerant electrons restricted to the surface of the fullerene molecule C₆₀. The Ag shift, i.e., the difference between the experimentalg-factor and theg-factor of free electron Δg = g ? 2.0023 for C ₆₀ ^?1 is negative as for a very small metallic conducting particle.g-factor value is proportional to the interaction between itinerant electrons in the conduction band, thus the Δg is negative for C ₆₀ ^?1 and C ₆₀ ^?3 having less than half filled conduction band, while Δg is positive for C ₆₀ ⁺ where the conduction band is almost filled.     

Mono and bidimensional1H NMR and inverse detected13C NMR of the duplex d(CA)3·d(TG)3

The unambiguous assignment of the aromatic protons of the duplex d(CA)₃·d(TG)₃ was carried out with the aid of HMQC and HMBC inverse detected¹³C NMR experiments atT=278 K. The NOE connections of these protons with the imino protons of the complementary bases — established by 2D NOESY experiments — indicated that the duplex is characterized by a canonical Watson-Crick basepairing pattern. Monodimensional¹H NMR experiments, also carried out atT=278K, in the presence of varying amounts of NaCl and with water suppression by presaturation and by spin echo techniques, showed that the imino protons of the TA and CG pairs of the duplex exchange with water through a process of local base pair opening and with different exchange rates.     

Electron spin echo at S-band: Nuclear modulations and decay in C60 powder

At S-band (≈ 3 GHz) the modulation amplitude of the Electron Spin Echo patterns is increased with respect to the amplitude at X-band: as a consequence, it is possible to reveal the presence of nuclei not detectable at X-band. In this paper the results obtained by running ESE experiments at S-band on a C₆₀ powder sample containing radicals are shown and discussed. The two- and three-pulse Electron Spin Echo patterns exhibit both¹³C modulation and proton modulation not detected at X-band. The experimental data are quantitatively analyzed by simulating the time-domain patterns and their Fourier transforms. It results that a noticeable amount of proton nuclei surrounds the intrinsic paramagnetic centers. On the basis of the analysis, a possible explanation of their existence is given.     

31P NMR studies on the interaction of morpholinyl anthracyclines and related compounds with d(CGTACG)2. Thermodynamic and kinetic parameters

³¹P NMR spectroscopy has been used to study the intercalation of the anthracyclines doxorubicin1, daunorubicin2, 4-demethoxydaunorubicin3, morpholinodoxorubicin4, methoxymorpholinodoxorubicin5 and 9-deoxydaunorubicin6 with the DNA fragment d(CGTACG)₂. The individual phosphate resonances of the oligonucleotide were assigned in the free as well as in the intercalated species. The³¹P chemical shift variations allowed us to identify the intercalation sites, which resulted to be the same for all compoundsi.e. between the terminal CG base-pairs of the helix (two molecules of drugper duplex). The binding constants, the dissociation rate constants and ΔG ^# values have been determined in different conditions of ionic strength and temperature. The kinetic constant (k _off) of the slow step of the anthracycline/duplex intercalation process has been directly measured by NOE exchange techniques. Binding constants depend on the ionic strength and on the self-association process so greatly, that their use to study by NMR anthracycline/DNA interactions is questionable. On the contrary, thek _off are not affected by these phenomena and present an interesting trend for1–6, thus showing that the average lifetime of the drug in the intercalation site appears to be important for determining the cytotoxicity and the antimitotic activity.     

Inosine — Adenosine base pairing in d-GGTACIAGTACC: Duplex and hairpin with a two-base loop

An oligonucleotide dodecamer d-GGTACIAGTACC containing two inosine-adenosine mismatched base-pairs has been studied by¹H and³¹P NMR spectroscopy. Unique assignments of¹H and³¹P spins have been achieved by using a recently proposed two-dimensionalheteronuclearlong rangecorrelation (2D-HELCO) technique. The 2D nuclear Overhauser enhancement spectroscopy (NOESY) spectrum recorded in a mixed solvent of 90% H₂O+10%²H₂O has been used to assign all the exchangeable imino and amino proton resonances. NMR results indicate that at concentrations above 5 mM, the molecule adopts a duplex structure where the inosine imino protons are hydrogen bonded. Cross-strand NOEs between the imino proton of I6 and H2 proton of A7 and that between H2 of I6 and H2 of A7 provide evidence for inosine-adenosine base-pairing, with both bases I6 and A7 inanti conformation. The observed NOE connectivitiesd1,d2 andd3 from almost the middle of the molecule to the two ends are consistent with a right handed B-DNA conformation. However, the molecule adopts a more extended conformation in the mismatch region to accomodate the bulky purine-purine (IA) base pairs. NMR experiments at lower concentrations indicate the coexistence of a monomeric hairpin with a two base loop, consisting of I6 and A7 units, in equilibrium with the duplex. 2D-ROESY experiment at such a concentration shows that the conformation of the stem of the hairpin does not deviate much from the corresponding region of the duplex and four nucleotides C5, I6, A7 and G8 undergo significant structural changes during the formation of hairpin loop.     

A program for simulation of powder-type EPR spectra

An algorithm of a computer program for simulation of powder type EPR spectra (S=1/2,I≠0) is described. For determination of the energy levels, the perturbation approach is used and corrections up to second order due to hyperfine, quadrupole, and nuclear Zeeman coupling are taken into account. No restrictions on the mutual orientations of the eigenvectors ofg, hyperfine, and quadrupole tensors are imposed. Simulated spectra for a model paramagnetic system (S=1/2,I=3/2) with axial symmetry and noncoinciding directions ofg _‖ andA _‖ are presented.     

Studies of the iron-sulphur centers of the bacteriaShewanella putrefaciens (MR-1)

Shewanella putrefaciens (MR-1) can be grown using any one of several different terminal acceptors. This respiratory versatility stimulated our studies of the respiratory chain of MR-1 using whole cell analysis by ESR spectroscopy. Initial analyses of aerobically grown cells showed the presence of the succinate dehydrogenase complex. Also, it was shown that inS. putrefaciens which were grown anaerobically with iron as the only electron acceptor the ESR signal atg=2.021 appeared at low temperatures. This ESR signal resembled the ESR signal of [Fe-S] center of succinate dehydrogenase in oxidized state. However this new ESR signal had a different temperature dependence. It can be seen at temperature as high as 40 K. The line shape andg-factor of the new center are very similar to those of [3Fe-4S] centers. As this ESR signal can be seen only in the anaerobic samples grown with iron as acceptor we suggest that this center is located in the terminal part of the respiratory chain and is associated with the reduction of iron or another electron acceptor.     

Temperature dependence of theg=6 EPR linewidth in high spin FeIII myoglobin samples

The temperature dependence of theg=6 line of high spin FeIII aqueous mixed water-glycerol myoglobin samples has been investigated by EPR spectroscopy. The trend with the temperature of the linewidth has been analyzed by taking into account both a temperature-independent contribution from the frozen structural heterogeneity (conformational substate distribution) and the relaxation processes. The temperature-dependent line broadening process due to the spin-lattice relaxation has been singled out by simulation of the experimental data and put into relationship to the density of the vibrational states. The effect on the vibrational modes of the protein-solvent system, as induced by the addition of large amount of the glass-making solvent, glycerol, is discussed.     

ESR study of Cu(II)-indomethacin and its pyridine and DMF adducts

Powder ESR spectra of [Cu₂(Ind)₄](H₂O)₂ at room temperature show the presence of copper acetate like dimers characterized by a strong antiferromagnetic exchange interaction (J≈?338 cm^?1). Two different monomeric species were evidenced in 40%Py+60%DMF solution absorbed on NaY zeolite: the Cu(Ind)₂(DMF)₂ with an elongated tetragonal-octahedral symmetry and the Cu(Ind)₂(Py)₂ with a CuN₂O₂ chromophore in atrans square-planar arrangement. Only one monomeric species Cu(Ind)₂(Py)₂ was identified in 20%Py+80%DMF and 20%Py+80% Chloroform solutions. The Cu(Py)₄ ²⁺ species of CuN₄ chromophore occurs in pyridine Cu(II)-indomethacin solution suggesting a decomposition of the solvit compound.     

Characterisation of the Ru/MgF2 catalyst with adsorbed O2, NO, CO probe molecules by EPR and IR spectroscopy

Electron paramagnetic resonance (EPR) and infrared (IR) spectroscopy were used to study the formation of ruthenium and adsorbed species appearing on the catalyst during O₂, NO, and CO adsorption at room temperature on 1 wt% Ru/MgF₂ catalysts prepared from Ru₃(CO)₁₂ . Both EPR and IR results provided clear evidence for the interaction between surface ruthenium and probe molecules. No EPR signals due to ruthenium (Ru) species were recorded at 300 and 77 K after H₂-reduction of the catalyst at 673 K. However, at 4.2 K a very weak EPR spectrum due to low-spin (4d⁵) Ru³⁺ complexes was detected. A weak anisotropic O₂^- radicals signal with g_∣∣=2.017 and g_⊥=2.003 superimposed on a broad (ΔB_pp=120 mT), slightly asymmetric line at g=2.45(1) was identified after O₂ admission to the reduced sample. Adsorption of NO gives only a broad, Gaussian-shaped EPR line at g=2.43(1) indicating that the admission of NO, similarly to O₂ adsorption, brings about an oxidation of Ru species in the course of the NO decomposition reaction. Introduction of NO over the CO preadsorbed catalyst leads to EPR spectrum with parameters g_⊥=1.996, g_∣∣=1.895, and A_⊥^N=2.9 mT assigned to surface NO species associated with Ru ions. The IR spectra recorded after adsorption of NO or CO probe molecules showed the bands in the range of frequency characteristic of ruthenium nitrosyl, nitro, and nitrate/nitrite species and the bands characteristic of ruthenium mono-and multicarbonyls, respectively. Addition of CO after NO admission to the catalyst leads to appearance in the IR spectrum, beside the ones characteristic of NO adsorption, the bands which can be attributed to Ru-CO₂ and Ru-NCO species, indicating that the reaction between NO and CO occurs. These species were also detected after CO adsorption followed by NO adsorption, additionally to the band at 1850 cm⁻¹ being due to cis-type species.     

Sonochemical synthesis of novel C60 fullerene 1,4-oxathiane derivative through the intermediate fullerene radical anion

We have discovered a selective and efficient method for the synthesis of previously unknown 1,9-(1′,4′-oxathiano)-1,9-dihydro-(C₆₀-I_h)[5,6]fullerene, a compound with the direct attachment of the sulfur atom to the fullerene core. The method is based on the reaction of C₆₀ with 1,2-hydroxythiols in the presence of inorganic bases in air under ultrasonication. The significance of ultrasound has been exemplified with the comparative conventional methods. The title compound has been identified with mass-(MALDI TOF/TOF), one- and two-dimensional NMR ¹H and ¹³C (COSY, HSQC, HMBS), IR, UV–Vis spectroscopic techniques. Using the direct EPR method, we have detected radical anion C₆₀^– (g = 2.0046 and ΔH = 2 G) as a key reaction intermediate of the sonochemical reaction. Based on the experimental results and quantum chemical calculations, we have proposed a mechanism for the conversion of C₆₀ and 2-mercaptoethanol to the C₆₀–1,4-oxathiane adduct.     

Observation of three sites for vanadyl in a biomineral, zinc sodium phosphate hexahydrate: an EPR investigation

Single crystal EPR study has been carried at room temperature for VO(II) doped zinc sodium phosphate hexahydrate. Single crystal rotations in each of the three mutually orthogonal crystallographic planes namely bc, ac, and ab indicate three chemically inequivalent sites, with intensity ratios of 25:13:1. The spin Hamiltonian parameters obtained for the two intense sites are: Site I: g_xx=1.983, g_yy=1.985, g_zz=1.933; A_xx=7.39 mT, A_yy=7.15 mT, A_zz=19.03 mT; Site. II: g_xx=1.985, g_yy=1.985, g_zz=1.937; A_xx=7.36 mT, A_yy=7.25 mT, A_zz=18.67 mT. The two VO bond directions in the two sites are approximately at right angles to each other. The powder spectrum clearly indicates two chemically inequivalent sites, confirming the single crystal analysis. Admixture coefficients, Fermi contact, and dipolar interaction terms have also been evaluated.     

Temperature dependence of the electronic spin relaxation of DCNQI salts

For the elucidation of the charge and spin dynamics of the radical anion salts of DCNQI with metallic counterions we have performed cw- and pulsed ESR experiments (βB _pp,T _1e ^?1 andT _2e ^?1 ) between 300 and 4 K at nine salts differing in counterions and sidegroups, respectively. We can explain the relaxation rates by dipolar electron-electron interaction and spin-orbit contribution. In the high temperature range we have a gradual decrease in the number of charge carriers by interband transitions without a slowing down of the mobility. With complete localization of the electron spins (no mobile electrons anymore) exchange interaction governs the spectral density, becoming strongly temperature dependent due to effective spin exchangeJ _eff(T), explained by an extended REHAC-model. This effective spin exchangeJ _eff(T) includes for the first time a contribution by the metallic counterions. For spin-orbit interaction we developed a model based on F. Adrian [1] not depending on the mixture of Bloch and spin states as given by Elliott [2]. This is achieved by the inclusion of the electronic probability on atoms with higher atomic numbers, modulated by phonons. This model explains the drastic changes in the ESR linewidth of different radical ion salts of DCNQI and allows inductively the prediction of the electronic properties of new radical ion systems of which just the molecular and crystal structure is known.     

New band system of YbI molecule

Thermal emission spectrum of YbI molecule has been photographed for the first time in the spectral regionλλ 6100–6400 Å using Saha’s high temperature furnace at a reciprocal linear dispersion of 7.3 Å/mm. A total of 52 single-headed and violet degraded bands have been recorded and are classified into a single system. Vibrational analysis has been carried out and it has been suggested that system arises from the ground state with the vibrational constantω″ _e=153.0 cm^?1.     

Very high frequency EPR — 94 GHz instrument and applications to primary reaction centers from photosynthetic red bacteria and to other disordered systems

There are many advantages to carrying out electron paramagnetic resonance experiments at very high frequencies, either as part of a multifrequency strategy for solving problems or for special characteristics of high frequencies. These special characteristics include the potential for high point sensitivity, enhanced resolution, separation of similar species, altered sensitivity to motion, suppression of motional effects, and many others. This paper describes a three-millimeter-wavelength (W-band, 94 GHz) EPR spectrometer built for a multi-user facility and illustrates with some examples, most of them being disordered systems. One significant example is the oxidized primary reaction center, P ₈₆₅ ⁺ , isolated from the red photosynthetic bacteriaRhodobacter Sphaeroides R-26. The W-band technique applied to both centers isolated from bacteria grown from either deuterated or ordinary growth media allows extraction of the fullg anisotropy in these centers and sets the stage for multifrequency EPR spectroscopy to yield a full analysis of the various contributions to linewidths in these systems.