A theoretical investigation of the interaction between H,Li, Na,K, and fullerenes

We studied the interaction between H, Li, Na, and K with one and two C₆₀ molecules using unrestricted Hartree–Fock (UHF) methods. We investigated the effects of distances between the doping atoms and the C₆₀ clusters, total charges, interaction energies, stabilities, HOMO‐LUMO energy differences, charge distribution, and potential energy surfaces. The effect of each doping atom was analyzed and potential technological applications discussed. © 2004 Wiley Periodicals, Inc. Int J Quantum Chem, 2005     

Adsorption behavior of Co and C2H2 on the graphite basal surface: A quantum chemistry study

The adsorption of CO and C₂H₂ molecules on the perfect basal surface of graphite is investigated by adopting cluster models in conjunction with quantum chemical calculations. The noncovalent interaction potential energy curves for three different orientations of CO and C₂H₂ molecules with respect to the inert basal plane of graphite are calculated via semi-empirical and Möller-Plesset ab initio methods. Then, we have considered the effects of interaction energies on the C≡O and C≡C bond lengths by performing the partial geometry optimization procedure on the CO-graphite and C₂H₂-graphite systems in various intermolecular distances. The computational analysis of all physical noncovalent potential energy curves reveals that the relative configurations in which CO and C₂H₂ molecules approach the graphite sheet from out of the plane have stronger interaction energy and so is more favorable from the energetic viewpoint. This means that the graphite layer prefers to increase its thickness via the chemical vapor deposition of CO and C₂H₂ on the graphite.     

Interaction Between C60 Fullerene and Alkali Metals Demonstrating Superconductivity

A discret summation method [1] has been used to calculate the van der Waals dispersion interactions between an alkali metal atom and individual C₆₀ fullerene molecules, as well as between an intercalated alkali metal atom and the face-centred-cubic lattice of solid fullerite. It is known [2, 3] that the conductivities observed in the doped C₆₀ films vary considerably for different alkali atoms. Our interest was to investigate any correlation between these conductivities and the long range potential field behaviour. In the present study, we have obtained interaction potential curves of the C₆₀ fullerene molecule including within its cage, as well the potential field topography within the overall C₆₀ fullerite solid unit cell. We have found that for all intercalated alkali metals, except Cs, there are voids within the unit-cell of fullerite where the dopant experiences attractive interactions. Whereas on the other hand, inside the fullerene cage only Li and Na experience attractive forces. Importantly, it has been shown that the localization of the crystallographic sites [4] of doped alkali metals in fullerite coincide with the potential energy minima of long range van der Waals forces.     

On the laterally averaged interaction potential between He atoms and the (0001) surface of graphite

Very low energy scattering of He atoms from the (0001) face of graphite has been used to determine the bound state energies of the laterally averaged He-graphite potential. These results disagree with the existing literature, but agree with new measurements by Chung, Kara and Frankl. Their implications with respect to both the need for three-body terms in the interaction of an atom with a physisorbed overlayer, and the value of the long-range He-graphite C₃ coefficient, are discussed.     

Velocity dependence of vibrational branching ratios in electronic energy transfer collisions of metastable argon atoms with nitrogen

Measurements have been made of the vibrational branching ratio (υ′=0)/(υ′=1) in N^*₂ (C³Π_u) formed in electronic energy transfer collisions between argon metastable atoms and ground state nitrogen molecules, using crossed molecular beams. In the relative collision energy range, 0.08–0.20 eV, this ratio is 3.5±0.2.     

Formation of M+ ions and electronic excitation under fast-atom bombardment conditions by using a liquid matrix

Japan The mechanism for the formation of molecular ions M^+· under fast-atom bombardment (FAB) conditions with a liquid matrix is discussed on the basis of the mass spectra of pyrene, coronene, and fullerene C₆₀ obtained by using electron impact, gas-phase fast-atom bombardment, and gas-phase fast-molecule bombardment techniques. The obtained results suggest that formation of the M^+· ions under FAB conditions is not due to direct collisions between analytes M and fast atoms A, but is due to collision interactions between M and recoiling matrix molecules B or matrix ions. It has been confirmed, furthermore, that the FAB conditions with a liquid matrix are sufficient in energy for formation of singly charged ions M^+· and insufficient for the formation of multiply charged ions M ^z+ (z=2, 3) of pyrene, coronene, and C₆₀.     

X-ray spectroscopic study of graphite fluoride (C2F) n intercalated with benzene

Samples of intercalated graphite fluoride of the C₂F·zR type (R is C₆H₆) before and after heating to 150 °C in a spectrometer vacuum chamber were studied by X-ray fluorescence spectroscopy. The C-Kα differential spectra of the samples mainly characterizes the electron state of carbon atoms in the benzene molecule inside the C₂F matrix. The differential spectrum is distinct from the spectrum of solid benzene by additional maxima, which indicate the interaction between the benzene molecules and the graphite fluoride matrix. Comparative analysis of the spectrum of the heated sample and those of graphite and graphite fluoride (CF) _n suggests that the layers of the C₂F matrix contain considerable regions of both completely fluorinated and graphite-like regions. Translated fromIzvestiya Akademii Nauk. Seriya Khimicheskaya, No. 4, pp. 705–708, April, 2000.     

Positron annihilation in C60 and K6C60

The positron density distributions in C₆₀ and K₆C₆₀ have been evaluated using the positron lifetime and Doppler-broadening spectroscopy for the annihilation radiation.In C₆₀, positrons are distributed in the interstitial sites between the C₆₀ molecules,which has been demonstrated by measurements of the temperature dependence of the Doppler-broadening of the annihilation radiation. On the other hand, the positron density distribution must be greatly changed in K₆C₆₀, because positrons are repelled by Coulomb interactions by the positively charged K atoms. It has been observed that there is an extremely short lifetime and a small Doppler-broadening component for the positron annihilation in K₆C₆₀. This component is considered to reflect the positron annihilation inside a C₆₀ molecule.     

Reactive scattering of a neon seeded oxygen atom beam

A high pressure microwave discharge source operating with a dilute mixture of O₂ in Ne has been used to produce a supersonic nozzle beam of O atoms seeded in Ne. This low energy supersonic O atom beam has been used to study the reactive scattering of O atoms with Cl₂ and CS₂ molecules at an initial translational energy E = 13 kJ mol^?1. The results are compared with rective scattering from the same reactions using a high energy O atom beam formed by seeding O atoms in He. The O + Cl₂ reaction proceeds via a short-lived collision complex where the lifetime of the collision complex depends upon the initial translational energy. However the O + CS₂ reaction follows a stripping mechanism which is unaffected by initial translational energy.     

The solid state 13C-NMR spectra of some intercalation compounds

The ¹³C-nuclear magnetic resonance spectra of graphite bromine (C₈Br) and two graphite potassium compounds (C₈K and C₂₄K) have been obtained in the solid state. A similar spectrum is observed for all three compounds. The major feature in all three compounds is a very broad upfield resonance. These spectra are interpreted as indicative of an interaction of the intercalate with the graphite π system leading to more aliphatic-like carbon atoms.     

A First‐Principles Study of Lithium Adsorption on a Graphene–Fullerene Nanohybrid System

The mechanism of Li adsorption on a graphene–fullerene (graphene–C₆₀) hybrid system has been investigated using density functional theory (DFT). The adsorption energy for Li atoms on the graphene–C₆₀ hybrid system (?2.285 eV) is found to be higher than that on bare graphene (?1.375 eV), indicating that the Li adsorption on the former system is more stable than on the latter. This is attributed to the high affinity of Li atoms to C₆₀ and the charge redistribution that occurs after graphene is mixed with C₆₀. The electronic properties of the graphene–C₆₀ system such as band structure, density of states, and charge distribution have been characterized as a function of the number of Li atoms adsorbed in comparison to those of the pure graphene and C₆₀. Li adsorption is found to preferentially occur on the C₆₀ side due to the high adsorption energy of Li on C₆₀, which imparts a metallic character to the C₆₀ in the graphene–C₆₀ hybrid system.     

Energy transfer in classical collinear and perpendicular central collisions of a structureless atom with a morse oscillator

The energy transfer in classical collinear (C_∞) and perpendicular (C_2v) central collisions of an atom with a Morse oscillator is compared. These collision geometries contribute in classical collisions to experimentally observed inelastic backward scattering of alkali ions from H₂ molecules. For both collision geometries the equations of motion reduce to a set of only two coupled differential equations which can be easily solved numerically. The calculations show that the C_2v collisions are much more effective than C_∞ collisions at all but the very lowest energies. The calculated ΔE/E versus E curves for C_2v collisions using a Born-Mayer potential for the atom atom-in-molecule interaction could be fitted to the experimental results for Na⁺-D₂ yielding reasonable potential values.     

He capture by negatively charged Buckminsterfullerene

The first observation of capture of He atoms by negatively charged Buckminsterfullerence (C₆₀) is reported. The collision energy dependence of the production of the endohedral complex is presented in the region of the energetic threshold and compared directly with results obtained using positively charged C₆₀. The threshold for capture by negative ions is shifted by ≈ 1.5 eV to higher energies. This shift can be accounted for by considering the different internal energies of the positive and negative ions.     

Modified statistical theory of energy transfer in ion-molecule collisions

The modified statistical theory developed previously for potentials appropriate to interactions in neutral-neutral collisions, is now extended to more strongly attractive potentials involved in ion-neutral collisions. The model system is the collisional deactivation of C₅H₉⁺ by a variety of both polar and non-polar neutral molecules. A 12 - 6 - 4 potential is used for ion interaction with non-polar neutrals, and a 12 - 6 - 4 - 2 potential, as modified by Su and Bowers to take into account the rotational energy of the neutral, for interaction with polar neutrals. Calculated is (ΔE), the average energy lost by the ion in a collision, and compared with experiment. For C₅H₉⁺-CH₄ collisions, the calculated (ΔE) agrees with experiment within 5%. Predictions of the theory, namely that (ΔE) should increase with excitation energy and should decrease with the size of the excited reactant, are found to be in fair agreement with the somewhat ambiguous experimental evidence.     

Assessing a double silicon decorated fullerene for the delivery of interacting flurbiprofen and salicylic acid drugs: A DFT approach

Since the number of drugs increases constantly, drug interactions appear as a critical issue to handle. The effective use of multiple drugs appears as another important subject to discuss and the use of targeted and selective delivery of drugs is becoming more important. Impurity doped C₆₀ fullerenes with various dopant atoms such as silicon or boron appear as promising drug delivery vehicles. Therefore, in the framework of this study, we investigated the interaction between salicylic acid and flurbiprofen and their controlled delivery by using double silicon decorated C₆₀ fullerene using density functional theory. Stability and reactivity considerations were also examined by investigating some important structural parameters, interaction energies and frontier molecular orbitals. The interactions were also monitored by examining important diagnostic vibrational bands. The strength of the interactions between atoms at the interaction sites was also identified by using the quantum theory of atoms in molecules.     

Ab-initio molecular dynamics simulation of monolayer C60 thin film on silicon (100) surface

Two dimensional band structure is calculated for a triangular lattice of C₆₀ molecules by using a mixed-basis approach in which wave functions are expanded with not only plane waves but also 1s and 2p atomic orbitals of carbon atoms. The present analysis modeling a charge transfer from Si dimers of the Si (100) surface suggests the existence of a small Fermi-surface. The resulting partial charge distribution is consistent with the recent STM observation of specific stripes, the direction of which is parallel to that of the topmost double bond of C₆₀, regardless of the intermolecular interaction. It is concluded that the orientation of C₆₀ on the Si surface is mainly determined by the direction of dimer arrays and not by the interaction between C₆₀ molecules.ACKNOWLEDGEMENT The authors are very grateful to the Institute for Supercomputing Research of RECRUIT Co. for the use of the NEC SX-2 supercomputer. Authors also thank IBM Japan and Japan IMSL Inc. for supporting them a good computer environment.     

Interaction between methyl and hydroxyl radicals: a theoretical study

In this paper, we conduct a computational quantum mechanic study of two molecules interaction between methyl (·CH₃) and hydroxyl (·OH) radicals. The molecular exploration has been focused on the possibility of finding non-bonding interactions (formation of complexes by weak-bond interaction among C–O–H atoms) and the potential energy reaction between those two molecules. It shows that the formed complexes presents in slightly lower potential energy than that of the reactants and/or products. The existence of these complexes could proceed to the further interaction, e.g. reaction of the molecules, as those complexes formed a particular configuration.     

Exohedral functionalization of C60 by [4+2] cycloaddition of multiple anthracenes

By using density functional theory, we have investigated [4+2] cycloaddition of one to four anthracene (ANT) molecules to a C₆₀ fullerene which has been already studied by experimentalists. It was found that the reaction is regioselective and the ANT molecule prefers to be adsorbed atop a C–C bond of the C₆₀ which is shared between two hexagons with reaction energy of ?25.2 kcal/mol (for one ANT). The HOMO of the ANT interacts with the LUMO of the C₆₀ via a cycloaddition reaction. Also five regioisomeric bis-adducts of ANT/C₆₀ complexes were compared from stand point of stability. Increasing the number of attached ANTs, the reaction energy becomes less negative. The HOMO–LUMO energy gap of C₆₀ is slightly changed and the potential barrier of the field electron emission from its surface may be reduced upon the reaction.