NH3 on a BC3 nanotube: effect of doping and decoration of aluminum

The adsorption of the NH₃ molecule was investigated on pristine, Al-doped and Al-decorated BC₃ nanotubes (BC₃NT) using density functional theory calculations. It was found that NH₃ prefers to be adsorbed on a B atom of the tube wall, releasing energy of 1.02 eV. Al-doping increases the acidity of the tube surface and, therefore, its reactivity toward NH₃ so that the released energy in this case is about 1.62 eV, while decorating the BC₃NT with Al atom decreases the acidity and reactivity. Although Al-doping has no significant effect on the electronic properties of the BC₃NT, Al-decoration significantly reduces its HOMO/LUMO energy gap from 2.37 to 1.16 eV so that the tube becomes an n-type semiconductor. However, we believe that the acidity of the BC₃NTs may be controlled by doping or decoration of Al atoms.     

A DFT study on the sensing behavior of a BC2N nanotube toward formaldehyde

We investigated the viability of using a BC₂N nanotube to detect formaldehyde (H₂CO) molecule by means of B3LYP and M06 density functionals. The results indicate that the molecule is weakly adsorbed on the intrinsic BC₂N nanotube releasing energy of 0.8 kcal mol^-1 (at B3LYP/6-31G(d)) without significant effect on the HOMO-LUMO energy gap and electrical conductivity of the tube. Thus, H₂CO cannot be detected using this intrinsic nanotube. To overcome this problem, a carbon atom of the tube wall was substituted by a Si atom. It was demonstrated that the Si-doped tube cannot only strongly adsorb the H₂CO molecule, but also may effectively detect its presence because of the increase in the electric conductivity of the tube.     

Density functional study of H<Subscript>2</Subscript>O molecule adsorption on α-U(001) surface

Periodic density functional theory (DFT) calculations were performed to investigate the adsorption of H₂O on U(001) surface. The metallic nature of uranium atom and different adsorption sites of U(001) surface play key roles in the H₂O molecular dissociate reaction. The long-bridge site is the most favorable site of H₂O-U(001) adsorption configuration. The triangle-center site of the H atom is the most favorable site of HOH-U(001) adsorption configuration. The interaction between H₂O and U surface is more evident on the first layer than that on any other two sub-layers. The dissociation energy of one hydrogen atom from H₂O is ?1.994 to ?2.215 eV on U(001) surface, while the dissociating energy decreases to ?3.351 to ?3.394 eV with two hydrogen atoms dissociating from H₂O. These phenomena also indicate that the O_ads can promote the dehydrogenation of H₂O. A significant charge transfer from the first layer of the uranium surface to the H and O atoms is also found to occur, making the bonding partly ionic.     

Theoretical study on the functionalization of BC2N nanotube with amino groups

Using density functional theory calculations, we investigated properties of a functionalized BC₂N nanotube with NH₃ and five other NH₂-X molecules in which one of the hydrogen atoms of NH₃ is substituted by X = ?CH₃, ?CH₂CH₃, ?COOH, ?CH₂COOH and ?CH₂CN functional groups. It was found that NH₃ can be preferentially adsorbed on top of the boron atom, with adsorption energy of ?12.0 kcal mol^?1. The trend of adsorption-energy change can be correlated with the trend of relative electron-withdrawing or -donating capability of the functional groups. The adsorption energies are calculated to be in the range of ?1.8 to ?14.2 kcal mol^?1, and their relative magnitude order is found as follows: H₂N(CH₂CH₃) > H₂N(CH₃) > NH₃ > H₂N(CH₂COOH) > H₂N(CH₂CN) > H₂N(COOH). Overall, the functionalization of BC₂N nanotube with the amino groups results in little change in its electronic properties. The preservation of electronic properties of BC₂N coupled with the enhancement of solubility renders their chemical modification with either NH₃ or amino functional groups to be a way for the purification of BC₂N nanotubes.     

Density functional studies of the stepwise substitution of pyridine,pyridazine, pyrimidine,pyrazine, and 1,3,5-triazine with BCO

Ozone (O₃) adsorption on pristine Stone–Wales (SW) defective BC₃ graphene-like sheets was investigated using density functional calculations. It was found that O₃ is weakly adsorbed on the pristine sheet. Two types of SW-defective sheets were studied, SW-CC and SW-BC, in which a defect is formed by rotating a C–C or B–N bond, respectively. O₃ molecules were found to be more reactive on SW-BC defective sheets. It was predicted that O₃ molecules are reduced to O₂ molecules on SW-BC sheets, overcoming an energy barrier of 34.2 kcal/mol^?1 at the B3LYP level of theory and 27.2 kcal/mol^?1 at the BP98 level of theory. Therefore, SW-BC sheets could potentially be employed as a metal-free catalyst for O₃ reduction. The HOMO–LUMO gap of a SW-BC sheet decreases from 2.16 to 1.21 eV after O₃ dissociation on its surface in the most stable state.     

Tuning hydrogen storage of carbon nanotubes by mechanical bending: theoretical study

The effects of mechanical bending on tuning the hydrogen storage of titanium functionalised (4,0) carbon nanotube have been assessed using density functional theory calculations with reference to the ultimate targets of the US Department of Energy (DOE). The assessment has been carried out in terms of physisorption, gravimetric capacity, projected densities of states, statistical thermodynamic stability and reaction kinetics. The Ti atom binds at the hollow site of the hexagonal ring. The average adsorption energies (?0.54 eV) per hydrogen molecule meet the DOE target for physisorption (?0.20 to ?0.60 eV). The curvature attributed to the bending angle has no effect on the average adsorption energies per H₂ molecule. With no metal clustering, the system gravimetric capacities are expected to be as large as 9.0 wt%. The reactions of the deformed (bent) carbon nanotube have higher probabilities of occurring than those of the un-deformed carbon nanotube. The Gibbs free energies, enthalpies and entropies meet the ultimate targets of the DOE for all temperatures and pressures. The closest reactions to zero free energy occur at (378.15 K/2.961 atm.) and reverse at (340 and 360 K/1 atm.). The translational component is found to exact a dominant effect on the total entropy change with temperature. Favourable kinetics of the reactions at the temperatures targeted by DOE are reported regardless of the applied pressure. The more preferable thermodynamic properties assigned to the bending nanotube imply that hydrogen storage can be improved compared to the nonbending nanotube.     

Oxygen doped SiC nanocrystals: first principles study of the optical properties

We have studied a typical spherical SiC nanocrystal with a diameter of 1.2 nm (Si₄₃C₄₄H₇₆) using linear combination of atomic orbitals in combination with pesudopotential density functional calculation. The role of fluorine and oxygen impurities was investigated on the electronic and optical properties of the Si₄₃C₄₄H₇₆ nanocrystal. Total energy calculations show that the fluorine doped Si₄₃C₄₄H₇₆ nanocrystals are unstable. Oxygen doped Si₄₃C₄₄H₇₆ have different binding energies in various substitutional and interstitial defects. The maximum binding energy of the oxygen at carbon substitutional defect is about ?0.5 eV and at interstitial defect is ?0.18 eV. The HOMO-LUMO gap of the pure Si₄₃C₄₄H₇₆ is about 6.71 eV and after doping with oxygen changes on the order of 0.1 eV. Our studies show that the refractive index of the doped Si₄₃C₄₄H₇₆ nanocrystal significantly dispersed in comparison with pure SiC nanocrystal especially at the range of 6 to 8 eV.     

Simulation of Adsorbate-Induced Surface Reconstruction

Abstract

Adsorbed atomic monolayers of atoms such as carbon and nitrogen can cause substantial reconstructions of a nickel {001} surface. In this simulation we combine an atomic-orbital-based calculation of electronic structure with an empirical pair-wise repulsive potential to model the covalent part of the total energy. For 0.5 monolayer coverage by the adsorbate, the surface metal layer relaxes into a p(2 × 2) structure, with transverse displacements of about 0.4 Å. At the same time these displaced surface nickel atoms ride up above second layer nickels, with a vertical displcement of about 0.4 Å. The covalent contribution to the relaxation energy comes out at about 2.0 eV per carbon atom and 1.4eV per nitrogen atom, of which the reconstruction contributes about 0.3eV.     

Hydrogen dissociation on diene-functionalized carbon nanotubes

Chemical functionalization of a zigzag carbon nanotube (CNT) with 1, 3-cyclohexadiene (CHD), previously reported by experimentalists, has been investigated in the present study using density functional theory in terms of energetic, geometric, and electronic properties. Then, the thermodynamic and kinetic feasibility of H₂ dissociation on the pristine and functionalized CNTs have been compared. The dissociation energy of the H₂ molecule on the pristine and functionalized CNT has been calculated to be about ?1.00 and ?1.55 eV, while the barrier energy is found to be about 3.70 and 3.51 eV, respectively. Therefore, H₂ dissociation is thermodynamically more favorable on the CNT-CHD system than on the pristine tube, while the favorability of the dissociation on the pristine tube is higher in term of kinetics.     

Acetylene chain reaction on hydrogenated boron nitride monolayers: a density functional theory study

Spin-polarized first-principles total-energy calculations have been performed to investigate the possible chain reaction of acetylene molecules mediated by hydrogen abstraction on hydrogenated hexagonal boron nitride monolayers. Calculations have been done within the periodic density functional theory (DFT), employing the PBE exchange correlation potential, with van der Waals corrections (vdW-DF). Reactions at two different sites have been considered: hydrogen vacancies on top of boron and on top of nitrogen atoms. As previously calculated, at the intermediate state of the reaction, when the acetylene molecule is attached to the surface, the adsorption energy is of the order of ?0.82 eV and ?0.20 eV (measured with respect to the energy of the non interacting molecule-substrate system) for adsorption on top of boron and nitrogen atoms, respectively. After the hydrogen abstraction takes place, the system gains additional energy, resulting in adsorption energies of ?1.52 eV and ?1.30 eV, respectively. These results suggest that the chain reaction is energetically favorable. The calculated minimum energy path (MEP) for hydrogen abstraction shows very small energy barriers of the order of 5 meV and 22 meV for the reaction on top of boron and nitrogen atoms, respectively. Finally, the density of states (DOS) evolution study helps to understand the chain reaction mechanism.

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Graphical abstract Acetylene chain reaction on hydrogenated boron nitride monolayers

     

A density functional theory analysis for the adsorption of the amine group on graphene and boron nitride nanosheets

In this paper first principles total energy calculations to study the adsorption of amine group (NH₂) on graphene (G) and boron nitride (hBN) nanosheets are developed; the density functional theory, within the local density approximation and Perdew-Wang functional was employed. The sheets were modeled with a sufficiently proved C_nH_m-like cluster with armchair edge. The optimized geometry was obtained following the minimum energy criterion, searching on four positions for each nanosheet: perpendicular to the carbon atom, on the hexagon, inside the hexagon and on the bridge C–C, for the G-amine interaction; and, perpendicular to the B, perpendicular to the N, on the hexagon, and inside the hexagon, for the hBN-amine interaction. A physisorption, with amine parallel to the C–C–C bond with a distance graphene-amine of 2.56 Å, was found. For the case of BN a B–N bond, with bond length equal to 1.56 Å, was found; the amine lies perpendicular to the nanosheet. When the graphene is doped with B and Al atoms a chemisorption with B–N (1.57 Å) and Al–N (1.78 Å) bonds is observed; the bond angle in the amine group is also incremented, 5.5° and 8.1°, respectively. In the presence of point defects (monovacancies) of B in the hBN-amine and C in the G-amine, there exists chemisorption, increasing the reactivity of the sheets.     

Noncovalent and covalent functionalization of a (5, 0) single-walled carbon nanotube with alanine and alanine radicals

We have systematically investigated the noncovalent and covalent adsorption of alanine and alanine radicals, respectively, onto a (5, 0) single-walled carbon nanotube using first-principles calculation. It was found that XH···π (X = N, O, C) interactions play a crucial role in the non-ovalent adsorption and that the functional group close to the carbon nanotube exhibits a significant influence on the binding strength. Noncovalent functionalization of the carbon nanotube with alanine enhances the conductivity of the metallic (5, 0) nanotube. In the covalent adsorption of each alanine radical onto a carbon nanotube, the binding energy depends on the adsorption site on CNT and the electronegative atom that binds with the CNT. The strongest complex is formed when the alanine radical interacts with a (5, 0) carbon nanotube through the amine group. In some cases, the covalent interaction of the alanine radical introduces a half-filled band at the Fermi level due to the local sp ³ hybridization, which modifies the conductivity of the tube.     

Nitrous oxide adsorption on pristine and Si-doped AlN nanotubes

Using density functional theory, we studied the adsorption of an N₂O molecule onto pristine and Si-doped AlN nanotubes in terms of energetic, geometric, and electronic properties. The N₂O is weakly adsorbed onto the pristine tube, releasing energies in the range of ?1.1 to ?5.7 kcal mol^-1. The electronic properties of the pristine tube are not influenced by the adsorption process. The N₂O molecule is predicted to strongly interact with the Si-doped tube in such a way that its oxygen atom diffuses into the tube wall, releasing an N₂ molecule. The energy of this reaction is calculated to be about ?103.6 kcal mol^-1, and the electronic properties of the Si-doped tube are slightly altered.     

Perovskite Oxyfluoride Electrode Enabling Direct Electrolyzing Carbon Dioxide with Excellent Electrochemical Performances

Solid oxide electrolysis cells (SOECs) can efficiently convert the greenhouse‐gas CO₂ to valuable fuel CO at the cathodes. Herein, fluorine is doped into mixed ionic–electronic conducting Sr₂Fe_1.5Mo_0.5O_6‐δ (SFM), to evaluate its potential use as a cathode for CO₂ reduction reaction (CO₂‐RR). SFM retains its cubic structure after doped with fluorine, forming perovskite oxyfluoride Sr₂Fe_1.5Mo_0.5O_6‐δF_0.1 (F‐SFM). The substitution of oxygen by fluorine increases CO₂ adsorption by a factor of ≈2, bulk oxygen vacancy concentration by 35–37% at 800 °C, and consequently enhances the surface reaction rate constant for CO₂‐RR and chemical bulk diffusion coefficient by factors of 2–3. The faster kinetics are also reflected by a lower polarization resistance of 0.656 Ω cm² for F‐SFM than 1.130 Ω cm² for SFM at 800 °C in symmetrical cells. Furthermore, the single cell with F‐SFM cathode exhibits the best CO₂ electrolysis performance among the reported perovskite electrodes, achieving current density of 1.36 A cm^?2 at 1.5 V and excellent stability over 120 h at 800 °C under harsh conditions. The theoretical computations confirm that fluorine doping is energetically favorable to CO₂ adsorption and dissociation. The present work provides a promising strategy for the design of robust cathodes for direct CO₂ electrolysis in SOECs.     

Selective detection of cyanogen halides by BN nanocluster: a DFT study

The electronic sensitivity and adsorption behavior toward cyanogen halides (X–CN; X?=?F, Cl, and Br) of a B₁₂N₁₂ nanocluster were investigated by means of density functional theory calculations. The X-head of these molecules was predicted to interact weakly with the BN cluster because of the positive σ-hole on the electronic potential surface of halogens. The X–CN molecules interact somewhat strongly with the boron atoms of the cluster via the N-head, which is accompanied by a large charge transfer from the X–CN to the cluster. The change in enthalpy upon the adsorption process (at room temperature and 1 atm) is about ?19.2, ?23.4, and ?30.5 kJ mol^?1 for X?=?F, Cl, and Br, respectively. The LUMO level of the BN cluster is largely stabilized after the adsorption process, and the HOMO–LUMO gap is significantly decreased. Thus, the electrical conductivity of the cluster is increased, and an electrical signal is generated that can help to detect these molecules. By increasing the atomic number of X, the signal will increase, which makes the sensor selective for cyanogen halides. Also, it was indicated that the B₁₂N₁₂ nanocluster benefits from a short recovery time as a sensor.     

Kinetic and thermodynamic study of the substituent effect on the amino-Claisen rearrangement of para-substituted N-allyl-N-arylamine: a Hammett study via DFT

In order to find the susceptibility of the amino-Claisen rearrangement and the next proton shift reaction of N-allyl-N-arylamine to the substituent effects in the para position, the kinetic and thermodynamic parameters were calculated at the B3LYP level using the 6-31G^** basis set. The calculated activation energies for the rearrangements and proton shift reactions are close to 44.4 and 49.5 kcal mol^? 1, respectively. The transition states of the rearrangement with electron-donor substituents are more stable than those with electron-withdrawing substituent groups, but for the proton shift reaction, this situation is reversed (with the exception of fluorine atom for the rearrangement and fluorine and chlorine atoms for the proton shift reaction). Negative values for the activation entropy confirm the concerted mechanism for the amino-Claisen rearrangement and proton shift reaction. The Hammett ρ values of ? 2.4172 and ? 1.7791 are obtained for σ_p and σ^?  (enhanced sigma) in the amino-Claisen rearrangement, respectively. The correlation between log(k _X/k _H) and σ_p is weaker than that with σ^?  (enhanced sigma). A negative Hammett ρ value indicates that the electron-donating groups slightly increase the rate of amino-Claisen rearrangement. A positive Hammett ρ value (2.4921) for the proton shift reaction indicates that electron-withdrawing groups increase the rate of reaction.     

Silicon–doping in carbon nanotubes: formation energies, electronic structures, and chemical reactivity

By carrying out density functional theory (DFT) calculations, we have studied the effects of silicon (Si)-doping on the geometrical and electronic properties, as well as the chemical reactivity of carbon nanotubes (CNTs). It is found that the formation energies of these nanotubes increase with increasing tube diameters, indicating that the embedding of Si into narrower CNTs is more energetically favorable. For the given diameters, Si-doping in a (n, 0) CNT is slightly easier than that of in (n, n) CNT. Moreover, the doped CNTs with two Si atoms are easier to obtain than those with one Si atom. Due to the introduction of impurity states after Si-doping, the electronic properties of CNTs have been changed in different ways: upon Si-doping into zigzag CNTs, the band gap of nanotube is decreased, while the opening of band gap in armchair CNTs is found. To evaluate the chemical reactivity of Si-doped CNTs, the adsorption of NH₃ and H₂O on this kind of material is explored. The results show that N–H bond of NH₃ and O–H bond of H₂O can be easily split on the surface of doped CNTs. Of particular interest, the novel reactivity makes it feasible to use Si-doped CNT as a new type of splitter for NH₃ and H₂O bond, which is very important in chemical and biological processes. Future experimental studies are greatly desired to probe such interesting processes.      

Theoretical study of the geometrical and electronic structures and thermochemistry of spherophanes

A set of supramolecular cage-structures—spherophanes—was studied at the density functional B3LYP level. Full geometrical structure optimisations were made with 6–31G and 6–31G(d) basis sets followed by frequency calculations, and electronic energies were evaluated at B3LYP/6–31++G(d,p). Three different symmetries were considered: C1, Ci, and Oh. It was found that the bonds between the benzene rings are very long to allow π-electron delocalisation between them. These spherophanes show portal openings of 2.596 Å in Spher1, 4.000 Å in Meth2, 3.659 Å in Oxa3, and 4.412 Å in Thia4. From the point of view of potential host–guest interaction studies, it should also be noted that the atoms nearest to the centre of the cavities are carbons bonded to X groups. These supramolecules seem to exhibit relatively large gap HOMO?LUMO: 2.89 eV(Spher1), 5.26 eV(Meth2), 5.73 eV(Oxa3), and 4.82 eV(Thia4). The calculated ΔH°_f (298.15 K) values at B3LYP/6–31G(d) are (in kcal mol^?1) 750.98, 229.78, ?10.97, and 482.49 for Spher1, Meth2, Oxa3, and Thia4, respectively. Using homodesmotic reactions, relative to Spher1, the spherophanes Meth2, Oxa3, and Thia4 are less strained by ?399.13 kcal mol^?1, ?390.40 kcal mol^?1, and ?411.38 kcal mol^?1, respectively. Their infrared and ¹³C NMR calculated spectra are reported.     

Tunable differential conductance of single wall C/BN nanotube heterostructure

The transport properties and differential conductance of the heterostructures constructed by (5,5) single wall carbon nanotube (SWCNT) and (5,5) single wall boron nitride nanotube (SWBNNT) are investigated using density functional theory in combination with non-equilibrium Green’s functions. We find that the transmission conductance of (5,5) BN/C nanotube heterostructure is not only continually depressed as the BNNT region increases but also the drop of the conductance is uniform in the energy window (?1.43 eV, 1 eV), which leads to linear I–V dependence for the systems when the bias is within this energy range. Moreover, the differential conductance linearly decreases when n?≤?3 but exponentially decreases when n?≥?3 for (5,5)(BN) _n /C heterostructure. Such tunable differential conductance of (5,5) BN/C nanotube heterostructure mainly derives from the blockage of the transport channels induced by the semiconductive BN segment.