Si‐Doped B12N12 Nanocage as an Adsorbent for Dissociation of N2O to N2 Molecule

Adsorption of N₂O molecule by using density functional theory calculations at the B3LYP/6–31G* level onto pristine and Si‐doped B₁₂N₁₂ nanocage in terms of energetic, geometric, and electronic properties was investigated. The results of calculations showed that the N₂O molecule is physically adsorbed on the pristine and Si‐doped B₁₂N₁₂ (Si_N) models, releasing energies in the range of –1.13 to –2.02 kcal mol⁻¹. It was found that the electronic properties of the models have not changed significantly upon the N₂O adsorption. On the other hand, the adsorption energy of N₂O on the Si‐doped B₁₂N₁₂ (Si_B model) was about –67.20 kcal mol⁻¹and the natural bond orbital charge of 0.58|e| is transferred from the nanocage to the N₂O molecule. In the configuration, the O atom of N₂O molecule is bonded to the Si atom of the nanocage, so that an N₂ molecule escapes from the wall of the nanocage. The results showed that the Si_B model can be an adsorbent for dissociation of the N₂O molecule.     

Surface interaction of H2O and H2S onto Ca12O12 nanocluster: Quantum‐chemical analyses

To find the selectivity of H₂S, we explicate the adsorption properties of water (H₂O) and hydrogen sulfide (H₂S) molecules on the external surfaces of free Ca₁₂O₁₂ nanocages using the density functional theory method. More specifically, binding energies, natural bond orbital charge transfer, dipole moment, molecular electrostatic potential, frontier molecular orbitals, density of states, and global indices of activities are calculated to deeply understand the impacts of the aforementioned molecules on the electronic and chemical properties of Ca₁₂O₁₂ nanocages. Our theoretical findings indicate that although H₂O seems to be adsorbed in molecular form, the H₂S molecule is fully dissociated during the adsorption process because of the weak bond between sulfur and hydrogen atoms of the molecule. Interestingly, the highest occupied molecular orbital–lowest unoccupied molecular orbital energy gap of the nanocage is decreased by 1.87 eV upon H₂S adsorption, indicating that the electrical conductivity of the nanocage is strongly increased by the dissociation process. In addition, the values of softness and electrophilicity for the H₂S‐Ca₁₂O₁₂ complex are higher than those for the free nanocage. Our results suggest that Ca₁₂O₁₂ nanoclusters show promise in the adsorption/dissociation of H₂S molecules, which can be used further for designing its selective sensor.     

A DFT study on electronic and optical properties of aspirin-functionalized B<Subscript>12</Subscript>N<Subscript>12</Subscript> fullerene-like nanocluster

In this work, the interaction of an aspirin (AS) molecule with the external surface of a boron nitride fullerene-like nanocage (B₁₂N₁₂) is studied by means of density functional theory (DFT) calculations. Equilibrium geometry, electronic properties, adsorption energy and thermodynamic stability are identified for all of the adsorbed configurations. Four stable configurations are obtained for the interaction of AS molecule with the B₁₂N₁₂ nanocage, with adsorption energies in the range of ?10.1 to ?37.7 kcal/mol (at the M06-2X/6-31 + G** level). Our results clearly indicate that Al-doping of the B₁₂N₁₂ tends to increase the adsorption energy and thermodynamic stability of AS molecule over this nanocage. We further study the adsorption of AS over the B₁₂N₁₂ and B₁₁N₁₂Al in the presence of a protic (water) or aprotic (benzene) solvent. It is found that the calculated binding distances and adsorption energies by the PCM and CPCM solvent models are very similar, especially for the B₁₂N₁₂ complexes. According to time-dependent DFT calculations, the Al-doping can shift estimated λ _max values toward longer wavelengths (redshift). Solvent effects also have an important influence on the calculated electronic absorption spectra of AS-B₁₂N₁₂ complexes.     

Electronic Response of Nano-sized Cages of ZnO and MgO to Presence of Nitric Oxide

We have performed a comparative theoretical study on the adsorption of nitric oxide (NO) on Zn₁₂O₁₂ and Mg₁₂O₁₂ nanocages in terms of their energetic, geometric, and electronic properties. It has been found that NO adsorption on the MgO nanocage is energetically more favorable than that on the ZnO one. In contrast to the ZnO nanocage, HOMO-LUMO energy gap (Eg) of MgO one is dramatically decreased in the presence of NO molecule so that it is transformed from an intrinsic semiconductor (Eg≈5.00 eV) to a p-type one (Eg≈1.93 eV). We have predicted that electronic and conductance properties of the Mg₁₂O₁₂ nanocage are sensitive toward NO molecule, thus it may be potential candidate in detection of NO molecules.     

DFT Study of Endohedral Atoms Effect on Electrophilicity of B16N16 Boron Nitride Nanocage: Comparative Analyses

Endohedral derivatives of B₁₆N₁₆ nanocage (M@B₁₆N₁₆, M?=?Li⁺, Na⁺, K⁺, Mg²⁺, Ne, O^2?, S^2?, F^?, Cl^?) and its iso-electronic fullerne M@C₃₂ have been employed to investigate the relation between the trapped atom/ion and electrophilicity of the B₁₆N₁₆ and C₃₂ nanocages. The electrophilicity index, ??, of these endohedral nanocages has been evaluated from the ionization potential and the electron affinity computed by vertical ionization/affinity at the B3LYP/6-311++G(df,pd) level. Obtained results illustrate that the nature of trapped atom/ion affects HOMO-LUMO band gap, global electrophilicity indices and reactivity of B₁₆N₁₆ and C₃₂ nanocages. Encapsulation B₁₆N₁₆ with different atom/ions may be a possible method for modifying HOMO-LUMO energy gap, electrophilicity and so chemical characteristics of and C₃₂ nanocages.     

Theoretical studies on structures and nonlinear optical properties of alkali doped electrides B12N12–M (M = Li,Na, K)

The structures and nonlinear optical properties of a novel class of alkali metals doped electrides B₁₂N₁₂–M (M = Li, Na, K) were investigated by ab initio quantum chemistry method. The doping of alkali atoms was found to narrow the energy gap values of B₁₂N₁₂ in the range 3.96–6.70 eV. Furthermore, these alkali metals doped compounds with diffuse excess electron exhibited significantly large first hyperpolarizabilities (β₀) as follows: 5571–9157 au for B₁₂N₁₂–Li, 1537–18,889 au for B₁₂N₁₂–Na, and 2803–11,396 au for B₁₂N₁₂–K. Clearly, doping of the alkali atoms could dramatically increase the β₀ value of B₁₂N₁₂ (β₀ = 0). Furthermore, their transition energies (ΔE) were also calculated. The results showed that these compounds had low ΔE values in the range 1.407–2.363 eV, which was attributed to large β₀ values of alkali metals doped B₁₂N₁₂ nanocage. © 2016 Wiley Periodicals, Inc.     

Novel BC2N Nanocages: A DFT Investigation

We modeled and studied three types of novel B₁₂C₂₄N₁₂ cages. The structure of these cages was inspired by those of BC₂N nanotubes and the B₂₄N₂₄ fulborene skeleton. Density functional theory was used to investigate the various properties of the cages. All three isomers of B₁₂C₂₄N₁₂ were vibrationally stable. The highest occupied molecular orbital‐lowest unoccupied molecular orbital band gap was dependent on the BC₂N cage type. The B₁₂C₂₄N₁₂‐II cage was the most favorable nanocage and exhibited a large electric dipole moment. Natural bonding orbital (NBO) analysis confirmed the existence of lone pairs and unoccupied orbitals in the B₁₂C₂₄N₁₂ cages. New donor–acceptor interactions of natural MOs (Molecular Orbitals) were observed in BC₂N nanocages. The NBO and atomic polar tensor charges appeared to be fairly well correlated, showing that atomic charges can be obtained at a lower computational cost in this way.     

B12N12 Nano-cage as Potential Sensor for NO2 Detection

The NO₂ molecule adsorption on B₁₂N₁₂ nano-cage was investigated using density func-tional theory calculations in terms of adsorption energy, HOMO/LUMO energy gap (Eg) changes, charge transfer, structural deformation, etc. Furthermore, some aspects of stability and properties of B₁₂N₁₂ including calculation of binding electronic and Gibbs free energies, density of states, and molecular electrostatic potential surfaces are investigated. Three pos-sible configurations for NO₂ adsorption on the B₁₂N₁₂ nano-cage are energetically found. Interestingly, the results reveals that the Eg of B₁₂N₁₂ cluster is very sensitive to the pres-ence of NO₂ molecules as its value reduces from 6.84 eV in free cluster to 3.23 eV in the most stable configuration of NO₂/cluster complex. This phenomenon dramatically increases the electrical conductivity of the cluster, suggesting that the B₁₂N₁₂ nano-cluster may be potential sensor for NO₂ gaseous molecule detection.     

A Density Functional Investigation of Fluorinated B12N12 Clusters

Density functional calculations have been carried out on a series of fluorinated B₁₂N₁₂ molecules. The fluorine atoms are more prone to absorb on the boron atoms than the nitrogen atoms in B₁₂N₁₂. The 1,3 addition is an energetically favorable adsorption site in one‐fluorine‐molecule adsorption. We found that the average bond energy of fluorine molecule is decreased with n increasing, but significantly larger than that of B₁₂N₁₂F. The energy gap of B₁₂N₁₂ is controllable by introducing fluorine molecules. Moreover, calculation of the Gibbs free energy of the B₁₂N₁₂+12F₂→B₁₂N₁₂F₂₄ reaction showed that this reaction is exothermic at low temperatures.     

Transition metal atom adsorptions on a boron nitride nanocage

We have applied density functional theory within B3LYP and M05 functionals to investigate the chemical functionalization of B₁₂N₁₂ nanocage with 3d transition metal (TM) atoms. Main focuses have been placed on configurations corresponding to the located minima of the adsorbates, corresponding adsorption energies, and the modified electronic properties of the cage. It was shown that there is linear correlation between the adsorption energies of the B3LYP and M05 as the results of M05 are higher than those of B3LYP, about 0.52 eV. Based on calculations, the most stable adsorption site is over the bond shared by a four- and a six-membered ring in the outer surface of cluster, in most cases. Based on the M05 results, the adsorption energies of the Sc, Ti, V, Co, and Fe are relatively high (>1.51 eV) and those of Mn, Ni, and Cu calculated to be in the range of 1.00–1.22 eV. The Cr atom forms a weak bond with a boron atom of the B₁₂N₁₂ cluster, while Zn atom cannot be chemically adsorbed. Charge transfer from metals to cluster ascertained that the B₁₂N₁₂ plays as an electron-trapping center. Inducing certain impurity states within the electron density of states, the TM adsorption significantly reduces the HOMO–LUMO gap of cluster, ranging from 32 to 79 %.     

Modification of the Solution Behavior of Pd12L24 Metal–Organic Nanocages via PEGylation

The dilute solutions behaviors of Pd₁₂L₂₄ metal–organic nanocage and its two PEGylated derivatives are explored. The basic nanocages can self‐assemble into vesicle‐like blackberry structures in polar solvents via counterion‐mediated attraction, whereas the PEGylated nanocages always stay as discrete ions under the same conditions, demonstrating that the PEGylation can improve the stability of the single nanocages. In addition, larger nanocages are found to self‐assemble in less polar solvents.     

Predicting adsorption behavior of Triacanthine anticancer drug with pure B12N12 nano-cage: A theoretical study

Predicting adsorption behavior of the Triacanthine (TRC) anticancer drug on the surface of B₁₂N₁₂ nano-cage was investigated using DFT and TD-DFT methods by B3LYP/6-311+G(d) level in the water solution. The adsorption energies of the TRC-B₁₂N₁₂ complexes (A-C) were shown that the adsorption process is exothermic. The UV/Vis absorption and IR spectra analysis were calculated to investigate the changes happening in adsorption of TRC over nano-cage. According to the results, the interaction of the TRC drug from the N9 atom on the B₁₂N₁₂ nano-cage (model A) has the most chemical stability rather than models B and C. Based on NBO analysis, the charge transfer process has happened between the TRC drug and B₁₂N₁₂ nano-cage. Recovery time, charge difference (ΔN), and ELF analysis were calculated. It was understood that the B₁₂N₁₂ nano-cage can be a good carrier for the delivery of TRC anticancer medicine.     

DFT study on the selective complexation of B12N12 nanocage with alkali metal ions

Density functional theory (DFT) calculations were applied at the M05-2X/6-311++G(d,p) level of the theory to investigate the interaction of the B₁₂N₁₂ nanocage (BN) and alkali metal ions (Li⁺, Na⁺, K⁺, Rb⁺ and Cs⁺) in the gas phase and in water. On the basis of the results, BN nanocage is able to form a selective complex with Li⁺. Water, as a solvent, reduces the stability of the metal ion-BN complexes in comparison with the gas phase. Natural bond orbital (NBO) and quantum theory of atoms in molecules (QTAIM) analyses, reveal that the electrostatic interaction between the BN and metal ions can be considered as the driving force for complex formation in which the role of water is of significance. Density of states (DOSs) analysis of the BN nanocage structure in the presence of different metal ions showed a noticeable change in the frontier orbitals, especially in the gas phase, and Fermi level shifting toward the lower values.     

O3 and SO2 sensing concept on extended surface of B12N12 nanocages modified by Nickel decoration: A comprehensive DFT study

Adsorption of SO₂ and O₃ molecules on pristine boron nitride (B₁₂N₁₂) and Ni-decorated B₁₂N₁₂ nano-cages has been systemically investigated through density functional theory (DFT) methods. Adsorption energies (thermodynamics), bond distances, charge analysis, dipole moments, orbital analysis and density of states are calculated by van der Waals DFT method (MPW1PW91) functional. The adsorption energies of O₃ and SO₂ on pristine B₁₂N₁₂ are about −143.8 and −14.0 kJ mol⁻¹, respectively. The interaction energies of O₃ and SO₂ with pristine B₁₂N₁₂ are indicative of chemisorption and physisorption, respectively. Ni-decorated B₁₂N₁₂ (Ni@BN) enhances adsorption of both O₃ and SO₂ species. The interaction energies for adsorption of SO₂ are about −166 and −277 kJ mol⁻¹ whereas the corresponding energies for O₃ are −362 and −396 kJ mol⁻¹ for configuration A and B, respectively. These observations show that functionalized B₁₂N₁₂ are highly sensitive toward SO₂ and O₃ molecules.     

DFT based insights into reactivity descriptors of encapsulated B<Subscript>24</Subscript>N<Subscript>24</Subscript> nanocages

The purpose of this study is to probe the DFT based chemical reactivity parameter, electrophilicity index as a possible molecular engineering of endohedral BN-nanocages. The structure and electronic properties of endohedral boron nitride nanocages have been investigated as a function of alkali atom inside the nanocage using density functional theory. We have calculated and analyzed basic characteristic related to the reactive behavior, such as HOMO–LUMO band gap, chemical hardness, chemical potential, vertical electron affinity, and vertical ionization potential, as well as the global electrophilicity index, ω(I, A) of the encapsulated B₂₄N₂₄ nanocages. We also investigated the MQZVP basis set effect on total electronic energy of the clusters.     

Study on the surface interaction of Furan with X12Y12 (X = B,Al, and Y = N,P) semiconductors: DFT calculations

Chemisorption of Furan on the surfaces of four different semiconductors (Al₁₂N₁₂, Al₁₂P₁₂, B₁₂N₁₂, and B₁₂P₁₂) has been investigated, and the results have been compared using density functional theory in terms of energetic, geometric, and electronic property. Two functionals, dispersion corrected (wB97XD) and non‐corrected (B3LYP), have been used for calculation of binding energy. The results show that chemisorption of Furan on these semiconductors is in the order of Al₁₂N₁₂ (−98.4 kJ mol⁻¹) > Al₁₂P₁₂ (−77.5 kJ mol⁻¹) > B₁₂N₁₂ (−46.6 kJ mol⁻¹) > B₁₂P₁₂ (−18.3 kJ mol⁻¹), while the order of change in the HOMO–LUMO gap of semiconductors upon adsorption of Furan is found as B₁₂N₁₂ > B₁₂P₁₂ > Al₁₂P₁₂ > Al₁₂N₁₂, which implies to the higher changes in the electronic structure of B‐containing clusters (B₁₂N₁₂ and B₁₂P₁₂) compared to Al‐containing clusters (Al₁₂N₁₂ and Al₁₂P₁₂). The NBO charge analyses reveal maximum and minimum charge transfer upon adsorption of Furan on B₁₂N₁₂ and B₁₂P₁₂, respectively. Based on the results, it was found that Al₁₂N₁₂ and B₁₂N₁₂ as the most appropriate adsorbent and the most sensitive sensor for Furan, respectively.     

A comparative study of Mannosylerythritol lipids (MELs) surfactant adsorption upon the Al12N12 and B12N12 nano-cages as potential candidates for detecting MELs

Aluminum nitride and boron nitride nanocages have recently been discovered. The properties of these compounds vary according to their size. In this paper, we study the adsorption of MELs on aluminum nitride and boron nitride nanocages in the solution phase using density functional theory. The results of adsorption energies indicate that during the adsorption on aluminum nanocages, ether oxygen atoms show stronger adsorption, while adsorption is stronger on boron nitride nanocage from the hydroxyl group oxygen. The results of thermodynamic calculations indicate that all adsorption positions of aluminum nitride are thermodynamically favorable. However, in the case of boron nitride, some positions are thermodynamically unfavorable. In terms of recovery time, borne nitride is not a good adsorbent because of very small recovery time. The aluminum nitride may be able to behave as a suitable sensor for the MELs in the solution phase. Nevertheless, boron nitride does not have this capability, since it does not significantly change the number of conducting electrons.     

Electron transport properties of boron nitride fullerene B24N24 doped with lithium atom: first-principles calculations

The transport properties of Li@B₂₄N₂₄ metallofullerene bridging two Au contacts are studied with a combined density functional theory and the non-equilibrium Green’s-function technique. Our calculated results show that the conductance of Li@B₂₄N₂₄ nanocage is generally higher than that of the undoped B₂₄N₂₄ molecule. We calculated the current–voltage characteristics for positive and negative bias voltages. It was found that due to presence of Li in B₂₄N₂₄ nanocage, a novel negative differential resistance (NDR) phenomenon is observed. Furthermore, the transmission coefficients of the Li@B₂₄N₂₄ metallofullerene at various external biases are analyzed and it indicates that the broadening of the transmission coefficient spectrum with increasing of the external biases confirms the NDR behavior at the I–V characteristic.     

Adsorption properties of hydrazine on pristine and Si-doped Al12N12 nano-cage

The interaction of hydrazine (N₂H₄) molecule with pristine and Si-doped aluminum nitride (Al₁₂N₁₂) nano-cage was investigated using the density functional theory calculations. The adsorption energy of N₂H₄ on pristine Al₁₂N₁₂ in different configurations was about –1.67 and –1.64 eV with slight changes in its electronic structure. The results showed that the pristine nano-cage can be used as a chemical adsorbent for toxic hydrazine in nature. Compared with very low sensitivity between N₂H₄ and Al₁₂N₁₂ nano-cage, N₂H₄ molecule exhibits high sensitivity toward Si-doped Al₁₂N₁₂ nano-cage so that the energy gap of the Si-doped Al₁₂N₁₂ nano-cage is changed by about 31.86% and 37.61% for different configurations in the Si_Al model and by about 26.10% in the Si_N model after the adsorption process. On the other hand, in comparison with the Si_Al model, the adsorption energy of N₂H₄ on the Si_N model is less than that on the Si_Al model to hinder the recovery of the nano-cage. As a result, the Si_N Al₁₂N₁₁ is anticipated to be a potential novel sensor for detecting the presence of N₂H₄ molecule.     

The electronic structure ofα-B12, B12P2 and B12AS2

The electronic band structures of the rhombohedral-based boron compounds -B₁₂, B₁₂P₂ and B₁₂ As₂ have been investigated along all symmetry directions. The calculations show that the band gap, in all cases, is of the order of 2 eV, which correlates with the known color of -rhombohedral boron. The materials should be intrinsic semi-conductors, as has recently been shown experimentally. The states around the band gap in -B₁₂ are dominated by the boron 2p atomic states. The bonding in the icosahedra, as illuminated by cluster calculations, is shown to be rather similar to that in the isolated B₁₂ icosahedron. Of the intericosahedron interactions, those between B(2) and B(2) atoms are the strongest and have a bond index just above unity. In B₁₂P₂ the orbitals of the P₂ moiety make a significant contribution to the valence band edge states and the conduction band edge states also incorporate considerable (55%) phosphorus 3d orbital character. In B₁₂As₂ the arsenic 4d orbitals do not have as much effect in that crystal as do the 3d orbitals in B₁₂P₂.