NMR Shielding Tensors and Thermodynamic Investigation of B 28 N 28 Nano-cone Structure : A molecule for Fe 3 + Capturing

M06&B3LYP/3-21G/6-31G/6-31G*/6-311G* density functional theory (DFT) and HF/3-21G/631G/6-31G*/6-311G *ab-initio calculations have performed for the structure and stability of B28N28 nano-cone. In this work, it was calculated the geometrical structure, and stability to predict NMR and thermodynamics parameters. We have found these kinds of nano-cone are useful for capturing of Fe3+ Ion

Its structure, which is in the form of a hexagonal mesh, resembles a graphite sheet and it carries a carbon atom located on the vertex of each mesh.The sheet has rolled and its two edges have connected seamlessly [6][7][8][9][10][11][12][13][14][15] .
Although it is a commonplace material using in pencil leads, its unique structure causes it to present characteristics that had not found with any other materials.CNT can be classified into single-wall CNT, double-wall CNT and multi-wall CNT according to the number of layers of the rolled graphite [16][17][18][19][20] .
The type attracting most attention is the single-wall CNT, which has a diameter deserving the name of "nanotube" of 0.4 to 2 nanometers.The length is usually in the order of microns, but single-wall CNT with a length in the order of centimeters has recently released [19][20][21][22][23][24][25] .
CNT can be classified into single-wall CNT, double-wall CNT and multi-wall CNT according to the number of layers of the rolled graphite.The type attracting most attention is the single-wall CNT, which has a diameter deserving the name of "nanotube" of 0.4 to 2 nanometers [20][21][22][23][24][25][26] .
The length is usually in the order of microns, but single-wall CNT with a length about centimeters have recently released.The extremities of the CNT have usually closed with lids of the graphite sheet 21- 30 .
Theoretical studies have been performed for fullerene-like B28N28 clustersin which it has been found that a structure built from squares and hexagons is more stable than those built from pentagons and hexagons.This is because in the second case less stable B-B and N-N bonds are formed  .
The most stable B28N28structure is built from six squares and eight hexagons  .
In this work, we focused on B28N28 nanocon.Our aim was to obtain the global minimum energy structure.For this structure, we use the hybrid B3LYP exchange-correlation functional within density functional theory.Primary, structure optimization calculated and then Nuclear Magnetic Resonance (NMR) parameters by density Functional Theory (DFT) method calculated on the optimized structure.Isotropic chemical shielding, anisotropic chemical shielding parameters at all of the atoms nuclei are presented in Table 1.And also, Thermodynamic Properties have been considered in Table 2 We have found that these kinds of Nanocones are useful for Fe 3+ Capturing.In material sciences Boron nitride, which appears in a manifold of crystalline modifications, has been an extremely practical material with hexagonal and cubic boron nitride as most outstanding materials.The BN cluster is a polar molecule and BN nanotubes have an inert chemical structure.We can see that there is a negative charge at nitrogen atom and a positive charge at boron atom, so we can use an electrophilic or nucleophilic reagent as a solution for BN clusters.
BN nanotubes are very suitable for composite materials because these structures have a higher temperature resistance to oxidation than the carbon nanotubes.All the BN nanotubes are semiconductors.The BN nanotubes have the band gaps which can be greater than 2 eV for most tubes also we know that the smallest carbon nanotubes are semiconductor and these structures obtain the properties of graphite when the diameter of these structures increases but BN nanotubes are semiconductors without attention to the diameter.On the basis of the similarities in characteristics between carbon and BN-based (BN=boron nitride) substances, BN-based nanotubes can be stable and therefore their electronic structure can be studied.The comparison between BN nanotubes and carbon nanotubes shows that BN nanotubes have more interesting characteristics than the carbon nanotubes  .
Recently the boron nitride (BN) nanoscale cone particles have been discovered and these structures are made up of conical shells without any seamless.Most of the studies about nanocones have been done so far with carbon structures.Highresolution transmission electron microscopy and nanobeam electron diffraction made the orientation of the BN hexagonal rings possible.Recently theoretical investigations on (BN) n nanocones have gained more attention in carbon nanotubes when there is not any experimental result [55-100].
Considering the above mentioned, BN nanotubes are very important and interesting for new research and can open a huge spectrum in the field of theoretical and experimental research.In the fig. 1 structure of B 28 N 28 is shown and this particular nanocone configuration has been proposed in this research.

Computational Method
The Gaussian 98 program was run to obtain the best prediction of this particular structure.Also all Ab-Initio and DFT (density functional theory) calculations were done with the Gaussian 98 program.Frequency analyses were carried out to show that the optimized structures are true minima or transition states on the potential energy surfaces of a specific structure without imaginary frequencies.
In this work, geometry optimizations in the gas phase for B 28 N 28 were performed at density functional theory (DFT) level with B3LYP and Ab-Initio with HF (hartree fock) methods in different basis sets at the temperature of 298.15K,The parameters were calculated for B 28 N 28 in the gas phase in different methods and basis sets include thermodynamic and NMR parameters.The chemical shielding shows the phenomenon which is dependent on the secondary magnetic field which is built by the induced movements of the electrons which encompass the nuclei.The chemical shielding is built by a three-by-three matrix which is biodegraded into a single scalar term, three antisymmetric pseudo vector components, and five components which correspond to a symmetric tensor.It can be observed the single scalar and the five symmetric tensor elements in the normal NMR spectra of the solids.
The chemical shielding tensor includes the chemical shift isotropy (CSI) and chemical shift anisotropy (CSA) and the anisotropy () of the tensor, the shielding tensor asymmetry parameter () and chemical shift () are calculated.
The thermodynamic parameters that were calculated in this research are Gibbs free energy, enthalpy, internal energy (It is clear that the sum of zero point energy (ZPE) and thermal energy is internal energy.)and entropy then these reports were compared with each other in order to obtain the best results.These results were reported in tables.

RESULTS AND DISCUSSION
The results are listed in tables 1-3, and the figures are explained in figs 1-4.The geometry optimization for B 28 N 28 nano-cone has been done with HF and B3LYP methods at different basis sets such as 4-31G, 6-31G, 6-31G* and 6-311G*.Then thermodynamic properties were calculated for this structure in gas phase at 298.15K in the same methods and basis sets.A comparison of Gibbs free energy (G), Enthalpy (H), Entropy (S) and Internal energy (E) in different methods and basis sets are shown in table 2. As shown in table 2, the maximum values for Gibbs free-energy (G) , Enthalpy (H) and Internal energy (E) were calculated when 6-311G* basis set had been applied at B3LYP method.
According to the results that are shown in table2, the largest values have been obtained in B3LYP method.
Considering the optimized structure, the NMR shielding tensors were calculated then these parameters were used to show active sites in this structure.The results of  iso ,  aniso, ,  and • for this nanocone in the same methods and basis sets are shown in table 3.Finally the charts of  iso ,  aniso,  and  for the atoms of B 10 N 11 in the 4-31G, 6-31G, 6-31G*, 6-311G* level of theory and B3LYP and HF methods.We can obtain the interesting results from the NMR charts.Comparison of these charts ( iso ,  aniso ,  and ) shows that some of peaks in these charts are similar to each other.If these peaks are reviewed, we can understand which similar atoms are situated in the same peaks of different charts.The comparison of these peaks shows that three atoms are exactly repeated in  iso ,  aniso ,  and  charts.These three atoms are the active sites in this structure in B 28 N 28   In general, the chart of electronic charge in different methods and basis sets is similar to the charts of NMR parameters Nitrogen atoms have more electrons than Boron atoms therefore the location of negative electronic charge is on Nitrogen atoms and  It is clear that Nitrogen atoms will be active sites in this structure.

CONCLUSION
In summary, the stability of B 28 N 28 was investigated.It is found that the amount of Gibbs free energy (G) , Enthalpy (H) and internal Energy (E) obtained in B3LYP/6-311G* level in the gas phase ( 298.15K ) are the largest amount and also optimization of B 28 N 28 nano-cone at the B3LYP/6-311G*is suitable for this structure.The NMR data and the thermodynamics results indicate that this kind of nano-cone is suitable for capturing Fe 3+ ion.