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Proceedings - Interdisciplinary Center for Nanotoxicity

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Conference on Current Trends in Computational Chemistry 2009<br />

construct the quantum mechanical structure of molecule, which is known as molecular graph<br />

(MG) [11]. The MG of studied molecule has been depicted in Figure 1b.<br />

The AIM analysis <strong>for</strong> the optimized structures (Figure 1a) has been per<strong>for</strong>med to obtain<br />

the topological properties of the bonds, such as the Laplacian of b ρ ( 2<br />

∇ ρb<br />

), total energy<br />

density (Hb) at BCPs, bond critical points (BCPs), ring critical points (RCPs) and also the bond<br />

2<br />

paths (BPs). As is known, ∇ ρb<br />

and/or Hb identifies whether the charge of the region is shared<br />

2<br />

2<br />

interactions ( ∇ ρ b < 0 and/or H b < 0 ) or closed shell interactions ( ∇ ρ b > 0 and/or H b > 0 ).<br />

The <strong>for</strong>mer characterizes shared interactions (covalent bonds), where the electron density<br />

concentrates in the inter nuclear region, whereas the latter is typically associated with<br />

interactions between closed‐shell systems (ionic bonds, hydrogen bonds, and vander waals<br />

molecules).<br />

a b<br />

Figure 1. (a) The optimized geometry of FOX‐7 at level of MP2/aug‐cc‐pVDZ. (b) The 3D<br />

molecular graph (MGs) of the equilibrium geometry of FOX‐7 (Red points are Bond Critical<br />

Points: BCPs; Yellow points are Ring Critical Points: RCPs. The lines are Bond Paths: BPs).<br />

The complete list of bond critical points of electron density (where ∇ρ = 0 ) and their<br />

mathematical characters have been gathered in Table 1 <strong>for</strong> FOX‐7 with RHF, B3LYP and MP2<br />

levels and aug‐cc‐pVDZ basis set. The completeness of critical point (CP) analysis has been<br />

checked by the satisfaction of Poincare‐Hopf rule [11,12].<br />

n − b + r − c = 1<br />

Where n is the number of nuclei and b, r and c are the number of bond, ring and cage<br />

critical points, respectively.<br />

In attention to Gillespie‐Popelier discusión [12], and Table 1, represent the following<br />

2<br />

bonding natures: the most of bonded interactions are shared covalent ( ∇ ρ b < 0 , H b < 0 and<br />

ρ b order of 10 ‐1 2<br />

a.u.) and O(s)‐H(s) and O(t)‐O(t) interactions with ∇ ρ b > 0 and H b > 0 are<br />

closed shell. O(s)‐H(s) is hydrogen bond and O(t)‐O(t) is not meaning classically. The vibrational<br />

mode of O(t)‐O(t) interaction along with bending of C<br />

NO 2<br />

NO 2<br />

in RHF, B3LYP and MP2 levels are<br />

313.6, 293.2 and 268.4 cm ‐1 respectively. So the normal mode is populated in room<br />

temperature and the BCP between O(t)‐O(t) can be disappeared.<br />

95

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