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首页> 外文期刊>Acta Crystallographica, Section B. Structural science, crystal engineering and materials >Nature of E_2X_2 σ(4c–6e) of the X---E—E---X type at naphthalene 1,8-positions and model, elucidated by X-ray crystallographic analysis and QC calculations with the QTAIM approach
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Nature of E_2X_2 σ(4c–6e) of the X---E—E---X type at naphthalene 1,8-positions and model, elucidated by X-ray crystallographic analysis and QC calculations with the QTAIM approach

机译：X-2X_2σ（4C-6E）的性质X --- E-E --- X型在萘1,8-位置和模型中，通过X射线晶体分析和QC方法阐明的Qtaim方法阐明

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The nature of E_2X_2 σ(4c–6e) of the X-*-E-*-E-*-X type is elucidated for 1-(8- XC_(10)H_6)E–E(C_(10)H_6X-8')-1' [(1) E, X= S, Cl; (2) S, Br; (3) Se, Cl; (4) Se, Br] after structural determination of (1), (3) and (4), together with model A [MeX--- E(H)—E(H)-- -XMe (E = S and Se; X = Cl and Br)]. The quantum theory of atoms-in-molecules dual functional analysis (QTAIM-DFA) is applied. The total electron energy densities H_b(r_c) are plotted versus H_b(r_c) – V_b(r_c)/2 for the interactions at the bond critical points (BCPs; *), where V_b(r_c) show the potential energy densities at the BCPs. Data for the perturbed structures around the fully optimized structures are employed for the plots, in addition to those of the fully optimized structures. The plots were analysed using the polar coordinate (R, θ) representation of the data of the fully optimized structures. Data containing the perturbed structures were analysed by (θ_p, k_p), where θ_p corresponds to the tangent line of the plot and k_p is the curvature. Whereas (R, θ) shows the static nature, (θ_p, k_p) represents the dynamic nature of interactions. E-*-E are all classified as shared shell (S) interactions for (1)–(4) and as weak covalent (Cov-w) in nature (S/Cov-w). The nature of pure CS (closed shell)/ typical-HB (hydrogen bond) with no covalency is predicted for E-*-X in (1) and (3), regular CS/typical-HB nature with covalency is predicted for (4), and an intermediate nature is predicted for (2). The NBO energies evaluated for E-*-X in (1)–(4) are substantially larger than those in model A due the shortened length at the naphthalene 1,8-positions. The nature of E_2X_2 of σ(4c–6e) is well elucidated via QTAIM-DFA.
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