\begin{document}$ O_h $\end{document} symmetry, SF6 has received wide attention for both the fundamental scientific interest and practical industrial applications. Theoretical work shows that the electronic configuration of ground electronic state \begin{document}$ ^1{\rm A_{1g}} $\end{document} of SF6 is \begin{document}${({\rm {core}})^{22}}{(4{\rm a_{1\rm g}})^2}{(3{{\rm t}_{1\rm u}})^6}{(2{{\rm e}_{\rm g}})^4}{(5{{\rm a}_{1\rm g}})^2}{(4{{\rm t}_{1\rm u}})^6}{(1{{\rm t}_{2\rm g}})^6}{(3{{\rm e}_{\rm g}})^4}{(1{{\rm t}_{2\rm u}})^6}{(5{{\rm t}_{1\rm u}})^6}{(1{{\rm t}_{1\rm g}})^6} $\end{document} and the symmetry of the HOMOs is \begin{document}$ T_{1g} $\end{document}. However, in some literature, the symmetry of HOMOs of SF6 has been written as \begin{document}$ T_{2g} $\end{document} instead of \begin{document}$ T_{1g} $\end{document}. The reason for this mistake lies in the fact that in the ab initial quantum chemical calculation used is the Abelian group \begin{document}$ D_{2h} $\end{document}, which is the sub-group of \begin{document}$ O_h $\end{document}, to describe the symmetries of molecular orbitals of SF6. However, there does not exist the one-to-one matching relationship between the representations of \begin{document}$ D_{2h} $\end{document} group and those of \begin{document}$ O_h $\end{document} group. For example, both irreducible representations \begin{document}$ T_{1g} $\end{document} and \begin{document}$ T_{2g} $\end{document} of \begin{document}$ O_h $\end{document} group are reduced to the sum of \begin{document}$ B_{1g} $\end{document}, \begin{document}$ B_{2g} $\end{document} and \begin{document}$ B_{3g} $\end{document} of \begin{document}$ D_{2h} $\end{document}. So the symmetry of the orbitals needs to be investigated further to identify whether it is \begin{document}$ T_{1g} $\end{document} or \begin{document}$ T_{2g} $\end{document}. In this work, we calculate the orbital functions in the equilibrium structure of ground state of SF6 by using HF/6-311G* method, which is implemented by using the Molpro software. The expressions of the HOMO functions which are triplet degenerate in energy are obtained. Then by exerting the symmetric operations of \begin{document}$ O_h $\end{document} group on three HOMO functions, we obtain their matrix representations and thus their characters. Finally, the symmetry of the HOMOs is verified to be \begin{document}$ T_{1g} $\end{document}. By using this process, we may determine the molecular orbital symmetry of any other molecules with high symmetry group."> - 必威体育下载

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    Wu Rui-Qi, Guo Ying-Chun, Wang Bing-Bing
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    • Abstract views:8026
    • PDF Downloads:63
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    • Received Date:19 December 2018
    • Accepted Date:20 February 2019
    • Published Online:20 April 2019

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