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Comparison of σ‐/π‐Hole Tetrel Bonds between TH<sub>3</sub>F/F<sub>2</sub>TO and H<sub>2</sub>CX (X=O, S, Se)

Wenbo DongLaboratory of Theoretical and Computational Chemistry, School of Chemistry and Chemical Engineering Yantai University Yantai 264005 People's Republic of ChinaBingbo NiuLaboratory of Theoretical and Computational Chemistry, School of Chemistry and Chemical Engineering Yantai University Yantai 264005 People's Republic of ChinaShufeng LiuLaboratory of Theoretical and Computational Chemistry, School of Chemistry and Chemical Engineering Yantai University Yantai 264005 People's Republic of ChinaJianbo ChengLaboratory of Theoretical and Computational Chemistry, School of Chemistry and Chemical Engineering Yantai University Yantai 264005 People's Republic of ChinaShaoli LiuLaboratory of Theoretical and Computational Chemistry, School of Chemistry and Chemical Engineering Yantai University Yantai 264005 People's Republic of ChinaQingzhong LiLaboratory of Theoretical and Computational Chemistry, School of Chemistry and Chemical Engineering Yantai University Yantai 264005 People's Republic of China
2019en
ABI

Аннотация

Abstract Several σ‐hole and π‐hole tetrel‐bonded complexes with a base H 2 CX (X=O, S, Se) have been studied, in which TH 3 F (T=C−Pb) and F 2 TO (T=C and Si) act as the σ‐hole and π‐hole donors, respectively. Generally, these complexes are combined with a primary tetrel bond and a weak H‐bond. Only one minimum tetrel‐bonded structure is found for TH 3 F, whereas two minima tetrel‐bonded complexes for some F 2 TO. H 2 CX is favorable to engage in the π‐hole complex with F 2 TO relative to TH 3 F in most cases, and this preference further expands for the Si complex. Particularly, the double π‐hole complex between F 2 SiO and H 2 CX (X=S and Se) has an interaction energy exceeding 500 kJ/mol, corresponding to a covalent‐bonded complex with the huge orbital interaction and polarization energy. Both the σ‐hole interaction and the π‐hole interaction are weaker for the heavier chalcogen atom, while the π‐hole interaction involving F 2 TO (T=Ge, Sn, and Pb) has an opposite change. Both types of interactions are electrostatic in nature although comparable contributions from dispersion and polarization are respectively important for the weaker and stronger interactions.

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