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Molecular Physics
An International Journal at the Interface Between Chemistry and Physics
Volume 107, 2009 - Issue 8-12: A Special Issue in Honour of Professor Henry F. Schaefer
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Invited Articles

Tetrahedranes. A theoretical study of singlet E4H4 molecules (E = C–Pb and B–Tl)

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Pages 911-922 | Received 17 Nov 2008, Accepted 08 Dec 2008, Published online: 07 Oct 2010
 

Abstract

Quantum chemical calculations using DFT (B3LYP) and ab initio (CCSD(T)) methods have been carried out to elucidate the E4H4 singlet potential energy hypersurface for the group-13 and group-14 elements. The results show that there are numerous E4H4 energy minima for the compounds of group-13 and group-14 elements. This holds particularly for the heavier atoms. The classical Td tetrahedron structure is energetically more favourable for the group-13 compounds E4H4 where the tetrahedron isomers are energy minima for all elements E except for thallium. The tetrahedranes Al4H4 1Al and Ga4H4 1Ga are the global energy minima on the singlet PES while 1B is slightly less stable than the singly hydrogen-bridged planar form 12B which has a rhombic B4 core. The lowest-lying energy minima for In4H4 and Tl4H4 are tetrahedranes where the E4 core is face-bridged by the hydrogen atoms. The classical Td tetrahedron structure of the group-14 elements is only for carbon and silicon an energy minimum at B3LYP/def2-TZVPP. The latter form of Si4H4 is a second-order saddle point at BP86/def2-TZVPP and MP2/def2-TZVPP. The global energy minimum form for C4H4 is the vinylideneacetylene isomer 27C which is −63.7 kcal/mol lower in energy than the tetrahedrane. The most stable isomers of Si4H4 and Ge4H4 at CCSD(T)/def2-QZVPP//B3LYP/def2-TZVPP//B3LYP/def2-TZVPP are the singly hydrogen edge-bridged tetrahedrane structures 18E, which are more than 40 kcal/mol lower in energy than the classical tetrahedrane. The B3LYP/def2-TZVPP calculations predict that tetrahedrane structure with edge-bridging hydrogen atoms 3Ge is slightly more stable than 18Ge. The former isomer is calculated as the global energy minimum on the singlet PES of Sn4H4 and Pb4H4.

Acknowledgement

The generous allotment of computer time by the HRZ Marburg, the CSC Frankfurt, the HHLR Darmstadt and the HLR Stuttgart, as well as their excellent service is gratefully acknowledged. This work was supported by the Deutsche Forschungsgemeinschaft.

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