Issue 4, 1986

Ab initio valence bond calculations for the ground state of ozone

Abstract

The results of ab initio valence-bond calculations, with an STO-6G basis set, are reported for the ground state of ozone. Both Heitler–London and localized molecular-orbital procedures have been used to construct the wavefunctions for the σ-bonds. Hybridization of the orbitals on each atom has been determined by energy considerations.

In accord with previous results, the primary Lewis structure is calculated to be the spin-paired diradical structure (6) with two σ-bonds, and a long, or formal, π-bond associated with the terminal atoms. However, the sum of weights for four Lewis structures (11)–(14), which arise from polarization of either σ-bond in (6), is calculated to exceed the weight for (6).

Particular attention is given to the calculation of energies for “increased-valence” structures (1) and (2), which are constructed by spin-pairing the two unpaired electrons of ground-state O2 with those of a ground-state oxygen atom. If a two-centre molecular orbital is used to accommodate the two electrons of the O—O σ-bond in each of these structures, then resonance between these structures is equivalent to resonance between numerous Lewis structures including (6)+(11)–(14), when Heitler–London procedures are used to formulate the wavefunctions for all electron-pair bonds in the Lewis structures. The results of calculations which utilize this approach indicate that resonance between increased-valence structures provides the primary valence bond representation for the O3 ground state. Such structures are stabilized slightly by interaction with the Lewis structures that involve excited states for the O atom and the O2 molecule. The resulting energy for resonance between these four valence-bond structures lies at least 0.134 au below the STO-6G RHF-MO energy of –224.091 au.

Article information

Article type
Paper

J. Chem. Soc., Faraday Trans. 2, 1986,82, 495-509

Ab initio valence bond calculations for the ground state of ozone

R. D. Harcourt, F. L. Skrezenek, R. M. Wilson and R. H. Flegg, J. Chem. Soc., Faraday Trans. 2, 1986, 82, 495 DOI: 10.1039/F29868200495

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