Theoretical Investigation of the Low-Lying Electronic States of Dioxirane:  Ring Opening to Dioxymethane and Dissociation into CO2 and H2

The low-lying electronic states of dioxirane (1), their ring opening to dioxymethane (2), and the dissociation of 2 into CO2 and H2 have been investigated by means of CASSCF and MRD-CI+Q quantum chemistry calculations. The ground state of 1 is a singlet with 4π electrons, 1A1(4π), while the ground s...

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Published inThe journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory Vol. 102; no. 19; pp. 3398 - 3406
Main Authors Anglada, Josep M, Bofill, Josep M, Olivella, Santiago, Solé, Albert
Format Journal Article
LanguageEnglish
Published American Chemical Society 07.05.1998
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Summary:The low-lying electronic states of dioxirane (1), their ring opening to dioxymethane (2), and the dissociation of 2 into CO2 and H2 have been investigated by means of CASSCF and MRD-CI+Q quantum chemistry calculations. The ground state of 1 is a singlet with 4π electrons, 1A1(4π), while the ground state of 2 is a 2π-electron singlet, 11A1(2π), lying 5.8 kcal/mol higher than 1 in energy. A 0 K activation energy of 21.4 kcal/mol is predicted for the thermal ring opening of 1 into 2, which takes place via a transition structure approximately corresponding to the crossing between the lower 1A1(4π) and 1A1(2π) states of both molecules. Twelve excited states have been calculated for 1 with vertical excitation energies ranging from 3.07 to 13.11 eV. The energy ordering of these states changes dramatically upon relaxation of the molecular geometries. The optimum geometries of these excited states show an ∠OCO in the 106.3−120.1° range, so they should be considered as excited states of 2. Minimum energy points of the intersection seam between the 11A2(3π)/11B1(3π), 11B1(3π)/1A1(2π), 11A2(3π)/1A1(4π), and 11B1(3π)/1A1(4π) potential energy surfaces have been located in an ∠OCO range of 91.0−104.6°. The photochemical ring opening of 1 into 2 may occur through vertical excitation to either the 11B1(3π) or 11A2(3π) states of 1 and subsequent radiationless decay to ground-state 2 via minimum energy intersection points on the potential energy surfaces of the appropriate states. The dissociation of ground-state 2 into CO2 and H2 is predicted to be exothermic by 105.2 kcal/mol with a 0 K activation energy of 3.2 kcal/mol, while the dissociations of the first four excited states of 2 are all predicted to be endothermic.
Bibliography:istex:B774988841604283077690265B584EA4E1C64E33
ark:/67375/TPS-M0T73M08-4
ISSN:1089-5639
1520-5215
DOI:10.1021/jp980501v