AB INITIO POTENTIAL ENERGY SURFACES FOR THE $I(^{2}P_{3/2})+O_{2}(a^{1}\Delta_{g})\leftrightarrow I(^{2}P_{1/2}) + O_{2}(X^{3}\Sigma^{-}{_{g}})$ ENERGY TRANSFER PROCESS
dc.creator | Kaledin, A. L. | en_US |
dc.creator | Heaven, M. C. | en_US |
dc.creator | Morokuma, K. | en_US |
dc.date.accessioned | 2006-06-15T19:04:25Z | |
dc.date.available | 2006-06-15T19:04:25Z | |
dc.date.issued | 1998 | en_US |
dc.identifier | 1998-RG-05 | en_US |
dc.identifier.uri | http://hdl.handle.net/1811/18935 | |
dc.description | Author Institution: Cherry L. Emerson Center for Scientific Computation and Department of Chemistry, Emory University | en_US |
dc.description.abstract | Ab initio electronic structure calculations have been used to investigate the electronic energy transfer process: $I(^{2}P_{3/2})+O_{2}(a^{1}\Delta_{g})\leftrightarrow I(^{2}P_{1/2})+O_{2}(X^{3}\Sigma^{-}{_{g}})$ Potential energy surfaces for all states associated with the reactants and products were obtained using CASSCF and CASPT2 methods, including the effective one-electron spin-orbit Hamiltonian. Surfaces correlating with the reactants and products were all found to be non-bonding. Shallow van der Waals minima were predicted at long range. Surface crossings were found at energies below the $I(^{2}P_{3/2})+O_{2}(a^{1}\Delta_{g})$ asymptote. It is probable that these crossings are responsible for the efficient transfer of electron energy in this system. | en_US |
dc.format.extent | 82552 bytes | |
dc.format.mimetype | image/jpeg | |
dc.language.iso | English | en_US |
dc.publisher | Ohio State University | en_US |
dc.title | AB INITIO POTENTIAL ENERGY SURFACES FOR THE $I(^{2}P_{3/2})+O_{2}(a^{1}\Delta_{g})\leftrightarrow I(^{2}P_{1/2}) + O_{2}(X^{3}\Sigma^{-}{_{g}})$ ENERGY TRANSFER PROCESS | en_US |
dc.type | article | en_US |
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