High Energy States of Ozone Obtained from New Ab Initio Potential Energy Surfaces and from Experimental Spectra Analyses: the “Reef Structure” Puzzle
Authors/Creators
- 1. Harvard-Smithsonian Center for Astrophysics Atomic and Molecular Physics Division Cambridge MA 02138, USA; Laboratory of Quantum Mechanics of Molecules and Radiative Processes, Tomsk State University, 36 Lenin Avenue, 634050 Tomsk, Russia
- 2. Groupe de Spectrométrie Moléculaire et Atmosphérique, UMR CNRS 7331, BP 1039, F-51687, Reims Cedex 2, France
- 3. Laboratory of Theoretical Spectroscopy, V. E. Zuev Institute of Atmospheric Optics, 1 Academician Zuev square, 634055 Tomsk, Russia; Laboratory of Quantum Mechanics of Molecules and Radiative Processes, Tomsk State University, 36 Lenin Avenue, 634050 Tomsk, Russia
- 4. Laboratoire Interdisciplinaire de Physique, Université de Grenoble 140 Avenue de la Physique BP 87 38402 Saint Martin d'Hères, France
- 5. Institute of Chemistry , Eötvös Loránd University, Pázmány Péter sétány 1/A, 1117 Budapest, Hungary
Description
High-energy states of ozone 16O3 and 18O3 isotopologues were predicted from a new ab initio potential energy surface1 and derived from experimental spectra analysis up to 7920 cm−1. A brief outline is given for highly accurate ab initio2 calculations and for new analytical PES modeling. The new analytical PES of ozone takes into account such structural properties of ozone as non-linear minimum energy path and non-additivity of the fragmentation energy. The ”reef structure” (activation barrier) problem is investigated as well as its influence on the shifting of harmonic frequencies and vibrational energy levels of ozone. Correction of ab initio data was made by accounting for the couplings of many excited electronic states3. It is shown that this correction leads to a smoother PES with the ”reef structure” almost vanishing. The PES ”without reef structure” appears to be more precise in terms of spectroscopy: vibration energies are in good agreement with available experimental data4,5,6 up to 94% of the dissociation energy with an average error of vibrational prediction near 1 cm−1, which is much better than all available calculations that involve the activation barrier on the transition state.
Notes
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PI_9_Kochanov.pdf
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Additional details
References
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