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Isotope Effects in the Predissociation of Excited States of N(2)(+) Produced by Photoionization of (14)N(2) and (15)N(2) at Energies Between 24.2 and 25.6 eV

Photoelectron/photoion imaging spectrometry employing dispersed VUV radiation from the SOLEIL synchrotron has been used to study the predissociation of N(2)(+) states located up to 1.3 eV above the ion's first dissociation limit. Branching ratios for unimolecular decay into either N(2)(+) or N(...

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Detalles Bibliográficos
Autores principales: Hrodmarsson, Helgi R., Thissen, Roland, Dowek, Danielle, Garcia, Gustavo A., Nahon, Laurent, Govers, Thomas R.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Frontiers Media S.A. 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6474291/
https://www.ncbi.nlm.nih.gov/pubmed/31032247
http://dx.doi.org/10.3389/fchem.2019.00222
Descripción
Sumario:Photoelectron/photoion imaging spectrometry employing dispersed VUV radiation from the SOLEIL synchrotron has been used to study the predissociation of N(2)(+) states located up to 1.3 eV above the ion's first dissociation limit. Branching ratios for unimolecular decay into either N(2)(+) or N(+) were obtained by measuring coincidences between threshold electrons and mass-selected product ions, using a supersonic beam of either (14)N(2) or (15)N(2) as photoionization target. The results confirm that predissociation of the [Formula: see text] state of (14)N(2)(+) is faster than emission to the electronic ground-state by a factor 10 or more for all vibrational levels v′ ≥ 3, while for (15)N(2)(+) the two decay modes have comparable probabilities for the levels v′ = 3, 4, and 5. In contrast, no significant isotope effect could be observed for the other states of N(2)(+) identified in the photoelectron spectrum. For both (14)N(2)(+) and (15)N(2)(+) isotopologues all vibrational levels of these other states decay to an extent of at least 95% by predissociation.