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Threshold Photoelectron Spectroscopy of IO and HOI

Iodine oxides appear as reactive intermediates in atmospheric chemistry. Here, we investigate IO and HOI by mass‐selective threshold photoelectron spectroscopy (ms‐TPES), using synchrotron radiation. IO and HOI are generated by photolyzing iodine in the presence of ozone. For both molecules, accurat...

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Autores principales: Schleier, Domenik, Reusch, Engelbert, Lummel, Lisa, Hemberger, Patrick, Fischer, Ingo
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6790590/
https://www.ncbi.nlm.nih.gov/pubmed/31508875
http://dx.doi.org/10.1002/cphc.201900813
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author Schleier, Domenik
Reusch, Engelbert
Lummel, Lisa
Hemberger, Patrick
Fischer, Ingo
author_facet Schleier, Domenik
Reusch, Engelbert
Lummel, Lisa
Hemberger, Patrick
Fischer, Ingo
author_sort Schleier, Domenik
collection PubMed
description Iodine oxides appear as reactive intermediates in atmospheric chemistry. Here, we investigate IO and HOI by mass‐selective threshold photoelectron spectroscopy (ms‐TPES), using synchrotron radiation. IO and HOI are generated by photolyzing iodine in the presence of ozone. For both molecules, accurate ionization energies are determined, 9.71±0.02 eV for IO and 9.79±0.02 eV for HOI. The strong spin‐spin interaction in the (3)Σ(−) ground state of IO(+) leads to an energy splitting into the Ω=0 and Ω=±1 sublevels. Upon ionization, the I−O bond shortens significantly in both molecules; thus, a vibrational progression, assigned to the I−O stretch, is apparent in both spectra.
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spelling pubmed-67905902019-10-18 Threshold Photoelectron Spectroscopy of IO and HOI Schleier, Domenik Reusch, Engelbert Lummel, Lisa Hemberger, Patrick Fischer, Ingo Chemphyschem Communications Iodine oxides appear as reactive intermediates in atmospheric chemistry. Here, we investigate IO and HOI by mass‐selective threshold photoelectron spectroscopy (ms‐TPES), using synchrotron radiation. IO and HOI are generated by photolyzing iodine in the presence of ozone. For both molecules, accurate ionization energies are determined, 9.71±0.02 eV for IO and 9.79±0.02 eV for HOI. The strong spin‐spin interaction in the (3)Σ(−) ground state of IO(+) leads to an energy splitting into the Ω=0 and Ω=±1 sublevels. Upon ionization, the I−O bond shortens significantly in both molecules; thus, a vibrational progression, assigned to the I−O stretch, is apparent in both spectra. John Wiley and Sons Inc. 2019-09-11 2019-10-02 /pmc/articles/PMC6790590/ /pubmed/31508875 http://dx.doi.org/10.1002/cphc.201900813 Text en © 2019 The Authors. Published by Wiley-VCH Verlag GmbH & Co. KGaA. This is an open access article under the terms of the http://creativecommons.org/licenses/by-nc/4.0/ License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited and is not used for commercial purposes.
spellingShingle Communications
Schleier, Domenik
Reusch, Engelbert
Lummel, Lisa
Hemberger, Patrick
Fischer, Ingo
Threshold Photoelectron Spectroscopy of IO and HOI
title Threshold Photoelectron Spectroscopy of IO and HOI
title_full Threshold Photoelectron Spectroscopy of IO and HOI
title_fullStr Threshold Photoelectron Spectroscopy of IO and HOI
title_full_unstemmed Threshold Photoelectron Spectroscopy of IO and HOI
title_short Threshold Photoelectron Spectroscopy of IO and HOI
title_sort threshold photoelectron spectroscopy of io and hoi
topic Communications
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6790590/
https://www.ncbi.nlm.nih.gov/pubmed/31508875
http://dx.doi.org/10.1002/cphc.201900813
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