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Rapid timescale for an oxic transition during the Great Oxidation Event and the instability of low atmospheric O(2)

The Great Oxidation Event (GOE), arguably the most important event to occur on Earth since the origin of life, marks the time when an oxygen-rich atmosphere first appeared. However, it is not known whether the change was abrupt and permanent or fitful and drawn out over tens or hundreds of millions...

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Autores principales: Wogan, Nicholas F., Catling, David C., Zahnle, Kevin J., Claire, Mark W.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: National Academy of Sciences 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9477391/
https://www.ncbi.nlm.nih.gov/pubmed/36067299
http://dx.doi.org/10.1073/pnas.2205618119
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author Wogan, Nicholas F.
Catling, David C.
Zahnle, Kevin J.
Claire, Mark W.
author_facet Wogan, Nicholas F.
Catling, David C.
Zahnle, Kevin J.
Claire, Mark W.
author_sort Wogan, Nicholas F.
collection PubMed
description The Great Oxidation Event (GOE), arguably the most important event to occur on Earth since the origin of life, marks the time when an oxygen-rich atmosphere first appeared. However, it is not known whether the change was abrupt and permanent or fitful and drawn out over tens or hundreds of millions of years. Here, we developed a one-dimensional time-dependent photochemical model to resolve time-dependent behavior of the chemically unstable transitional atmosphere as it responded to changes in biogenic forcing. When forced with step-wise changes in biogenic fluxes, transitions between anoxic and oxic atmospheres take between only 10(2) and 10(5) y. Results also suggest that O(2) between [Formula: see text] and [Formula: see text] mixing ratio is unstable to plausible atmospheric perturbations. For example, when atmospheres with these O(2) concentrations experience fractional variations in the surface CH(4) flux comparable to those caused by modern Milankovich cycling, oxygen fluctuates between anoxic ([Formula: see text]) and oxic ([Formula: see text]) mixing ratios. Overall, our simulations are consistent with possible geologic evidence of unstable atmospheric O(2), after initial oxygenation, which could occasionally collapse from changes in biospheric or volcanic fluxes. Additionally, modeling favors mid-Proterozoic O(2) exceeding [Formula: see text] to [Formula: see text] mixing ratio; otherwise, O(2) would periodically fall below [Formula: see text] mixing ratio, which would be inconsistent with post-GOE absence of sulfur isotope mass-independent fractionation.
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spelling pubmed-94773912022-09-16 Rapid timescale for an oxic transition during the Great Oxidation Event and the instability of low atmospheric O(2) Wogan, Nicholas F. Catling, David C. Zahnle, Kevin J. Claire, Mark W. Proc Natl Acad Sci U S A Physical Sciences The Great Oxidation Event (GOE), arguably the most important event to occur on Earth since the origin of life, marks the time when an oxygen-rich atmosphere first appeared. However, it is not known whether the change was abrupt and permanent or fitful and drawn out over tens or hundreds of millions of years. Here, we developed a one-dimensional time-dependent photochemical model to resolve time-dependent behavior of the chemically unstable transitional atmosphere as it responded to changes in biogenic forcing. When forced with step-wise changes in biogenic fluxes, transitions between anoxic and oxic atmospheres take between only 10(2) and 10(5) y. Results also suggest that O(2) between [Formula: see text] and [Formula: see text] mixing ratio is unstable to plausible atmospheric perturbations. For example, when atmospheres with these O(2) concentrations experience fractional variations in the surface CH(4) flux comparable to those caused by modern Milankovich cycling, oxygen fluctuates between anoxic ([Formula: see text]) and oxic ([Formula: see text]) mixing ratios. Overall, our simulations are consistent with possible geologic evidence of unstable atmospheric O(2), after initial oxygenation, which could occasionally collapse from changes in biospheric or volcanic fluxes. Additionally, modeling favors mid-Proterozoic O(2) exceeding [Formula: see text] to [Formula: see text] mixing ratio; otherwise, O(2) would periodically fall below [Formula: see text] mixing ratio, which would be inconsistent with post-GOE absence of sulfur isotope mass-independent fractionation. National Academy of Sciences 2022-09-06 2022-09-13 /pmc/articles/PMC9477391/ /pubmed/36067299 http://dx.doi.org/10.1073/pnas.2205618119 Text en Copyright © 2022 the Author(s). Published by PNAS. https://creativecommons.org/licenses/by/4.0/This open access article is distributed under Creative Commons Attribution License 4.0 (CC BY) (https://creativecommons.org/licenses/by/4.0/) .
spellingShingle Physical Sciences
Wogan, Nicholas F.
Catling, David C.
Zahnle, Kevin J.
Claire, Mark W.
Rapid timescale for an oxic transition during the Great Oxidation Event and the instability of low atmospheric O(2)
title Rapid timescale for an oxic transition during the Great Oxidation Event and the instability of low atmospheric O(2)
title_full Rapid timescale for an oxic transition during the Great Oxidation Event and the instability of low atmospheric O(2)
title_fullStr Rapid timescale for an oxic transition during the Great Oxidation Event and the instability of low atmospheric O(2)
title_full_unstemmed Rapid timescale for an oxic transition during the Great Oxidation Event and the instability of low atmospheric O(2)
title_short Rapid timescale for an oxic transition during the Great Oxidation Event and the instability of low atmospheric O(2)
title_sort rapid timescale for an oxic transition during the great oxidation event and the instability of low atmospheric o(2)
topic Physical Sciences
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9477391/
https://www.ncbi.nlm.nih.gov/pubmed/36067299
http://dx.doi.org/10.1073/pnas.2205618119
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