Astronomical tunings of the Oligocene–Miocene transition from Pacific Ocean Site U1334 and implications for the carbon cycle

Astronomical tuning of sediment sequences requires both unambiguous cycle pattern recognition in climate proxy records and astronomical solutions, as well as independent information about the phase relationship between these two. Here we present two different astronomically tuned age models for...

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Main Authors: H. M. Beddow, D. Liebrand, D. S. Wilson, F. J. Hilgen, A. Sluijs, B. S. Wade, L. J. Lourens
Format: Article
Language:English
Published: Copernicus Publications 2018-03-01
Series:Climate of the Past
Online Access:https://www.clim-past.net/14/255/2018/cp-14-255-2018.pdf
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spelling doaj-ad856340417d46d985a1a17a952064222020-11-24T22:15:58ZengCopernicus PublicationsClimate of the Past1814-93241814-93322018-03-011425527010.5194/cp-14-255-2018Astronomical tunings of the Oligocene–Miocene transition from Pacific Ocean Site U1334 and implications for the carbon cycleH. M. Beddow0D. Liebrand1D. Liebrand2D. S. Wilson3F. J. Hilgen4A. Sluijs5B. S. Wade6L. J. Lourens7Department of Earth Sciences, Faculty of Geosciences, Utrecht University, Utrecht, the NetherlandsPalaeoClimate.Science, Utrecht (province), the NetherlandsMARUM – Center for Marine Environmental Science, University of Bremen, Bremen, GermanyDepartment of Earth Science, University of California, Santa Barbara, CA, USADepartment of Earth Sciences, Faculty of Geosciences, Utrecht University, Utrecht, the NetherlandsDepartment of Earth Sciences, Faculty of Geosciences, Utrecht University, Utrecht, the NetherlandsDepartment of Earth Sciences, Faculty of Mathematical and Physical Sciences, University College London, Gower Street, London, UKDepartment of Earth Sciences, Faculty of Geosciences, Utrecht University, Utrecht, the NetherlandsAstronomical tuning of sediment sequences requires both unambiguous cycle pattern recognition in climate proxy records and astronomical solutions, as well as independent information about the phase relationship between these two. Here we present two different astronomically tuned age models for the Oligocene–Miocene transition (OMT) from Integrated Ocean Drilling Program Site U1334 (equatorial Pacific Ocean) to assess the effect tuning has on astronomically calibrated ages and the geologic timescale. These alternative age models (roughly from  ∼ 22 to  ∼ 24 Ma) are based on different tunings between proxy records and eccentricity: the first age model is based on an aligning CaCO<sub>3</sub> weight (wt%) to Earth's orbital eccentricity, and the second age model is based on a direct age calibration of benthic foraminiferal stable carbon isotope ratios (<i>δ</i><sup>13</sup>C) to eccentricity. To independently test which tuned age model and associated tuning assumptions are in best agreement with independent ages based on tectonic plate-pair spreading rates, we assign the tuned ages to magnetostratigraphic reversals identified in deep-marine magnetic anomaly profiles. Subsequently, we compute tectonic plate-pair spreading rates based on the tuned ages. The resultant alternative spreading-rate histories indicate that the CaCO<sub>3</sub> tuned age model is most consistent with a conservative assumption of constant, or linearly changing, spreading rates. The CaCO<sub>3</sub> tuned age model thus provides robust ages and durations for polarity chrons C6Bn.1n–C7n.1r, which are not based on astronomical tuning in the latest iteration of the geologic timescale. Furthermore, it provides independent evidence that the relatively large (several 10 000 years) time lags documented in the benthic foraminiferal isotope records relative to orbital eccentricity constitute a real feature of the Oligocene–Miocene climate system and carbon cycle. The age constraints from Site U1334 thus indicate that the delayed responses of the Oligocene–Miocene climate–cryosphere system and (marine) carbon cycle resulted from highly non-linear feedbacks to astronomical forcing.https://www.clim-past.net/14/255/2018/cp-14-255-2018.pdf
collection DOAJ
language English
format Article
sources DOAJ
author H. M. Beddow
D. Liebrand
D. Liebrand
D. S. Wilson
F. J. Hilgen
A. Sluijs
B. S. Wade
L. J. Lourens
spellingShingle H. M. Beddow
D. Liebrand
D. Liebrand
D. S. Wilson
F. J. Hilgen
A. Sluijs
B. S. Wade
L. J. Lourens
Astronomical tunings of the Oligocene–Miocene transition from Pacific Ocean Site U1334 and implications for the carbon cycle
Climate of the Past
author_facet H. M. Beddow
D. Liebrand
D. Liebrand
D. S. Wilson
F. J. Hilgen
A. Sluijs
B. S. Wade
L. J. Lourens
author_sort H. M. Beddow
title Astronomical tunings of the Oligocene–Miocene transition from Pacific Ocean Site U1334 and implications for the carbon cycle
title_short Astronomical tunings of the Oligocene–Miocene transition from Pacific Ocean Site U1334 and implications for the carbon cycle
title_full Astronomical tunings of the Oligocene–Miocene transition from Pacific Ocean Site U1334 and implications for the carbon cycle
title_fullStr Astronomical tunings of the Oligocene–Miocene transition from Pacific Ocean Site U1334 and implications for the carbon cycle
title_full_unstemmed Astronomical tunings of the Oligocene–Miocene transition from Pacific Ocean Site U1334 and implications for the carbon cycle
title_sort astronomical tunings of the oligocene–miocene transition from pacific ocean site u1334 and implications for the carbon cycle
publisher Copernicus Publications
series Climate of the Past
issn 1814-9324
1814-9332
publishDate 2018-03-01
description Astronomical tuning of sediment sequences requires both unambiguous cycle pattern recognition in climate proxy records and astronomical solutions, as well as independent information about the phase relationship between these two. Here we present two different astronomically tuned age models for the Oligocene–Miocene transition (OMT) from Integrated Ocean Drilling Program Site U1334 (equatorial Pacific Ocean) to assess the effect tuning has on astronomically calibrated ages and the geologic timescale. These alternative age models (roughly from  ∼ 22 to  ∼ 24 Ma) are based on different tunings between proxy records and eccentricity: the first age model is based on an aligning CaCO<sub>3</sub> weight (wt%) to Earth's orbital eccentricity, and the second age model is based on a direct age calibration of benthic foraminiferal stable carbon isotope ratios (<i>δ</i><sup>13</sup>C) to eccentricity. To independently test which tuned age model and associated tuning assumptions are in best agreement with independent ages based on tectonic plate-pair spreading rates, we assign the tuned ages to magnetostratigraphic reversals identified in deep-marine magnetic anomaly profiles. Subsequently, we compute tectonic plate-pair spreading rates based on the tuned ages. The resultant alternative spreading-rate histories indicate that the CaCO<sub>3</sub> tuned age model is most consistent with a conservative assumption of constant, or linearly changing, spreading rates. The CaCO<sub>3</sub> tuned age model thus provides robust ages and durations for polarity chrons C6Bn.1n–C7n.1r, which are not based on astronomical tuning in the latest iteration of the geologic timescale. Furthermore, it provides independent evidence that the relatively large (several 10 000 years) time lags documented in the benthic foraminiferal isotope records relative to orbital eccentricity constitute a real feature of the Oligocene–Miocene climate system and carbon cycle. The age constraints from Site U1334 thus indicate that the delayed responses of the Oligocene–Miocene climate–cryosphere system and (marine) carbon cycle resulted from highly non-linear feedbacks to astronomical forcing.
url https://www.clim-past.net/14/255/2018/cp-14-255-2018.pdf
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