The Paleocene-Eocene thermal maximum (PETM) may represent the best paleo-analog for rapid and massive carbon release to the ocean and atmosphere. Thus, constraining the carbon release rate at its onset is critical. Wright and Schaller (1) use records from apparently rhythmically layered shelf sediments to argue that the layering is annual and that the onset of the carbon isotope excursion (CIE, fingerprint for carbon release) in the surface ocean was complete in 13 y. Using basic carbon cycle and climate considerations, we show this is not feasible. In fact, Wright and Schaller’s isotope records indicate that the CIE onset took at least several millennia. This finding rules out a cometary origin of the carbon release.
For a near instantaneous release of carbon into the atmosphere, the magnitude of the CIE in the surface ocean directly following the release is
where Ms and Mi are the source and initial surface ocean + atmosphere carbon mass and δ’s are isotope compositions (2). Ms = 3,000 Pg (following ref. 1) requires δs ≅ −55‰ to produce the recorded CIE of ∼3‰ in the entire exogenic (surface) carbon reservoir. With initial pCO2 = 1,000 ppmv, δi = −3‰, and Mi = 3,200 Pg, CIEmax ≅ 25‰. A surface ocean CIE of this magnitude would develop on a timescale of decades, before the signal is diluted through mixing with intermediate- and deep-ocean water. We quantify CIEmax mechanistically using the carbon cycle/climate models LOSCAR (Long-term Ocean-atmosphere-Sediment CArbon cycle Reservoir Model) (3) and GENIE (Grid Enabled Integrated Earth System Model) (4), yielding CIEmax ≅ 20–22‰ (Fig. 1A). Hence, if the sediment layering in Wright and Schaller (1) were annual, the measured surface CIE should have exceeded 20‰. This result contrasts the observed ∼3.5‰ at Millville (Fig. 1A).
Fig. 1.
Observed and modeled CIE (A), normalized CIE and climate response (B), and inverse modeling approach (C). Isotope data [Millville, IODP 174AX (1)] are plotted assuming near instantaneous carbon release and a 13-y timescale for the CIE onset as proposed by Wright and Schaller (1) (10-point running mean shown in B). Carbon release in LOSCAR (3), and GENIE model (4) is 3,000 Pg at δ13C = −55‰ over 1 mo in A and B to produce the final recorded 3‰ CIE in the total surface (exogenic) carbon reservoir and to simulate near instantaneous carbon input. All records and model output are normalized to percent response in B; ΔT = model surface temperature anomaly. (C) Diagnosed cumulative carbon emissions to the atmosphere required for a linear ∼3‰ decline in the δ13C of ocean surface dissolved inorganic carbon (black) over 13 y in GENIE (4) for −60‰ (solid) and −22‰ (dashed) carbon sources; resulting mean global sea surface temperature (SST) change shown in red.
The δ18O records of Wright and Schaller (1) are indicative of warming at the PETM onset. Statistical analysis of the Millville δ18O and δ13C records (measured on the same samples) shows zero leads/lags within the data-resolution limit, implying that the full amplitude of surface warming must also have been completed within 13 y. However, the climate system’s inertia (mostly ocean heat capacity) delays surface warming by up to centuries (5). The result is a substantial lag between δ13C and warming as confirmed by our carbon/climate models (Fig. 1B), achieving only ∼50–60% of the final surface temperature anomaly (ΔT) within 13 y. We also forced our model (4) to produce a ∼3‰ CIE over 13 y (inverse approach). However, the associated temperature rise is negligible (Fig. 1C). Hence, a 13-y timescale for the completion of the surface carbon-cycle and climate response, as proposed in Wright and Schaller (1), is impossible, unless the Paleocene ocean’s heat capacity was near zero. Additional model runs show that a minimum timescale of several millennia is required for the PETM onset to eliminate leads/lags between surface CIE and ΔT. Assuming layers are not a drilling artifact, we note that rhythmically layered shelf sediments, in which the layering neither represents primary sediment deposition nor annual deposition, form off modern river deltas, the paleoenvironment of the ancient New Jersey Shelf (6). We see nothing in Wright and Schaller’s (1) measurements to conclude that the PETM onset was completed in 13 y, nor that a cometary impact could have materially contributed to the recorded global CIE.
Footnotes
The authors declare no conflict of interest.
References
- 1.Wright JD, Schaller MF. Evidence for a rapid release of carbon at the Paleocene-Eocene thermal maximum. Proc Natl Acad Sci USA. 2013;110(40):15908–15913. doi: 10.1073/pnas.1309188110. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 2.Dickens GR, O'Neil JR, Rea DK, Owen RM. Dissociation of oceanic methane hydrate as a cause of the carbon isotope excursion at the end of the Paleocene. Paleoceanography. 1995;10(6):965–971. [Google Scholar]
- 3.Zeebe RE. Time-dependent climate sensitivity and the legacy of anthropogenic greenhouse gas emissions. Proc Natl Acad Sci USA. 2013;110(34):13739–13744. doi: 10.1073/pnas.1222843110. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 4.Ridgwell A, Schmidt DN. Past constraints on the vulnerability of marine calcifiers to massive CO2 release. Nat Goesci. 2010;3:196–200. [Google Scholar]
- 5.Hansen J, Sato M, Kharecha P, von Schuckmann K. Earth’s energy imbalance and implications. Atmos Chem Phy. 2011;11:13421–13449. [Google Scholar]
- 6.Wang Z, Saito Y, Hori K, Kitamura A, Chen Z. Yangtze offshore, China: Highly laminated sediments from the transition zone between subaqueous delta and the continental shelf. Estuar Coast Shelf Sci. 2005;62(1):161–168. [Google Scholar]

