The Late Cretaceous ‘greenhouse’ world witnessed a transition from one of the warmest climates of the past 140 million years to cooler conditions, yet still without significant continental ice. Low-latitude sea surface temperature (SST) records are a vital piece of evidence required to unravel the cause of Late Cretaceous cooling, but high-quality data remain illusive. Here, using an organic geochemical palaeothermometer (TEX86), we present a record of SSTs for the Campanian–Maastrichtian interval (~83–66 Ma) from hemipelagic sediments deposited on the western North Atlantic shelf. Our record reveals that the North Atlantic at 35 °N was relatively warm in the earliest Campanian, with maximum SSTs of ~35 °C, but experienced significant cooling (~7 °C) after this to <~28 °C during the Maastrichtian. The overall stratigraphic trend is remarkably similar to records of high-latitude SSTs and bottom-water temperatures, suggesting that the cooling pattern was global rather than regional and, therefore, driven predominantly by declining atmospheric pCO2 levels.
One of the warmest climates of the past 140 million years occurred in the early Late Cretaceous (late Cenomanian—early Turonian, between 95 and 90 Ma)1,2,3,4, with ice-free polar regions5, tropical sea surface temperatures (SSTs) greater than 35 °C (ref. 2) and shallow latitudinal temperature gradients6,7. The interval following this (late Turonian through Maastrichtian, ~90 to 66 Ma) is considered to have been a period of significant global cooling, possibly driven by a combination of declining pCO2 levels and opening ocean gateways1,4,5,8,9. Although general trends in Late Cretaceous climate evolution are relatively well established1,4,5, these inferences are largely based on either bulk fine-fraction carbonate or benthic foraminiferal stable isotope data, representing mixed (fine fraction) or bottom-water temperature records. The rate and structure of Late Cretaceous SST cooling is poorly constrained, as most reconstructions are limited to short, fragmentary and low-stratigraphic-resolution planktonic foraminifera δ18O records6,7,9,10,11. Furthermore, the recognition of early diagenetic recrystallization of planktonic foraminifera at the sea floor, or shortly after burial12, has led to the rejection of many estimates of Cretaceous low-latitude SSTs that were anomalously cool compared with equivalent modern latitudes (the so-called cool tropics paradox). The shortcomings of carbonate-based palaeothermometry can, in some cases, be circumnavigated by using organic palaeotemperature proxies, such as TEX86 (TetraEther indeX of tetraether consisting of 86 carbon atoms)13, which we apply here to a critical, but poorly quantified, interval of climate change—the Campanian–Maastrichtian.
The TEX86 palaeothermometer provides estimates of mean annual SST13, independent of initial seawater chemistry and, compared with carbonate microfossils, is less subject to the modifying effects of diagenesis13. The TEX86 proxy is based on the observed relationship between the ratio of different thaumarchaeotal membrane lipids (tetraether) and the mean annual temperature of the seawater in which the organisms lived13,14,15,16. However, TEX86 is still a relatively new method and development of the proxy is ongoing. For example, recent studies have suggested that TEX86 values may be influenced by archaeotal and thaumarchaeotal biology (taxonomy, diversity changes, physiology, life habitats)15,16,17 and oceanographic setting (for example, water depth), which has led to discussions about how best to apply the temperature calibration in studies of past climate13,14,18,19.
Our samples come from the Shuqualak–Evans borehole in Mississippi (USA) that comprises a ~240 m-thick sequence of shelfal, hemipelagic sediments. Deposition during the Cretaceous occurred at a palaeolatitude of ~35°N20, on a broad shelf bordering the subtropical western North Atlantic to the east and the proto-Caribbean region to the south (Fig. 1). Our age model is based on integrated calcareous nannofossil and planktonic foraminifera datums and indicates rapidly deposited Campanian sediments overlain by a Maastrichtian sequence with slower sedimentation rates (see Methods, Supplementary Table 1 and Supplementary Fig. 1 for a detailed age model description). The succession appears to be stratigraphically complete from the early to late Campanian, whereas the Santonian–Campanian transition and the overlying Maastrichtian sediments are relatively condensed. TEX86 analysis of the Shuqualak–Evans core reveals a significant cooling of ~7 °C during the Campanian, which we compare with records of SSTs from low and high latitudes, and a global compilation of bottom waters. The similarity in long-term trends in these datasets highlights the global nature of late Cretaceous cooling, whilst raising interesting questions regarding the sensitivities of past greenhouse climates to changing boundary conditions such as palaeogeography and atmospheric pCO2.
TEX86 data and SST estimates
TEX86 values from the Shuqualak–Evans borehole decrease from a maximum of 0.90 in the lowermost Campanian to a minimum of 0.70 in the Campanian–Maastrichtian boundary interval (Fig. 2). In the lower Maastrichtian, the TEX86 values rise to 0.75, followed by a decrease to 0.71. In the upper Maastrichtian, values rise again to 0.78. The lower Campanian TEX86 values, in particular, are far higher than those observed in the modern ocean14, implying much higher SSTs in early Campanian times. Different calibrations exist between GDGT (Glycerol Dialkyl Glycerol Tetraether) relative abundances and SST (for example, TEX86, 1/TEX86, TEX86H, TEX86L, pTEX86, BAYSPAR)14,19,21. TEX86H has been widely viewed as the most appropriate calibration for past greenhouse climates and is used here for discussion of our estimates of Cretaceous SSTs, as our measured values of TEX86 are high and the study site is a low-latitude setting14,21. However, the estimates we provide should be considered to be maximum values, as a recent study18 has suggested that TEX86L might be more appropriate than TEX86H at sites where the palaeowater depth was shallower than 1000, m, such as at Shuqualak. The recently developed BAYSPAR method19 yields similar average values to TEX86H, although the uncertainty estimate suggests a wide range of possible values around the average (±~5 to ~8 °C), due to issues related to the regression parameters and extrapolation of the TEX86 proxy19. For completeness, we give SSTs calculated using TEX86L and BAYSPAR in the Supplementary Table 2 and Supplementary Fig. 2 (see Methods). Although the choice of calibration does change the absolute temperature estimates from the Shuqualak–Evans borehole, critically the stratigraphic trends remain the same (Supplementary Fig. 2). The TEX86H calibration indicates maximum SSTs of ~34–36 °C for the earliest Campanian and ~28–29 °C for the Campanian–Maastrichtian transition (Fig. 2). The Maastrichtian SSTs vary between 28° and 31 °C, showing some evidence for warming and cooling events, but these variations are within the statistical error of the TEX86H calibration (±2.5 °C)14, and the magnitude of change in the Maastrichtian should be interpreted with caution.
The maximum TEX86H-based SST estimates of 28–35 °C from the Shuqualak–Evans borehole suggest that Late Cretaceous climate was consistently warmer at ~35 °N than at present (average SSTs at 35 °N in the modern ocean are ~20 °C), and this conclusion is broadly true even using the TEX86L calibration (Supplementary Fig. 2). These estimates of low-latitude SST are consistent with recently published TEX86 data from Israel22, which suggest a range of SSTs from ~23 to 33 °C (using TEX86H) during the Campanian–Maastrichtian at a palaeolatitude of 5° to 15 °N. Compared with the data from Shuqualak–Evans, the data from Israel display a greater range of SSTs and lower maximum values, which may be the result of deposition within an upwelling system. In contrast to these TEX86-based estimates of SSTs, a previous study based on δ18O palaeothermometry of mixed-layer-dwelling planktonic foraminifera from Blake Nose (western North Atlantic ~30 °N palaeolatitude) suggested SSTs of 19–25 °C7, which are equal to, or cooler than, present day SSTs at the equivalent latitude. It has been suggested that early diagenetic recrystallization of planktonic foraminifera could account for some of the lower temperatures reported from the Coniacian–Maastrichtian of Blake Nose7. Comparison with the TEX86 data (using either TEX86H, TEX86L or BAYSPAR) from Shuqualak–Evans lends some support to this explanation for the mid to late Campanian (for example, R. calcarata zone). Furthermore, the highest SSTs we reconstruct (35 °C using TEX86H) are broadly consistent with (sub)tropical temperature estimates from other Mesozoic and Paleogene greenhouse intervals. For example, low- to mid-latitude mid-Cretaceous (Cenomanian–Turonian) and early Paleogene (Eocene) data from exceptionally well-preserved foraminiferal δ18O and TEX86 suggest that SSTs of 33 °C and above were typical in these greenhouse climate regimes23,24,25.
The addition of our new data to existing high-quality Late Cretaceous SST records from the equatorial2,24 and North Atlantic26, South Atlantic6,7, Tanzania12,25 and tropical Pacific27 provides an overview of the spatial and temporal evolution of SSTs for this time interval (Fig. 3 and Supplementary Fig. 3). Although limited by the number of available records, this compilation suggests a very shallow latitudinal temperature gradient during the Turonian, which steepened in the Campanian through Maastrichtian. Similar SSTs at 0° and 35°N in the North Atlantic during the Turonian–earliest Campanian may be due, in part, to the relative isolation and restriction of the basin, which was only connected by shallow and/or restricted gateways to the South Atlantic, Pacific and Tethys oceans at that time. However, the similarity between North Atlantic SSTs and estimates from the southern Tethys22 may suggest that North Atlantic temperatures were not remarkably different from other ocean basins at low latitudes, although, clearly, more good-quality data from the Tethys and Pacific are required to fully validate this hypothesis.
The similarity between Campanian–Maastrichtian low- (this study) and high-latitude6,7 SST trends and the global benthic foraminiferal δ18O record during the Campanian–Maastrichtian4,5 indicates that the Campanian cooling, evident in all datasets, was not solely a high-latitude phenomenon, but represents a global event. This cooling coincided with, and may have been related to, reconfiguration of oceanic gateways28,29 and hence deep, intermediate and shallow ocean circulation4,29,30,31. However, for significant deep- and surface-water cooling to occur across a wide range of latitudes, in both upwelling and non-upwelling settings, we suggest that declining atmospheric pCO2 levels32, possibly due to decreasing ocean crust production33, were the ultimate driver of this long-term climate evolution. The changing tectonic configuration may have led to slight differences in the timing and pattern of change in different regions and water depths, a hypothesis that could be tested with improved age-models for all critical sites and improved estimates of the timing of key tectonic events. The steepening of latitudinal temperature gradients during the Late Cretaceous is consistent with predictions from climate modelling34 that suggest that the latitudinal gradient is strongly dependent on pCO2 levels, with shallower gradients at higher pCO2. Short-term variability in Maastrichtian benthic foraminifera δ18O has previously been interpreted as representing repeated reversals of deep-ocean circulation from low- to high-latitude sources10. However, the existence of broadly synchronous trends in our SST data, and temperature-indicative changes in calcareous nannofossil assemblages8, suggest that the benthic δ18O record may also be responding, ultimately, to changes in climate, possibly driven by pCO2.
Our new data provide a critical addition to the understanding of climate evolution, from extreme warmth during the mid-Cretaceous to the termination of greenhouse conditions at the end of the Eocene. The data demonstrate that the transition from the so-called ‘supergreenhouse’ conditions of the mid-Cretaceous (Aptian–Turonian) to the cooler greenhouse world of the later Cretaceous and early Paleogene, occurred through gradual global cooling, rather than rapid, stepped changes, and that cooling was not confined to high latitudes. A similar transition has also been documented for the Eocene, before the switch to icehouse-mode climates in the Oligocene, albeit with much lower magnitude cooling at low latitudes23,35,36. The long-term cooling trend at high latitudes in the Eocene was likely caused by the opening of the Tasman Gateway during the early to middle Eocene, rather than a simple decrease in atmospheric pCO2 alone, which would have led to more substantial cooling of (sub)equatorial surface waters than is observed36. It has been suggested that, during the late Eocene, declining pCO2 levels eventually crossed a critical threshold (of ~750 p.p.m.) at the Eocene/Oligocene (E/O) boundary, which allowed the rapid growth of the Antarctic ice sheet and a stepped climate change into an icehouse state37,38,39. Why, then, did significant continental ice-sheet growth occur at the E/O boundary, but not during the late Cretaceous, given the cooler Late Campanian and Maastrichtian water temperatures (surface and deep) and cooling at both high and subequatorial latitudes5? Proxy reconstructions and models do not provide an unambiguous picture of the temporal evolution of Late Cretaceous–early Paleogene atmospheric pCO2 levels and trends40, although, overall, the latest Cretaceous appears to have been characterized by lower pCO2 levels than the mid-Cretaceous. It is therefore unclear whether the absence of continental scale glaciation was because pCO2 did not fall sufficiently far, or because the pCO2 threshold limit for ice-sheet growth was lower during the Late Cretaceous compared with the Eocene, due to different baseline conditions, such as ocean gateway configurations. Modelling of the E/O boundary event37 suggests that open tectonic gateways around Antarctica are not necessarily required for initiation of continental scale glaciation, but they can exert a control on the amount of pCO2 decline needed for glaciation. In the case of the E/O boundary, modelling suggests that, for major glaciation to occur with a closed Drake Passage, the pCO2 threshold would be ~140 p.p.m. lower than in a scenario with the Drake Passage open. During the Late Cretaceous, both the Drake Passage and the Tasman Gateway were closed and, thus, it is likely that the threshold for glaciation was <~600 p.p.m.V. Understanding why a major ice sheet was not initiated in the Late Cretaceous during an interval of marked global cooling, given some superficial similarities to Eocene climate trends and absolute values, is an intriguing challenge, which, if addressed through additional data and modelling, could provide valuable insights into the long-term controls on cryosphere development during greenhouse and ‘doubthouse’ conditions, climate sensitivity to changing pCO2, and the plausibility of glacioeustatic sea-level change during the Late Cretaceous and Early Paleogene.
Core location and palaeogeography
The Shuqualak–Evans core is from Shuqualak, Mississippi, USA (32°58′49′′N, 88°34′8′′W) and was sampled for TEX86 from a depth of 9.45 m down to 251.46 m, spanning the Santonian/Campanian boundary interval through to the uppermost Maastrichtian.
Figure 1 shows a model of the palaeogeographic evolution of North America during the latest Cretaceous. In these reconstructions and others (for example, ref. 20) the Shuqualak–Evans borehole was situated on a broad shelf bordering the North Atlantic Ocean and Gulf of Mexico during the latest Cretaceous. Surface ocean circulation reconstructions (summarized in ref. 31) suggest that this location was likely not influenced by waters of the Western Interior Seaway and this is supported by calcareous nannofossil assemblage components and abundances, which suggest an open ocean water mass.
Biostratigraphy and age-model
The age-model for the Shuqualak–Evans core is based on integrated calcareous nannofossil41 and planktonic foraminifera42 biostratigraphic datums (Supplementary Fig. 1 and Supplementary Table 1), with calibrated absolute ages taken from Gradstein et al.42 For the uppermost Campanian through Maastrichtian (25.91–9.45 m), the age model is calculated as a linear function, with tie points at base Lithraphidites quadratus (16.76 m, 69.18 Ma42) and base Micula prinsii (12.80 m, 67.30 Ma42). This suggests a low sedimentation rate of ~2.1 m per Myr ago. We assign a minimum age of 66 Ma to the shallowest sample (9.45 m), as the nannofossils indicate a Cretaceous age yet the age-model predicts a Palaeocene age and we cannot further refine the age-model above 12.80 m, which appears to be topmost Maastrichtian. For most of the Campanian (245.36–30.48 m), the age-model is a linear function, with tie points at base Broinsonia parca subsp. constricta (239.27 m, 81.38 Ma42) and base Uniplanarius sissinghii (134.11 m, 77.61 Ma42). This indicates a high sedimentation rate of ~27.9 m per Myr. For the lowermost sample analysed for geochemistry, the age model is constrained by base Broinsonia parca subsp. parca (245.36 m, 81.43 Ma42) and the presence of Arkhangelskiella cymbiformis (252.83 m, assigned maximum age of 83.20 Ma42), indicating a low sedimentation rate of ~4.2 m per Myr ago. Note that the co-occurrence of Dicarinella asymetrica and A. cymbiformis (at 251.46 m) suggests that the age of the lowermost sample analysed for TEX86 is around the Santonian/Campanian boundary interval. The TEX86 and SST data are given in relation to the sample depths in Supplementary Fig. 2 and Supplementary Table 2.
GDGT extraction and analysis
Samples were solvent extracted using the technique previously published by Schouten et al.13,43 Approximately 6 g powdered sample was ultrasonically extracted using one time methanol, three times dichloromethane (DCM)/methanol (1:1, v/v) and three times DCM. All extracts were combined and dried under a continuous N2 flow at 40 °C. Any water remaining in the samples was removed by passing the extracts (dissolved in DCM/methanol (3:1, v/v)) over a column containing anhydrous Na2SO4. Extracts were split into polar and apolar fractions by column chromatography, using hexane/DCM (9:1, v/v) and DCM/methanol (1:1, v/v) sequentially as the eluents and Al2O3 as the stationary phase. The polar extract containing the targeted GDGTs was dissolved in hexane/propanol (99:1, v/v) and then filtered through a PTFE (polytetrafluoroethylene) 0.45 μm filter. After drying down, the samples were redissolved in a certain volume of hexane/propanol (99:1, v/v), which depends on the weight of each polar fraction. All 48 samples were analysed in the Department of Earth Sciences at UCL on an Agilent 1200 series HPLC attached to a G6130A single-quadrupole mass spectrometer. The analytical protocol followed is as described in Schouten et al.43. The abundance of both isoprenoid and branched GDGTs was measured in selective ion monitoring mode. Ion peaks of the respective GDGTs were integrated to determine the relative abundance of each molecule in the sample. These abundances were then used to determine the TEX86, TEX86H (GDGT-index 2), and TEX86L (GDGT-index 1) indices13,14. These indices are defined as follows:
SST calculations from GDGT abundances
To calculate SSTs, we used the following equations from Kim et al.14 which are based upon a comprehensive modern core-top dataset:
At temperatures >15 °C expected during greenhouse periods in Earth history, it has been recommended14 that the TEX86H index should be used, as both indices should yield the same estimate of SST according to the modern core-top calibration dataset, but TEX86H has an associated calibration error that is significantly lower (±2.5 °C) compared with that of TEX86L (±4 °C). However, application of TEX86L and TEX86H to datasets from Early Cenozoic sediments21 has revealed that they do not always yield the same estimates of SST, with TEX86L generally yielding lower temperatures. At high-latitude Palaeocene–Eocene sites in New Zealand, Hollis et al.21 found that TEX86L yielded SST estimates more comparable to inorganic proxies (δ18O, Mg/Ca) than TEX86H, but suggested that, at low latitudes and high TEX86 values, TEX86H might be as appropriate. In their analysis of the ability of the different GDGT-based proxies to replicate inorganic SST estimates, Hollis et al.21 noted that, at high TEX86 values above 0.70, the over-estimation of SST is less than 5 °C using TEX86H. Furthermore, at TEX86 values above 0.75, they suggested that TEX86L underestimates SST. The oxygen-isotopic compositions of well-preserved planktonic foraminifera of Cenomanian–Santonian age from Demerara Rise (~5 °N palaeolatitude) yield SSTs typically in the range of 35 to >37 °C24, comparable to SSTs derived by TEX86H of 35 to 37 °C from the same site (recalculated by us from the published TEX86 data). Therefore, through the consideration of previous suggestions and multiproxy records of low-latitude mid-Cretaceous SSTs, it would initially appear that the TEX86H calibration represents the best estimate of SSTs for the Shuqualak–Evans borehole. Furthermore, in order to be able to compare our new data with previously published Late Cretaceous TEX86 data2,24, from which TEX86L values are not yet available, we have had to use the TEX86H index in Fig. 3. Nonetheless, in Supplementary Figs 2 and 3 we show both the TEX86H and TEX86L data (where possible) and the calculated SSTs to illustrate the potential range of values. We also present in Supplementary Fig. 2 SSTs calculated using the recently developed BAYSPAR approach19. The BAYSPAR model considers how the relationship between TEX86 and temperature varies spatially and considers uncertainties in the modern SST-TEX86 relationship. Critically, the stratigraphic trends for Shuqualak–Evans are near identical, irrespective of which proxy is used and, thus, our conclusions regarding the temporal evolution of the direction of Late Cretaceous climatic and latitudinal gradient change remains valid, even if absolute values are harder to constrain.
Recent work, based on an analysis of modern water-column GDGT abundance profiles, the core-top calibration dataset and a compiled Paleogene dataset, suggests that TEX86H may be less appropriate than TEX86L for use at sites where the water depth was approximately shallower than 1000, m (such as Shuqualak). This is likely due to variations in the export dynamics of individual GDGT compounds with depth, and an apparent temperature/water depth bias in the core-top calibration dataset18. In both the modern core-top calibration dataset and the Paleogene dataset, sites deposited in <1,000 m of water exhibit low GDGT-2/GDGT-3 (/) ratios and high offsets between SSTs calculated by TEX86H and TEX86L (ΔH-L). We have been able to obtain the raw GDGT data for the sites on Demerara Rise, which were thought to have been deposited at water depths of <1500, m44. The GDGTs from these sites exhibit low / ratios and high ΔH-L, which Taylor et al.18 suggest is characteristic of water depths <1,000 m. We therefore contend that it is appropriate in Supplementary Fig. 3 to compare Demerara Rise and Shuqualak–Evans using either TEX86H or TEX86L (as the water depth of all sites was likely about, or shallower than, 1000, m). The application of the TEX86L calibration to our data from Shuqualak–Evans suggests SSTs of ~28 °C for the earliest Campanian and ~20 °C for the Campanian–Maastrichtian transition, which are some ~7–8 °C lower than the estimates of the TEX86H model, and much closer to modern SSTs at comparable latitudes, which perhaps is surprising given that Late Cretaceous pCO2 levels are thought to have been higher than present (~600 to 800 p.p.m. versus 280 p.p.m. for the preindustrial modern)40. Furthermore, the use of TEX86L suggests almost no temperature gradient between 5° and 60° absolute palaeolatitude during the Turonian–Santonian, which also seems unlikely. The issue of how best to calculate temperatures from GDGT data is ongoing and it may be that a calibration based on suspended particulate organic matter may overcome some of the issues described above16,18.
Repeated analysis of an in-house standard and selected samples suggest that analytical reproducibility of TEX86 is better than ±0.009, in line with previous studies45 that suggest an analytical error for TEX86 index of ±0.01. In our data, we estimate that the error on SST estimates associated with analytical precision is <±0.4 °C for the TEX86H calibration, and <±0.6 °C using TEX86L. Analytical error is far less than the standard error associated with the core-top calibrations, which for TEX86H is ±2.5 °C, and for the TEX86L calibration is ±4.0 °C21.
BIT and MI indices
The GDGTs analysed for the TEX86 palaeotemperature proxy are mainly produced by marine thaumarchaeota. However, the same GDGTs are also produced by terrestrial soil organisms and methanotrophs.
GDGTs of terrestrial origin can be washed into the marine realm by rivers, potentially biasing SST reconstructions. Apart from isoprenoid GDGTs, which are used for the TEX86 techniques, terrestrial organisms also produce branched GDGTs46. Branched GDGTs are typical of terrestrial organisms, but they do not occur among marine thaumarchaeota46. Thus, the branched GDGTs are used to quantify the terrestrial GDGT contamination in marine sediment samples by calculating the Branched and Isoprenoid Tetraether (BIT) index46. The BIT index is based on the ratio of branched GDGTs to the isoprenoid GDGT crenarchaeol46. In our study, the measurement of these branched GDGTs was included in the analytical protocol. There is no significant relationship between BIT and TEX86 in our data (Supplementary Fig. 4) and the BIT index is between 0.05 and 0.15 (Supplementary Fig. 2). This is well below the recommended threshold of 0.2, above which soil microbial contamination may be problematic47. Thus the SST estimates made in this study are probably not altered by an influence of terrestrial GDGTs.
GDGTs produced by methanotrophs within the sediments can distort the TEX86 signal and lead to erroneous estimates of palaeotemperature. The degree of influence of methanotropic archaea can be estimated using the Methane Index (MI)17. Normal marine sediments have values <0.3, whereas sediments influenced by high rates of methane production have values >0.5. The interval from 0.3 to 0.5 marks the transition between the two environments17. The MI values from Shuqualak vary from ~0.1 to 0.25 (Supplementary Fig. 2), suggesting normal marine conditions and a lack of GDGT production by methanotrophs. We therefore conclude that methanotrophic production of GDGTs has not impacted adversely on our TEX86 records.
Palaeotemperatures from foraminiferal oxygen isotopes
In Fig. 3 and Supplementary Fig. 3, we show estimates of palaeotemperature based upon the oxygen-isotopic (δ18O) composition of a global compilation of benthic foraminiferal data4, selected low-latitude planktonic foraminiferal datasets12,25 and mixed-layer-dwelling planktonic foraminifera from southern high-latitude sites (DSDP Site 511 and ODP Site 690)6,7. Calcareous dinoflagellate cysts from ODP Site 690 have similar d18O values to planktic foraminifera48 but are not included as a suitable temperature calibration for Cretaceous dinoflagellates is not available. Note for the Turonian-age samples from Tanzania, we have recalculated the SST range using the typical range of planktonic δ18O values measured (−4 to −5 ‰)25. In order to apply a consistent approach to calculating temperatures from δ18O of foraminiferal calcite, we have recalculated temperatures from the original published oxygen-isotopic datasets. We used equation (6) to calculate temperatures49:
where T=temperature (°C), δcc=δ18O of foraminiferal calcite (‰, VPDB) and δw=δ18O of ambient seawater.
We used a δw value of −1.27, which includes a correction of −0.27 for the conversion of Vienna Standard Mean Ocean Water to Vienna PeeDee Belemnite and an ice volume value of −1‰. For calculation of SSTs from planktonic foraminifera, we applied an additional latitudinal salinity correction50 to δw, using the palaeolatitudes of DSDP Site 511 and ODP Site 690 in the Late Cretaceous (58°S and 67°S, respectively) and equation (7):
where x=absolute palaeolatitude between 0° and 70°. Palaeolatitudinal positions for each site were using the ODSN Plate reconstruction software ( http://www.odsn.de/odsn/services/paleomap/paleomap.html).
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We gratefully acknowledge funding from the German Science Foundation (DFG Research Stipend Li 2177/1-1 to C.L.), a Royal Society (UK) URF (S.A.R.), a NERC (UK) grant (J.A.L.), a NERC (UK) studentship (K.L.), The Curry Fund of UCL (C.L.), the Cushman Foundation for Foraminiferal Research (J.M. Resig Fellowship to F.F.) and the Spanish Ministerio de Ciencia e Innovación project CGL2011-22912, co-financed by the European Regional Development Fund (I.P.-R., J.A.A., J.A.L.). We thank T. Dunkley-Jones and J. Young for assistance in collecting the samples and S. Schouten for providing TEX86L data from Demerara Rise. This paper is dedicated to Ernie Russell, who sadly died after submission of the manuscript.
The authors declare no competing financial interests.
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Linnert, C., Robinson, S., Lees, J. et al. Evidence for global cooling in the Late Cretaceous. Nat Commun 5, 4194 (2014). https://doi.org/10.1038/ncomms5194
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