The Early Jurassic (late Pliensbachian to early Toarcian) was a period marked by extinctions, climate fluctuations, and oceanic anoxia. Although the causes of the early Toarcian Oceanic Anoxia Event (OAE) have been fairly well studied, the events that lead to the Toarcian OAE, i.e. the events in the late Pliensbachian, have not been well constrained. Scenarios of the driving mechanism of biotic and environmental changes of the late Pliensbachian have ranged from LIP volcanism (the Karoo-Ferrar LIP), ocean stagnation, and changing ocean circulation, to orbital forcing. The temporal relationship between the Karoo LIP and the late Pliensbachian (Kunae-Carlottense ammonite Zones) are investigated in an effort to evaluate a causal relationship. We present the first absolute timescale on the Kunae and Carlottense Zones based on precise high-precision U-Pb geochronology, and additional geochemical proxies, for a range of environmental proxies such as bulk organic carbon isotope compositions, Hg concentration, and Hg/TOC ratios, and Re-Os isotopes to further explore their causal relationship. The data presented here show that causality between the Karoo LIP and the late Pliensbachian events cannot be maintained.
The Early Jurassic (Pliensbachian-Toarcian) was a period marked by recurrent biotic crises and environmental change. In the late Pliensbachian, there is compelling evidence that significant biotic and climatic changes took place1,2,3,4. For instance, a series of minor extinction events have been recorded in the Margaritatus Zone, at the Subnodosus, Gibbosus Subzones, and in the Spinatum Zone at the Hawskerense Subzone with extinctions happening at the species level (90–70%) in North-western European localities2,5. The same events have been reported in their correlative ammonite zones in North America, i.e., Kunae and Carlottense Zones, respectively1,6, highlighting the global extent of these extinction events. The carbon isotope record of the late Pliensbachian displays significant shifts, with a prominent positive shift below the Margaritatus-Spinatum boundary3,7 known as the late Pliensbachian event (LPE). This shift has been recognized in the carbonate carbon4, bulk organic carbon3,8,9, and terrestrial organic carbon3,8. Furthermore, important periods of production and preservation of organic matter (OM) take place in the late Pliensbachian, with potential evidence for an oceanic anoxic event (OAE)10. However, the causes of the extinction crisis and environmental changes are still conjectural. Because the events of the late Pliensbachian immediately precede the much larger early Toarcian OAE there has been speculation that the events of the late Pliensbachian might also be driven by the same magmatic event5,6,11,12,13. Due to the contrasting environmental conditions between the late Pliensbachian and the Toarcian OAE, the volcanic release of S-bearing aerosols has been evoked as the driving mechanism of the cool climatic conditions at this time4,12,14. However, definitive evidence for the occurrence of enhanced volcanism during the late Pliensbachian is still missing. Therefore, investigating the temporal relationship between the late Pliensbachian events and the Karoo-Ferrar LIP magmatism is crucial for potentially unravelling the causes of the climate fluctuations of this time. Lastly, the palaeoenvironmental changes of the late Pliensbachian have yet to be reported outside of the Western Tethys marine environments, which prevents a conclusive appreciation of the global effect of these environmental disturbances.
This paper aims to reconstruct the palaeoenvironmental changes of the late Pliensbachian outside of Western Tethys to evaluate the possible global extent of the climatic fluctuations and to test their temporal relation to LIP volcanism. To this aim, we have investigated the Nicely and Suplee Formations in the Izee-Suplee basin of the Blue Mountains terranes, East Oregon, USA15,16, an organic rich-mudstone series that spans the lower Kunae Zone to uppermost Carlottense Zone. High-precision U-Pb ages are presented to evaluate the temporal relation to LIP volcanism, in addition to bulk δ13Corg, TOC, Rock Eval data, and Hg/TOC chemostratigraphy. Using these proxies for various environmental factors, we establish a precise timeline of environmental changes in the late Pliensbachian.
Stratigraphic framework and ammonite biostratigraphy
Four sections were sampled: St. Clair, Sterrett, Rosebud, and Garden of Concretions (Fig. 1). These sections include the Suplee, and Nicely Formations and the base of the Hyde Fm., in the Izee terrane, OR, USA (FS. 1 Supplementary Information S.I). The stratigraphic thickness of the Suplee, Nicely and Hyde Fm sections are 14 m, 77 m, and 4 m, respectively. Ammonoids occur throughout the Suplee and Nicely Formations17,18 and encompass much of late Pliensbachian (Domerian). Two North American zones are recognized for that interval, the Kunae and Carlottense Zones (Fig. 1)19. Range charts giving the stratigraphic distribution of the ammonoids are provided in the SI.
U-Pb geochronology and age-depth modelling
A total of ten ash beds were dated; SC1T = 184.02 ± 0.05/0.07/0.21 Ma, MSWD = 1.2, n = 7; WS13T = 184.36 ± 0.07/0.08/0.21 Ma, MSWD = 0.76, n = 4; SC11T = 184.55 ± 0.04/0.06/0.21 Ma, MSWD = 1.4, n = 5; SC19T = 185.18 ± 0.07/0.08/0.21 Ma, MSWD = 2.8, n = 3; SC24T = 183.92 ± 0.06/0.10/0.22, MSWD = 0.32, n = 5; SC28T = 185.47 ± 0.04/0.06/0.21 Ma, MSWD = 1.3, n = 4; SC_47T = 186.52 ± 0.16/0.17/0.26 Ma, MSWD = 0.53, n = 5; Rb_50 = 186.71 ± 0.06/0.08/0.21 Ma, MSWD = 1.2, n = 3, SC57T = 186.82 ± 0.04/0.06/0.21 Ma, MSWD = 0.52, n = 5, Rb_22 = 186.96 ± 0.07/0.10/0.22 Ma, MSWD = 0.67, n = 4 (FS. 2). Only one of the ten ash beds (SC24T 183.92 ± 0.06/0.10/0.22 Ma) yielding consistently younger U-Pb data that violated the stratigraphic superposition was excluded from the Bayesian age-depth model. We interpreted the date as being affected by Pb-loss. All Th-corrected 206Pb/238U ages are presented in FS. 2, and the raw data can be found in TS.1 (SI). The age-depth envelope with a 95% confidence interval can be found in Fig. 1 and age for every 10 cm of the stratigraphic record can be found in TS.2 (SI).
Bulk organic carbon isotopes
Three trends in the organic carbon isotope record have been recognized (Fig. 2, raw data in TS.3). In the lower Kunae Zone, the δ13Corg values decrease from −27.5 to −30.5‰ (Segment I), representing a −3.0‰ shift. In the middle-upper Kunae Zone, start a positive trend from −29.5 to −28.0‰. This shift lasts from the middle-upper Kunae Zone to the lower Carlottense Zone (Fig. 2; segment II). During the trend towards higher δ13Corg values, at the uppermost Kunae Zone, around the Kunae-Carlottense boundary, there is a short negative excursion to −31‰. After the positive trend, the δ13Corg values begin to become lower again; however, due to the 10-metre gap in the sedimentary record of the St. Clair, the trend is not so apparent although δ13Corg reach values of −30‰ (Fig. 2). The δ13Corg values from the Suplee Fm. and in the lower Nicely Fm. seem to display a fairly consistent trend. In the upper Nicely Fm., δ13Corg values are somewhat scattered.
Re-Os isotope data
Samples from the lower Nicely Fm. show Re concentrations between 8.92 and 71.59 ppb, with the most Re-rich sample in the middle of the sequence (Fig. 2, data in TS.4). Osmium concentration varies to a lesser degree, between 240 and 552 ppt, resulting in 187Re/188Os ratios between 117 and 1737. Measured 187Os/188Os varies between 1.97 and 4.31 across the sequence. Initial 187Os/188Os values at 186.5 Ma are around 2 for the majority of samples, with some outliers to both higher and lower values (Fig. 2). One sample yields negative initial 187Os/188Os, suggesting the addition of Re. While concentrations for both Os and Re are comparable to values observed in other black shale suites in the late Sinemurian-early Pliensbachian (Robin Hood’s Bay, Yorkshire, UK20), the calculated initial 187Os/188Os values are notably more radiogenic (187Os/188Os of ~2 vs. 0.2–0.4).
Rock Eval data
The variation of Rock Eval data with stratigraphic depth is plotted in Fig. 2, and other plots in FS. 4 and FS. 5 (data in TS.3). In the lower to middle Nicely Fm., TOC values increase steadily from 0.5% to 2.0%. Likewise, HI ranges from 27 to 50 mg HC/g TOC. The OI values show an inverse correlation with HI values and decrease from 150 to 60 mg CO2/g TOC. Around the Carlottense-Kunae boundary (~40 m of stratigraphic height) a sharp increase in TOC values reaches 4%, with a sharp increase in HI values to 50–228 mg HC/g TOC and a S2 peak reaching values > 4 mg HC/g, and a sharp decrease in OI values reaching 50 mg CO2/g TOC. Subsequently, TOC decreases to values close to 0% and so do HI values at 50–60 mg HC/g TOC. S2 peaks (the amount of hydrocarbons associated with kerogen) shift to values below 2 mg HC/g, and OI values increase, reaching values of 150–200 mg CO2/g TOC. Total organic carbon values increase again to close to 2%, HI values continue low ca. 50 mg HC/g TOC, S2 peaks cluster ca. 1 mg HC/g, OI values cluster ca. 100 mgCO2/gTOC. In the upper Nicely Fm., TOC values are scattered varying from 1 to 3%. Both HI and OI values are low clustering around 50–80 mg HC/g TOC and 50–80 mg CO2/g TOC, respectively. Tmax values are high in the lowermost Nicely Fm. with values between 460–470 °C. For the middle to upper Nicely Fm. Tmax values stay within the 444–460 °C range with some minor exceptions.
Mercury concentrations were measured on selected samples (Fig. 2, data in TS.3). Mercury was normalized with TOC values from Rock Eval pyrolysis. An anomaly in Hg concentration is found at the lower Kunae Zone, with values reaching over 2 ppm. This spike in Hg concentration shows a positive covariance between the spike and the Hg/TOC values reaching beyond 2 (ppm/%). From the middle-upper Kunae Zone to the lower Carlottense Zone Hg and Hg/TOC values are considered background levels (Fig. 2). The second spike in Hg concentration is in the middle of the Carlottense Zone, with Hg concentrations reaching 0.5 ppm. The spike is not as prominent as that of the first spike; however, a positive covariance with Hg/TOC ratios is also observed with ratios reaching 0.25 (ppm/%).
The global carbon isotope record of the late Pliensbachian
To interpret our δ13Corg curve, we compared it with four other published carbon isotope curves for the same time interval. Here we attempt to build a global understanding of the carbon isotope fluctuations for the late Pliensbachian to potentially validate the environmental changes of the interval on a global scale. The δ13Corg record of the Nicely and Suplee Formations display several trends through the Kunae and Carlottense Zones that are very similar to those of the Western Tethys sections. In the lower Kunae Zone, the δ13Corg shift from −27.5 to −30.5‰, represents a −3.0‰ change (Fig. 3). In Europe, this negative shift is observed in the lower-middle Margaritatus Zone in the Staithes section and in the Paris Basin21 in the lower Subnodosus Subzone.
In the middle-upper Kunae Zone values have a range between −28.5 to −29.5‰, following a positive trend until the lower Carlottense Zone. In the Robin Hood’s Bay locality3, the shift occurs in the upper of the Margaritatus Zone at the Gibbosus-Subnodosus boundary, where it was named the “Late Pliensbachian event”3 (LPE), and is also reproduced in the Staithes locality8. The excursion is not reproduced in the Paris Basin21 at the same ammonite level. This location does, however, show a positive excursion at the upper Subnodosus Subzone and into the lower Gibbosus Subzone, which we interpret to be equivalent and attribute the small mismatch to possibly the resolution of ammonite data available. In the Peniche section4, Portugal, we suggest that the positive excursion spanning the upper Margaritatus and lower Spinatum would be correlative to both positive excursions at the same age as here. During this positive trend, at the uppermost Kunae Zone, just before the Kunae-Carlottense boundary, there is a short negative excursion; with δ13Corg values that reach −30 to −31‰. We tentatively interpret this excursion to be correlated to a small shift in the carbon isotope record from the Staithes section8 (Fig. 3), however, limited to a single data point. Neither in the Paris basin nor the Peniche section is this short negative excursion recognized.
In the middle of the Carlottense Zone, the carbon isotope values become more negative, and we correlate this negative trend as the negative trend in the lower to middle Spinatum Zone8. In the Paris Basin, we correlate this negative trend to be equivalent to the negative trend in the middle-upper Spinatum Zone. In the Peniche section, the values are fairly scattered in the upper Spinatum Zone but show an overall negative trend in the values. In summary, we argue that our carbon isotope curve from the middle Kunae to the uppermost Carlottense Zone does show similarities with other carbon isotope curves from North-western European sections. Nevertheless, the global extent of these variations is still debatable since in carbon isotope curves from other localities14,22 these fluctuations are not observed in the late Pliensbachian. Although, the absence of such carbon isotope fluctuations might be related to localised effects or reveal the incompleteness of the stratigraphic record, at least for some of these localities.
Our chemostratigraphic data display several important changes throughout the Kunae and Carlottense Zones (Figs. 2 & 3). In the lower Kunae Zone, there is a negative −3.0‰ shift in δ13Corg (Segment I; Fig. 2), and a coeval anomaly in the Hg concentrations and Hg/TOC. High Hg contents in marine sediments have been used to link environmental change and biotic crises to LIP activity in at least four cases in the Phanerozoic13,23,24,25,26,27. Additionally, the highly radiogenic 187Os/188Os(i) values during the negative organic carbon excursion (N-CIE) (Fig. 2) indicate increased weathering of the continental crust, which has been attributed to the occurrence of LIP activity28,29. The OM deposited during the N-CIE has high Tmax values > 460 °C, suggesting that the OM is over-mature. This suggests that burial overprint could have affected our geochemical proxies in this interval (Segment I). In fact, the S2 peaks (<0.5 mgHC/g) and TOC values (<0.5 mgHC/g) are low, but this could indicate either diagenetic overprint of the HI values as well as poor preservation of OM, e.g. in well-oxygenated bottom waters30,31. Recognizing one from the other is often difficult. Despite that, the overall Tmax values from the Nicely Fm. are usually above 440 °C even for parts of the Nicely Fm that have high TOC and S2 peaks, which would indicate that post-depositional processes have affected the OM to some extent (FS. 4 & FS. 5). For instance, the large Hg/TOC spikes might be biased due to the low TOC values as a result of diagenetic overprint. Consequently, the HI and OI are, at least during the N-CIE, not reliable to infer on the nature of the OM because the TOC is too low. However, the isotopic composition of bulk organic carbon is not affected by hydrocarbon maturation or even low-grade metamorphism32,33. Therefore, there is no evidence to suggest that the N-CIE shift observed in the lower Kunae, or our δ13Corg dataset as whole, is the product of alteration. In terms of Re-Os systematics, when compared to other Early Jurassic sediment suites, the lower Nicely Fm. samples are comparable to other reported organic-rich mudstones28,34,35,36 with the exception of their very radiogenic 187Os/188Os values. Hydrocarbon maturation does not affect the isotopic system37, and substantial loss of ~45–80% of Re through hydrocarbon migration would be required to achieve initial 187Os/188Os typical for Jurassic seawater; which is considered unlikely given the high Re and Os concentrations measured (TS. 4). Thus, the unusually radiogenic initial 187Os/188Os values are unlikely to be the result of secondary processes.
Even though the link between the N-CIE and LIP is plausible geochemically, from a geochronological perspective, the connection seems problematic. The negative excursion is bracketed between 186.74 ± 0.06 Ma to 185.94 ± 0.39 Ma, deduced from our age model (Fig. 1). Our absolute timescale for the late Pliensbachian is compatible with a U-Pb high-precision age in the Kunae Zone at 185.49 ± 0.16 Ma in Canada28. A possible causal relationship between the Karoo-Ferrar LIP and the late Pliensbachian carbon cycle disturbance has been suggested based on the Ar-Ar chronometer1,38, and based on our temporal timescale for the late Pliensbachian the link is possible. However, biotic crises and environmental change in the Phanerozoic operate on a timescale that is significantly shorter than the analytical uncertainty produced by the Ar-Ar systematics. On average, the analytical precision of 40Ar/39Ar ages at 2σ is in the order of 1–2%, which for the Early Jurassic produces ages with ± 1.5–3.0 Ma resulting in an apparent long lifespan for the Karoo LIP of over 10 Myr11. Conversely, U-Pb high-precision geochronology has routinely produced ages at 0.1–0.05% precision. The use of a precisely calibrated EARTHTIME 202Pb-205Pb-238U-235U tracer solution39,40, improved error propagation algorithms41,42, the shift to single grains analysis, lowering of laboratory blanks, have all contributed to the successfulness of the technique43. As a result, high-precision U-Pb geochronology has shown that biotic crises and environmental change occur at 104-105 year timescale and constrains the lifespan of the most notorious Phanerozoic LIPs between 500–800 kyr44,45,46,47,48. Therefore, 40Ar/39Ar ages have not been successful in yielding sufficient temporal resolution to adequately assess causality between LIPs and biotic and environmental crises, and the link is often left elusive. This has been the case in at least all five major mass extinctions events in the Phanerozoic49. In the case of the N-CIE in the lower Kunae Zone, the excursion is 3.5 Myr older than the oldest known occurrence of the Karoo-Ferrar LIP, i.e., the New Amalfi Sheet at 183.243 ± 0.045 Ma44 (Fig. 4). Therefore, the lack of temporally coeval volcanic rocks of the Karoo-Ferrar LIP or other LIP to the N-CIE and Hg enrichment in the lower Kunae precludes any link to large scale volcanism as a driving mechanism.
Although the use of Hg/TOC as a geochemical proxy for LIP activity in the marine record has shown considerable promise in linking LIPs and some biotic crises and environmental change13,23,25,26,27, the link continues to be tenuous. The long-term enrichment of Hg in the marine environment is possible by other pathways than solely via oxidation of volcanic Hg0 delivered via rainfall. Volcanic Hg is readily absorbed and accumulated into the terrestrial reservoir (biomass and soils) and is a viable source of recycled Hg into the marine environment during environmental changes24,50. Furthermore, Hg/TOC as a geochemical proxy for LIP activity has only been successful in only a small number of cases. Percival et al.51 have shown that 187Os/188Os(i) is much more consistently recording the effect of LIP volcanism than Hg/TOC in the marine record. Therefore, our geochemical evidence would indeed suggest LIP activity, although which LIP is still unknown. Oceanic hydrothermal activity input has been shown to enrich Hg in the marine record52,53; however, this scenario would be unlikely based on our highly radiogenic187Os/188Os(i) data (Fig. 2).
Similar scenarios where marine Hg enrichment has no clear temporal connection to LIP activity are found in other cases in the Phanerozoic. In the Frasnian-Famennian biotic crisis, for instance, there is evidence for marine Hg enrichment54 and a global warming event55, but a temporal connection to any LIP activity is unclear and remains speculative. Moreover, astronomically forced climate change has proven successful in explaining the environmental change during the Frasnian-Famennian biotic crisis56. To explain the N-CIE and Hg/TOC spike in the lower Kunae Zone, a similar driving mechanism might be proposed. For instance, orbitally forced environmental change has been postulated to potentially destabilize the cryosphere, which can become an important source of isotopically light carbon to the atmosphere-ocean system57. The increased pCO2 would trigger global warming and enhanced continental run-off, which potentially erodes large areas of organic-rich sediments or wetlands58. These could have also been a viable source of isotopically light carbon to the atmosphere-ocean system50 as well as a source of remobilized terrestrial Hg24,50 and radiogenic Os28,29,36 to the marine environment. Furthermore, induced global warming could also trigger the dissociation of methane-hydrates from continental margin sediments, which could have also contributed as a source of isotopically light carbon59. This scenario would explain the geochemical evidence from the lower Kunae Zone without the need to evoke LIP volcanism.
Subsequent to the negative excursion in the lower Kunae Zone, our geochemical data include a positive trend in the δ13Corg, here interpreted to be correlative to the LPE (Segment II; Fig. 2). Our geochemical data allows the trend towards higher δ13Corg values to be further subdivided into three distinct periods with respect to the nature of OM being deposited. The first period (185.94 ± 0.40 Ma to 185.35 ± 0.14 Ma) is characterised; by the deposition of terrestrial OM (type III) with TOC values increasing from 0.8–2.0%. Period II (185.35 ± 0.14 Ma to 185.18 ± 0.07 Ma) characterised; by a mixture of type II and type III OM with perhaps an increase of type II OM (HI values > 200 HC/g TOC; OI values < 50 mgCO2/TOC) (Fig. 2) with an increase of TOC occurring around the Kunae-Carlottense boundary. During the upper Kunae and lower Carlottense Zone, we have better confidence in characterising; the OM deposited because TOC values (2–4 wt%) and S2 peak values (1–8 mgHC/g) are higher (Fig. 2) although still low when compared, for instance, to Toarcian OAE black shales31. Period III (185.18 ± 0.07 Ma to 184.92 ± 0.24 Ma) is characterised; by the deposition of type III OM and TOC values of < 2%. Period III (185.18 ± 0.07 Ma to 184.92 ± 0.24 Ma) is characterised; by the deposition on type III OM and TOC values also of <2%.
Overall, the OM from the Nicely Fm. is predominantly type III, with a small part being type II (Period II Fig. 2 & FS. 4,A/B; FS. 5). Furthermore, our characterisation; of the OM from the Nicely Fm. as predominantly type III OM is in agreement with other studies that report Rock Eval pyrolysis data from the Spinatum and Margaritatus Zones from western Tethys31,60,61,62,63 (FS. 5). Tmax values for LPE are higher than in North-western European sections, which suggest that the OM is mature to over-mature (FS. 4C/D; FS. 5) and confirms a degree of alteration has affected the OM in the Nicely Fm. Even though secondary processes have, to some degree, affected the HI in the Nicely Fm., hydrocarbon migration has potentially left a more refractory OM residue, i.e., type III OM. Therefore, it follows that the variations in the carbon-isotope record from the Nicely Fm. are not the result of the mixing of different OM end-members with different carbon isotopic composition, but rather are mainly a variation in the δ13Corg of terrestrial OM reservoir. Therefore, the fluctuations potentially reflect changes in the global carbon reservoir at the Earth’s surface. In Western Tethys sections, the LPE positive δ13C shift has been suggested to have affected the global carbon cycle3,4,14,64,65. The coeval deposition of dark shales with high TOC values just below the Margaritatus-Spinatum boundary (at the Gibbosus-Subnodosus boundary) in European sections (Fig. 3), and now in North America (around the Kunae-Carlottense boundary, ca. 185.2 Ma; Fig. 2), provides further evidence that the positive δ13C trend of the LPE is potentially global. The preservation and production of organic carbon in several late Pliensbachian marine sections suggest that a minor OAE possibly took place during the LPE3,4,8,10, or at least during period II (185.35 ± 0.14 Ma to 185.18 ± 0.07 Ma Ma) where potentially a higher proportion of type II in the bulk OM is preserved (Fig. 2). However, the apparent coeval accumulation of organic-rich rocks below the Margaritatus-Spinatum boundary does not necessarily imply widespread oceanic anoxia. Alternatively, enhanced productivity in surface waters, coupled with a high sedimentation rate could result in the deposition and preservation of OM without resulting in an OAE. Furthermore, evidence for the preservation of terrestrial OM over marine OM during the late Pliensbachian (FS. 5) certainly favours this scenario, i.e., oceanic anoxia was not as severe to the degree at which marine OM would be preserved globally. Therefore, the existence of an OAE during this time is still conjectural.
Many palaeoclimatic studies in the Early Jurassic predict low temperatures in the upper Margaritatus Zone and into the Spinatum Zone3,4,66,67,68,69,70 (Fig. 4) of which the causes have been suggested to be the result of the Karoo-Ferrar LIP emplacement1,6,11. Large scale volcanism is believed to lower global temperatures via the protracted volcanic degassing of SO2 and the rapid conversion to sulphate aerosols71,72,73. From our data set, no connection to LIP volcanism can thus be established. During the LPE, Hg and Hg/TOC return to background levels, and from a temporal perspective, a causal connection to the Karoo-Ferrar LIP would be unlikely (Fig. 4) as the event is still ca.1.5 Myr older than the Karoo-Ferrar LIP. In the absence of a clear connection to the occurrence of a LIP, the degassing of SO2 sourced from LIPs is unlikely to be the process responsible for the cool and dry climates of the LPE.
In the middle of the Carlottense Zone (Segment III, Fig. 2) δ13Corg values show a N-CIE starting at 184.92 ± 0.24 Ma to 184.51 ± 0.09 Ma, with TOC values ranging from 1% to close to 2%, and the coincident increase in the Hg concentrations and Hg/TOC ratios. The Hg/TOC ratios range from 0.15 to 0.50 ppm/%, which is comparable to the Hg/TOC spikes during the Toarcian OAE13. Unfortunately, the Os isotopic composition of the Nicely Fm. was not obtained in this segment; therefore, a link to volcanism of the Karoo-Ferrar LIP is tenuous; additionally, from a geochronological perspective the link is also not substantiated (Fig. 4).
In Segment IV, the δ13Corg indicates a negative shift towards the Pliensbachian-Toarcian boundary, which appears to agree with the global carbon isotopic trend towards the Pliensbachian-Toarcian (Pl-To) boundary13. However, our geochemical record in the uppermost Pliensbachian is not continuous enough and does not allow any discussion on the events that take place at Pl-To boundary.
The late Pliensbachian has been considered as a period of protracted cool and dry climate3,4,70,74. However, our detailed proxies for environmental factors support the hypothesis that pulsed and contrasting climatic conditions operated during the late Pliensbachian, with potential warm periods evident in the lower Margaritatus Zone and cooler climates around the Margaritatus-Spinatum boundary and into the Spinatum Zone10,14. Our organic geochemical proxies for the LPE, for the first time outside of the Western Tethys realm, provide further evidence for the global deposition of organic-rich rocks below the Margaritatus-Spinatum boundary. However, conclusive evidence for an OAE during the LPE is still lacking. The driving mechanisms for these environmental changes in the late Pliensbachian have been speculated to be the result of volcanism1,4,6,10,11,12, ocean stagnation74, changing ocean circulation70, and orbital climate forcing57. Here we have shown that LIP volcanism is an unlikely candidate for the driving mechanism since no LIP is known to occur between ca. 187–184 Ma. A causal link to the Karoo-Ferrar LIP has been suggested based on 40Ar/39Ar ages1,6,11; however, the low accuracy and analytical precision of the methodology hinders a more precise connection. As a result, based on high-precision U-Pb geochronology, the degassing of volcanic S-species (SO2) inducing an ice-house climate12,72,75, for instance, is an unlikely driving mechanism of the cool and dry climate of late Pliensbachian. The Hg/TOC spikes throughout the late Pliensbachian adds to the growing body of evidence showing that prominent deviations of the marine Hg/TOC record alone cannot be readily used as a proxy for LIP activity and is better when combined with high-precision U-Pb geochronology to accurately and precisely evaluate temporal relationship to LIPs. Finally, it has long been speculated that the events of both the late Pliensbachian and the early Toarcian were biotic and climatic responses to the same underlying driving mechanism; i.e. the emplacement of the Karoo-Ferrar LIP. Each of their contrasting climate conditions have been thought as being regulated by different stages of volcanic degassing of the Karoo-Ferrar LIP (e.g. CO2 vs SO2)4,6. However, our geochronological data effectively decouples the driving mechanisms of climate change between the late Pliensbachian (Kunae-Carlottense Zones) and early Toarcian as being separate and unrelated.
Stratigraphic sampling and sample processing
In the field, sections and beds were measured using a metre; stick, and numbered consecutively. The outcrops were cleaned with a brush, altered/weathered samples removed with the aim of collecting fresh samples when possible. Samples for geochemistry were collected every 30–50 cm (on average) of all stratigraphic sections with the exception of the Garden of Concretions. Ash beds were collected, whenever present. Samples for geochemical analysis were powered using an agate mill. Ash beds were processed using a tungsten mill, zircons separated by gravitational floating methods in water, magnetic separation and heavy liquid density separation.
The geochronological method of choice was U-Pb zircon CA-ID-TIMS because yields 206Pb/238U dates at 0.1–0.05% precision. The depositional age of ash beds was calculated from the weighted means of the youngest overlapping 206Pb/238U dates (FS 3), assuming that the youngest subset of grains are a meaningful age for the depositional age of the ash bed and that older grains record prolonged residence of zircon in the magmatic systems as well as intramagmatic recycling. In the text, all quoted ages of ash beds are weighted mean 206Pb/238U ages corrected for initial 230Th disequilibrium. General chemical abrasion procedures followed the ones described in79 modified after80. Grains were handpicked and selected for annealing at 900 °C for 48 hours. Grains from each individual sample were chemically abraded for 12 hours in 3 ml Teflon beakers at 210 °C with 12 N HF inside a pressure dissolution vessel. Following chemical abrasion, the grains were then placed inside 3 ml Teflon beakers rinsed and cleaned. Grains were cleaned 6.2 N HCl and 7 N HNO3 inside 3 ml Savillex beaker at 80 °C on a hot plate. Total dissolution was done in microcapsules in 12 N HF for 48 hours at 210 °C and spiked using the EARTHTIME 202Pb-205Pb-235U-233U and EARTHTIME 205Pb-235U-233U tracer solutions. Conversion to chloride was done by using 6.2 N HCl for 12 hours at 180 °C in the pressure dissolution vessels. 3.1 N HCl was added to the microcapsules before eluting Pb and U using micro columns. The micro columns were first cleaned using four steps alternating 6.2 N HCl and ultrapure H2O. Samples were collected in 7 ml Savillex beakers. Data acquisition was done at the Department of Earth Sciences, University of Geneva, Switzerland, using a Thermo Scientific Triton thermal ionisation; mass spectrometer. Each measured ratio was corrected for fractionation using a 202Pb/205Pb of 0.99989 when the 202Pb-205Pb-235U-233U and EARTHTIME was used. When EARTHTIME 205Pb-235U-233U was used Pb fractionation was assumed to be 0.13 ± 0.5% a.m.u (2σ). All common Pb measured was assumed to be from laboratory blank. Uranium was measured as UO2+ in static mode on Faraday cups equipped with 1012 Ω resistors. Auto focusing and peak centring was performed at the beginning of every block, with each block consisting of 20 cycles each. Baselines were monitored on ± 0.5 mass units. 238U/235U of the sample and blank was assumed to be 137.818 ± 0.045 (2σ)81. The oxide correction in U measurements was assumed 16OU/18OU = 0.00241. Uranium decay constant values were used from82,83. Raw U-Pb data was reduced using U-Pb Redux and Tripoli42 and the data reported in TS.1. Uncertainty and error propagation algorithm used in Redux software is described in41. Uncertainties are reported as X/Y/Z; X includes analytical uncertainty, Y includes additional tracer (ET2535or ET535) calibration uncertainty, and Z includes additional 238U decay constant uncertainty.
Bayesian age-depth modelling
In order to assign absolute numerical ages of palaeontological markers, biostratigraphic zone boundaries, to estimate the duration of carbon isotopic fluctuations, and of sedimentation rates, Bayesian statistical interpolation was used using the Bchron package in R studio84,85. An age-depth model has been calculated with a 95% confidence uncertainty envelope for every designated stratigraphic depth (10 cm) within the sedimentary column. The model relies on some fundamental assumptions: (1) the subset of U-Pb dates from selected grains as well as their uncertainties are normally distributed, (2) the principle of stratigraphic superposition is not violated. The model assumes that sediment accumulation rate is a random process which implies piecewise monotonic sediment accumulation paths between two dated horizons. These sediments accumulation paths are considered to have Poisson distribution and the thickness of sediment accumulation a gamma distribution. This approach allows for sedimentations rates to vary, in contrast to linear interpolation that considers sedimentations rates to be constant.
To present a statistically valid interpretation of our geochemical data, we fitted the geochemical data points by using a spline-regression model in R Studio. Since the geochemical data appear to have been affected by secondary processes, the main goal of the spline-fitting model is to distinguish between the true geochemical signals from the noise in the data set generated by secondary processes. The model considers each data point as random and normally distributed variables, rather than absolute values. The regression curve should not be understood as the absolute values of the geochemical parameter over time, but rather a main trend in the geochemical data. The code was written and made available for free by Prof. Albert Y. Kim, from the Smith College, MA, USA. The code can be found in the Supplementary Information as well as Prof. Albert Y. Kim’s personal GitHub webpage: https://gist.github.com/rudeboybert/752f7aa1e42faa2174822dd29bfaf959 (last access: 12.01.2019)
Carbon isotope analysis
The whole-rock powdered samples were decarbonated using 10% HCl acids, weighed 300–500 microgram per sample, and placed in tin microcapsules. The carbon isotope composition of organic matter was determined by flash combustion on a Carlo Erba 1108 elemental analyser connected to a Thermo Fisher Scientific Delta V Plus (Bremen, Germany) isotope ratio mass spectrometer that was operated in the continuous helium flow mode via a Conflo III split interface. The stable carbon isotope compositions were reported in the delta (δ) notation as the per mil (‰) deviations of the isotope ratio relative to Vienna Pee Dee Belemnite limestone (VPDB) standard (δ13Corg value in ‰ vs. VPDB). The repeatability and intermediate precision of the δ13Corg analyses, determined by the standard deviation of replicated analyses of laboratory organic standards and unknown samples, were better than 0.1‰ (1 SD). The accuracy of the analyses was checked periodically by analyses of the international reference materials (USGS-24 graphite, IAEA-PEF1 polyethylene foil, and NBS-22 oil).
Rock Eval pyrolysis
Characterisation; of the organic matter was measured using whole-rock powders on a Rock Eval 6 pyrolysis at the University of Lausanne. Analysed samples weighed 100 to 150 mg. Pyrolysis consists of stepwise heating from 25 °C to 500 °C at a rate of 25 °C/minute. During heating a release of CO and CO2 is monitored and graphed by S1, S2, and S3 peaks. S1 peaks are acquired from 25 °C to 300 °C, when hydrocarbon as generated. S2 peaks are monitored from 300 °C to 500 °C representing the sum of all hydrocarbons, and the hydrocarbon potential, and related the amount of hydrogen within the organic matter. The temperature recorded at the peak of S2 is the Tmax. S3 peaks were monitored from 300–390 °C and monitor the amount of CO and CO2 being released and relate to the amount of oxygen within the Organic matter. Total Organic content (TOC) is calculated in percent per weight, based the total amount of all carbon components released as pyrolized carbon and residual carbon. Hydrogen Index (HI) (HI, mg HC /g TOC, where HC is hydrocarbons), Oxygen Index (OI, mg CO2/g TOC). An in-depth overview of the methodology can be seen in86.
Mercury analyses were done by atomic absorption spectrometry designed for Hg analysis on the Zeeman R-915F at the University of Lausanne. Analyses were made by thermal evaporation of whole-rock powdered samples not previously treated. To ensure accuracy, precision, and reproducibility of each measurement the same sample was run at least twice and an average mean value was calculated per sample.
Re-Os isotopic analysis
Approximately 0.5 g of finely powdered sample was mixed with a 185Re-190Os tracer solution in a borosilicate Carius tube. After addition of 4 ml 2 M H2SO4, the Carius tube was frozen in a dry ice/2-propanol mixture. Prior to sealing, 4 ml of 2 M H2SO4 containing 0.2 g/g dissolved CrO3 was added. Samples were digested at 200 °C overnight. Osmium: Carius Tubes tubes were refrozen in a dry ice/2-propanol mixture for opening. Osmium was extracted following a procedure modified after87, using a liquid/liquid extraction with CHCl3, followed by back extraction into 9 M HBr. The samples were taken to dryness, followed by micro-distillation of the Os88. For measurement by N-TIMS, samples were loaded onto 99.999% Pt wire (Materion) with a saturated Ba(OH)2 in 0.1 M NaOH solution as activator. Samples were measured at the National Centre for Isotope Geochemistry (NCIG) at University College Dublin on a ThermoScientific Triton as OsO3–89,90. Measurements were performed on the SEM in peak-hopping mode. Interferences of 187ReO3 on 187OsO3 were monitored with 185ReO3 and corrected for. Oxygen corrections were performed using 17O/16O of 0.0003709 and 18O/16O of 0.002044991. Mass fractionation was corrected using 192Os/188Os of 3.08392. Long-term reproducibility of measurements was monitored by repeated measurements of the Durham Romil Os Standard solution (DROsS), which yielded a 187Os/188Os value of 0.16091 ± 0.00016 (n = 56), in good agreement with results from other laboratories (0.160924 ± 0.00000493, Durham University; 0.16078 ± 0.0002494, University of Alberta). A blank processed alongside the samples for this study yielded 109 fg of Os with a 187Os/188Os of 0.26. Rhenium: The remainder of the sample was taken to dryness, and redissolved in 15 ml of 5 M NaOH solution. Rhenium was extracted in 15 ml of acetone95. After drydown of the acetone, Re was purified over anion resin columns (AG1-X8, 200-400 mesh). Measurements were performed on the Thermo Scientific Neptune at NCIG, using a SIS glass spray chamber. Solutions were doped with W, and mass bias was corrected using a 184W/186W of 1.0777. Rhenium standard solutions were run at the beginning and end of the analytical session, and additional mass bias corrections were carried out for a 185Re/187Re value of 0.5974. All corrections were minor. The total Re blank processed alongside the samples was 65 pg.
All the raw data can be found in the Supplementary Information.
Caruthers, A. H., Smith, P. L. & Grocke, D. R. The Pliensbachian-Toarcian (Early Jurassic) extinction: A North American perspective. In Volcanism, Impacts, and Mass Extinctions: Causes and Effects: Geological Society of AmericaSpecial Paper 505 225–243, https://doi.org/10.1130/2014.2505(11) (2014).
Dera, G., Neige, P., Dommergues, J. L. & Brayard, A. Ammonite paleobiogeography during the Pliensbachian-Toarcian crisis (Early Jurassic) reflecting paleoclimate, eustasy, and extinctions. Glob. Planet. Change78, 92–105 (2011).
Korte, C. & Hesselbo, S. P. Shallow marine carbon and oxygen isotope and elemental records indicate icehouse-greenhouse cycles during the Early Jurassic. Paleoceanography26, 2011–2160 (2011).
Suan, G. et al. Secular environmental precursors to Early Toarcian (Jurassic) extreme climate changes. Earth Planet. Sci. Lett.290, 448–458 (2010).
Dera, G. et al. High-resolution dynamics of Early Jurassic marine extinctions: the case of Pliensbachian-Toarcian ammonites (Cephalopoda). J. Geol. Soc. London.167, 21–33 (2010).
Caruthers, A. H., Smith, P. L. & Gröcke, D. R. The Pliensbachian-Toarcian (Early Jurassic) extinction, a global multi-phased event. Palaeogeogr. Palaeoclimatol. Palaeoecol.386, 104–118 (2013).
Gómez, J. J., Comas-Rengifo, M. J. & Goy, A. Palaeoclimatic oscillations in the Pliensbachian (Early Jurassic) of the Asturian Basin (Northern Spain). Clim. Past12, 1199–1214 (2016).
Ruhl, M. et al. Astronomical constraints on the duration of the Early Jurassic Pliensbachian Stage and global climatic fluctuations. Earth Planet. Sci. Lett.455, 149–165 (2016).
Jenkyns, H. C. & Clayton, C. J. Lower Jurassic epicontinental carbonates and mudstones from England and Wales: Chemostratigraphic signals and the early Toarcian anoxic event. Sedimentology44, 687–706 (1997).
Silva, R. L. & Duarte, L. V. Organic matter production and preservation in the Lusitanian Basin (Portugal) and Pliensbachian climatic hot snaps. Glob. Planet. Change131, 24–34 (2015).
Jourdan, F., Féraud, G., Bertrand, H., Watkeys, M. K. & Renne, P. R. The 40 Ar/ 39 Ar ages of the sill complex of the Karoo large igneous province: Implications for the Pliensbachian-Toarcian climate change. Geochemistry, Geophys. Geosystems9, 1–20 (2008).
Guex, J. et al. Thermal erosion of cratonic lithosphere as a potential trigger for mass-extinction. Sci. Rep.6, 1–9 (2016).
Percival, L. M. E. et al. Globally enhanced mercury deposition during the end-Pliensbachian extinction and Toarcian OAE: A link to the Karoo–Ferrar Large Igneous Province. Earth Planet. Sci. Lett.428, 267–280 (2015).
Silva, R. L., Duarte, L. V., Comas-Rengifo, M. J., Mendonça Filho, J. G. & Azerêdo, A. C. Update of the carbon and oxygen isotopic records of the Early-Late Pliensbachian (Early Jurassic, ~187Ma): Insights from the organic-rich hemipelagic series of the Lusitanian Basin (Portugal). Chem. Geol.283, 177–184 (2011).
Dorsey, R. J. & LaMaskin, T. A. Stratigraphic record of Triassic-Jurassic collisional tectonics in the Blue Mountains province, northern Oregon. Am. J. Sci.307, 1167–1193 (2007).
LaMaskin, T. A., Vervoort, J. D., Dorsey, R. J. & Wright, J. E. Early Mesozoic paleogeography and tectonic evolution of the western United States: Insights from detrital zircon U-Pb geochronology, Blue Mountains Province, northeastern Oregon. Bull. Geol. Soc. Am.123, 1939–1965 (2011).
Dickinson, W. R. & Vigrass, L. W. Geology of the Suplee-Izee area, Crook, Grant, and Harney Counties, Oregon. State Oregon Dep. Geol. Miner. Ind. Bull.58, 109 (1965).
Imlay, R. W. Lower Jurassic (Pliensbachian and Toarcian) ammonites from eastern Oregon and California. United States Geol. Surv. Prof. Pap. C1–C51 (1968).
Smith, P. L., Tipper, H. W., Taylor, D. G. & Guex, J. An ammonite zonation for the Lower Jurassic of Canada and the United States: the Pliensbachian. Can. J. Earth Sci.25, 1503–1523 (1988).
Porter, S. J., Selby, D., Suzuki, K. & Gröcke, D. Opening of a trans-Pangaean marine corridor during the Early Jurassic: Insights from osmium isotopes across the Sinemurian–Pliensbachian GSSP, Robin Hood’s Bay, UK. Palaeogeogr. Palaeoclimatol. Palaeoecol.375, 50–58 (2013).
Peti, L. et al. Sinemurian–Pliensbachian calcareous nannofossil biostratigraphy and organic carbon isotope stratigraphy in the Paris Basin: Calibration to the ammonite biozonation of NW Europe. Palaeogeogr. Palaeoclimatol. Palaeoecol.468, 142–161 (2017).
Them, T. R. et al. High-resolution carbon isotope records of the Toarcian Oceanic Anoxic Event (Early Jurassic) from North America and implications for the global drivers of the Toarcian carbon cycle. Earth Planet. Sci. Lett.459, 118–126 (2017).
Grasby, S. E., Beauchamp, B., Bond, D. P. G., Wignall, P. B. & Sanei, H. Mercury anomalies associated with three extinction events (Capitanian Crisis, Latest Permian Extinction and the Smithian/Spathian Extinction) in NW Pangea. Geol. Mag.153, 285–297 (2016).
Grasby, S. E. et al. Isotopic signatures of mercury contamination in latest Permian oceans. Geology45, 55–58 (2017).
Sanei, H., Grasby, S. E. & Beauchamp, B. Latest Permian mercury anomalies. Geology40, 63–66 (2012).
Percival, L. M. E. et al. Mercury evidence for pulsed volcanism during the end-Triassic mass extinction. Proc. Natl. Acad. Sci.114, 7929–7934 (2017).
Thibodeau, A. M. et al. Mercury anomalies and the timing of biotic recovery following the end-Triassic mass extinction. Nat. Commun.7, 11147 (2016).
Them, T. R. et al. Evidence for rapid weathering response to climatic warming during the Toarcian Oceanic Anoxic Event. Sci. Rep.7, 1–10 (2017).
Percival, L. M. E. et al. Osmium isotope evidence for two pulses of increased continental weathering linked to Early Jurassic volcanism and climate change. Geology44, 759–762 (2016).
Meyers, P. A. Organic geochemical proxies of paleoceanographic, paleolimnologic, and paleoclimatic processes. Org. Geochem.27, 213–250 (1997).
Fantasia, A., Föllmi, K. B., Adatte, T., Spangenberg, J. & Mattioli, E. Expression of the Toarcian Oceanic Anoxic Event: New insights from a Swiss transect. Sedimentology66, 262–284 (2019).
Spangenberg, J. E. & Macko, S. A. Organic geochemistry of the San Vicente zinc–lead district, eastern Pucará Basin, Peru. Chem. Geol.146, 1–23 (1998).
Spangenberg, J. E. & Frimmel, H. E. Basin-internal derivation of hydrocarbons in the Witwatersrand Basin, South Africa: evidence from bulk and molecular δ13C data. Chem. Geol.173, 339–355 (2001).
Cohen, A. S., Coe, A. L., Bartlett, J. M. & Hawkesworth, C. J. Precise Re–Os ages of organic-rich mudrocks and the Os isotope composition of Jurassic seawater. Earth Planet. Sci. Lett.167, 159–173 (1999).
Cohen, A. S. The rhenium–osmium isotope system: applications to geochronological and palaeoenvironmental problems. J. Geol. Soc. London161, 729–734 (2004).
Cohen, A. S. & Coe, A. L. New geochemical evidence for the onset of volcanism in the Central Atlantic magmatic province and environmental change at the Triassic-Jurassic boundary. Geology30, 267–270 (2002).
Creaser, R. A., Sannigrahi, P., Chacko, T. & Selby, D. Further evaluation of the Re-Os geochronometer in organic-rich sedimentary rocks: a test of hydrocarbon maturation effects in the Exshaw Formation, Western Canada Sedimentary Basin. Geochim. Cosmochim. Acta66, 3441–3452 (2002).
Jourdan, F. et al. 40Ar/39Ar ages of CAMP in North America: Implications for the Triassic–Jurassic boundary and the 40K decay constant bias. Lithos110, 167–180 (2009).
Condon, D. J., Schoene, B., McLean, N. M., Bowring, S. A. & Parrish, R. R. Metrology and traceability of U–Pb isotope dilution geochronology (EARTHTIME Tracer Calibration Part I). Geochim. Cosmochim. Acta164, 464–480 (2015).
McLean, N. M., Condon, D. J., Schoene, B. & Bowring, S. A. Evaluating uncertainties in the calibration of isotopic reference materials and multi-element isotopic tracers (EARTHTIME Tracer Calibration Part II). Geochim. Cosmochim. Acta164, 481–501 (2015).
McLean, N. M., Bowring, J. F. & Bowring, S. A. An algorithm for U-Pb isotope dilution data reduction and uncertainty propagation. Geochemistry, Geophys. Geosystems12, 1–26 (2011).
Bowring, J. F., McLean, N. M. & Bowring, S. A. Engineering cyber infrastructure for U-Pb geochronology: Tripoli and U-Pb_Redux. Geochemistry, Geophys. Geosystems12, 1–19 (2011).
Ovtcharova, M. et al. Developing a strategy for accurate definition of a geological boundary through radio-isotopic and biochronological dating: The Early–Middle Triassic boundary (South China). Earth-Science Rev.146, 65–76 (2015).
Burgess, S. D., Bowring, S. A., Fleming, T. H. & Elliot, D. H. High-precision geochronology links the Ferrar large igneous province with early-Jurassic ocean anoxia and biotic crisis. Earth Planet. Sci. Lett.415, 90–99 (2015).
Burgess, S. D. & Bowring, S. A. High-precision geochronology confirms voluminous magmatism before, during, and after Earth’s most severe extinction. Sci. Adv.1, 1–14 (2015).
Schoene, B. et al. U-Pb constraints on pulsed eruption of the Deccan Traps across the end-Cretaceous mass extinction. Science (80-.).363, 862–866 (2019).
Davies, J. H. F. L. et al. End-Triassic mass extinction started by intrusive CAMP activity. Nat. Commun.8, 1–8 (2017).
Corfu, F., Svensen, H. & Mazzini, A. Comment to paper: Evaluating the temporal link between the Karoo LIP and climatic-biologic events of the Toarcian Stage with high-precision U-Pb geochronology by Bryan Sell, Maria Ovtcharova, Jean Guex, Annachiara Bartolini, Fred Jourdan, Jorge E. Spangen. Earth Planet. Sci. Lett.434, 349–352 (2016).
Bond, D. P. G. & Grasby, S. E. On the causes of mass extinctions. Palaeogeogr. Palaeoclimatol. Palaeoecol.478, 3–29 (2017).
Them, T. R. et al. Terrestrial sources as the primary delivery mechanism of mercury to the oceans across the Toarcian Oceanic Anoxic Event (Early Jurassic). Earth Planet. Sci. Lett.507, 62–72 (2019).
Percival, L. M. E. et al. Does large igneous province volcanism always perturb the mercury cycle? Comparing the records of Oceanic Anoxic Event 2 and the end-Cretaceous to other Mesozoic events. Am. J. Sci.318, 799–860 (2018).
Lowrie, W., Alvarez, W. & Asaro, F. The origin of the White Beds below the Cretaceous-Tertiary boundary in the Gubbio section, Italy. Earth Planet. Sci. Lett.98, 303–312 (1990).
Smit, J., Koeberl, C., Claeys, P. & Montanari, A. Mercury anomaly, Deccan volcanism, and the end-Cretaceous mass extinction: COMMENT. Geology44, e381–e381 (2016).
Racki, G., Rakocinski, M., Marynowski, L. & Wignall, P. B. Mercury enrichments and the Frasnian-Famennian biotic crisis: A volcanic trigger proved? Geology46, 543–546 (2018).
Joachimski, M. M. et al. Devonian climate and reef evolution: Insights from oxygen isotopes in apatite. Earth Planet. Sci. Lett.284, 599–609 (2009).
De Vleeschouwer, D. et al. Timing and pacing of the Late Devonian mass extinction event regulated by eccentricity and obliquity. Nat. Commun.8, 2268 (2017).
Ruebsam, W., Mayer, B. & Schwark, L. Cryosphere carbon dynamics control early Toarcian global warming and sea level evolution. Glob. Planet. Change172, 440–453 (2019).
Bridgham, S. D., Cadillo-Quiroz, H., Keller, J. K. & Zhuang, Q. Methane emissions from wetlands: biogeochemical, microbial, and modeling perspectives from local to global scales. Glob. Chang. Biol.19, 1325–1346 (2013).
Hesselbo, S. P. et al. Massive dissociation of gas hydrate during a Jurassic oceanic anoxic\nevent. Nature406, 392–395 (2000).
Fantasia, A., Föllmi, K. B., Adatte, T., Spangenberg, J. & Montero-Serrano, J.-C. The Early Toarcian oceanic anoxic event: Paleoenvironmental and paleoclimatic change across the Alpine Tethys (Switzerland). Glob. Planet. Change162, 53–68 (2018).
Montero-Serrano, J. C. et al. Continental weathering and redox conditions during the early Toarcian Oceanic Anoxic Event in the northwestern Tethys: Insight from the Posidonia Shale section in the Swiss Jura Mountains. Palaeogeogr. Palaeoclimatol. Palaeoecol.429, 83–99 (2015).
Mailliot, S. et al. Late Pliensbachian–Early Toarcian (Early Jurassic) environmental changes in an epicontinental basin of NW Europe (Causses area, central France): A micropaleontological and geochemical approach. Palaeogeogr. Palaeoclimatol. Palaeoecol.273, 346–364 (2009).
Schootbrugge, B. V. D. et al. Early Jurassic climate change and the radiation of organic- walled phytoplankton in the Tethys Ocean. Paleobiology31, 73–97 (2005).
Jenkyns, H. C. & Clayton, C. J. Black shales and carbon isotopes in pelagic sediments from the Tethyan Lower Jurassic. Sedimentology33, 87–106 (1986).
Rosales, I., Quesada, S. & Robles, S. Geochemical arguments for identifying second-order sea-level changes in hemipelagic carbonate ramp deposits. Terra Nov.18, 233–240 (2006).
McArthur, J. M., Donovan, D. T., Thirlwall, M. F., Fouke, B. W. & Mattey, D. Strontium isotope profile of the early Toarcian (Jurassic) oceanic anoxic event, the duration of ammonite biozones, and belemnite palaeotemperatures. Earth Planet. Sci. Lett.179, 269–285 (2000).
Rosales, I., Quesada, S. & Robles, S. Paleotemperature variations of Early Jurassic seawater recorded in geochemical trends of belemnites from the Basque–Cantabrian basin, northern Spain. Palaeogeogr. Palaeoclimatol. Palaeoecol.203, 253–275 (2004).
Bailey, T. R., Rosenthal, Y., McArthur, J. M., van de Schootbrugge, B. & Thirlwall, M. F. Paleoceanographic changes of the Late Pliensbachian–Early Toarcian interval: a possible link to the genesis of an Oceanic Anoxic Event. Earth Planet. Sci. Lett.212, 307–320 (2003).
Suan, G. et al. Duration of the Early Toarcian carbon isotope excursion deduced from spectral analysis: Consequence for its possible causes. Earth Planet. Sci. Lett.267, 666–679 (2008).
Korte, C. et al. Jurassic climate mode governed by ocean gateway. Nat. Commun.6, 1–7 (2015).
Self, S., Thordarson, T. & Widdowson, M. Gas fluxes from flood basalt eruptions. Elements1, 283–287 (2005).
Self, S., Widdowson, M., Thordarson, T. & Jay, A. E. Volatile fluxes during flood basalt eruptions and potential effects on the global environment: A Deccan perspective. Earth Planet. Sci. Lett.248, 517–531 (2006).
Black, B. A. et al. Systemic swings in end-Permian climate from Siberian Traps carbon and sulfur outgassing. Nat. Geosci.11, 949–954 (2018).
Dera, G. et al. Climatic ups and downs in a disturbed Jurassic world. Geology39, 215–218 (2011).
Robock, A. Volcanic eruptions and climate. Rev. Geophys.38, 191–219 (2000).
Sell, B. et al. Evaluating the temporal link between the Karoo LIP and climatic–biologic events of the Toarcian Stage with high-precision U–Pb geochronology. Earth Planet. Sci. Lett.408, 48–56 (2014).
Hesselbo, S. P., Jenkyns, H. C., Duarte, L. V. & Oliveira, L. C. V. Carbon-isotope record of the Early Jurassic (Toarcian) Oceanic Anoxic Event from fossil wood and marine carbonate (Lusitanian Basin, Portugal). Earth Planet. Sci. Lett.253, 455–470 (2007).
Littler, K., Hesselbo, S. P. & Jenkyns, H. C. A carbon-isotope perturbation at the Pliensbachian–Toarcian boundary: evidence from the Lias Group, NE England. Geol. Mag.147, 181–192 (2010).
Widmann, P., Davies, J. H. F. L. & Schaltegger, U. Calibrating chemical abrasion: Its effects on zircon crystal structure, chemical composition and U Pb age. Chem. Geol.511, 1–10 (2019).
Mattinson, J. M. Zircon U-Pb chemical abrasion (‘CA-TIMS’) method: Combined annealing and multi-step partial dissolution analysis for improved precision and accuracy of zircon ages. Chem. Geol.220, 47–66 (2005).
Hiess, J., Condon, D. J., McLean, N. M. & Noble, S. R. 238U/235U Systematics in Terrestrial Uranium-Bearing Minerals. Science (80-.).335, 1610–1614 (2012).
Jaffey, A. H., Flynn, K. F., Glendenin, L. E., Bentley, W. C. & Essling, A. M. Precision measurement of half-lives and specific activities of U235 and U238. Phys. Rev. C4, 1889–1906 (1971).
Schoene, B., Latkoczy, C., Schaltegger, U. & Günther, D. A new method integrating high-precision U-Pb geochronology with zircon trace element analysis (U-Pb TIMS-TEA). Geochim. Cosmochim. Acta74, 7144–7159 (2010).
Haslett, J. & Parnell, A. A simple monotone process with application to radiocarbon-dated depth chronologies. J. R. Stat. Soc. Ser. C (Applied Stat.57, 399–418 (2008).
Parnell, A. C., Haslett, J., Allen, J. R. M., Buck, C. E. & Huntley, B. A flexible approach to assessing synchroneity of past events using Bayesian reconstructions of sedimentation history. Quat. Sci. Rev.27, 1872–1885 (2008).
Espitalié, J., Deroo, G. & Marquis, F. Rock-Eval pyrolysis and its application. Rev. l’Institut Français du Pétrole16, 755–784 (1985).
Cohen, A. S. & Waters, F. G. Separation of osmium from geological materials by solvent extraction for analysis by thermal ionisation mass spectrometry. Anal. Chim. Acta332, 269–275 (1996).
Birck, J. L., Barman, M. R. & Capmas, F. Re-Os Isotopic Measurements at the Femtomole Level in Natural Samples. Geostand. Geoanalytical Res.21, 19–27 (1997).
Creaser, R. A., Papanastassiou, D. A. & Wasserburg, G. J. Negative Thermal Ion Mass-Spectrometry of Osmium, Rhenium, and Iridium. Geochim. Cosmochim. Acta55, 397–401 (1991).
Völkening, J., Walczyk, T. & Heumann, K. G. Osmium isotope ratio determinations by negative thermal ionization mass spectrometry. Int. J. Mass Spectrom. Ion Process.105, 147–159 (1991).
Nier, A. O. A Redetermination of the Relative Abundances of the Isotopes of Carbon, Nitrogen, Oxygen, Argon, and Potassium. Phys. Rev.77, 780–793 (1950).
Brandon, A. D., Humayun, M., Puchtel, I. S. & Zolensky, M. E. Re-Os isotopic systematics and platinum group element composition of the Tagish Lake carbonaceous chondrite. Geochim. Cosmochim. Acta69, 1619–1631 (2005).
Luguet, A. et al. Enriched Pt-Re-Os Isotope Systematics in Plume Lavas Explained by Metasomatic Sulfides. Science (80-.).319, 453–456 (2008).
Liu, J. & Pearson, D. G. Rapid, precise and accurate Os isotope ratio measurements of nanogram to sub-nanogram amounts using multiple Faraday collectors and amplifiers equipped with 1012Ω resistors by N-TIMS. Chem. Geol.363, 301–311 (2014).
Li, X. et al. Efficient electroluminescence based on a novel binuclear rhenium complex. Opt. Mater. (Amst).31, 1173–1176 (2009).
L.F.DL would like to thank CAPES (Under Project 1130-13-7) and UNIGE for financial support. U.S. acknowledges the longstanding and generous financial support of the Swiss National Science Foundation for the isotope laboratories at University of Geneva. We thank Phil & Kristy St. Clair for access to their land and their generous hospitality.
The authors declare no competing interests.
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De Lena, L.F., Taylor, D., Guex, J. et al. The driving mechanisms of the carbon cycle perturbations in the late Pliensbachian (Early Jurassic). Sci Rep 9, 18430 (2019). https://doi.org/10.1038/s41598-019-54593-1
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