Abstract
A hypothesized rise in oxygen levels in the Neoproterozoic, dubbed the Neoproterozoic Oxygenation Event, has been repeatedly linked to the origin and rise of animal life. However, a new body of work has emerged over the past decade that questions this narrative. We explore available proxy records of atmospheric and marine oxygenation and, considering the unique systematics of each geochemical system, attempt to reconcile the data. We also present new results from a comprehensive COPSE biogeochemical model that combines several recent additions, to create a continuous model record from 850 to 250 Ma. We conclude that oxygen levels were intermediate across the Ediacaran and early Palaeozoic, and highly dynamic. Stable, modern-like conditions were not reached until the Late Palaeozoic. We therefore propose that the terms Neoproterozoic Oxygenation Window and Palaeozoic Oxygenation Event are more appropriate descriptors of the rise of oxygen in Earth's atmosphere and oceans.
Keywords: Neoproterozoic, Palaeozoic, oxygenation, redox proxies, COPSE
1. Introduction
Since the Great Oxidation Event, 2.5–2.3 billion years ago (Ga), oxygen has been a persistent feature of Earth's atmosphere [1], but has remained at low levels throughout the Palaeoproterozoic and Mesoproterozoic eras (2.5–1.0 Ga). A hypothesized rise towards modern oxygen levels in the Neoproterozoic (1.0–0.54 Ga) was dubbed the ‘Neoproterozoic Oxygenation Event’ (NOE) [2]. Evidence for the NOE included broad increases in the average molybdenum and vanadium concentrations in black shales [3]; an increase in the isotope fractionation between sulfate and pyrite (Δ34SSO4−pyr) [4]; and Fe speciation evidence for local deep water oxygenation [5].
Geochemical data collected over the last decade have disrupted this narrative. Despite an increase in the breadth and depth of proxy data now available, we appear to be further from a consensus on the timing and dynamics of oxygenation. Some proxies support a single, unidirectional step change in oxygen levels, although the estimates of the timing span almost 600 Myr [6–15]. Other proxy data support a more dynamic system, with large oscillations in oxygen availability [16–18].
How can we reconcile these different proxy records? One possibility is that some of the geochemical data do not record ancient redox conditions, because they have been overprinted by diagenesis and metamorphism. While some published data may need to be revisited, other geochemical signals are reproducible in samples from different basins (e.g. uranium isotopes [18,19] or redox sensitive trace elements [7,17,20,21]). In addition, geochemical redox analysis can be paired with petrography or other geochemical data to screen for potential alteration. Another possibility is that we are misinterpreting primary geochemical signals. Because today's oceans are largely well-oxygenated, proxy systems are calibrated in isolated basins and lakes, and these environments may not provide a reasonable analogue for a globally anoxic deep ocean. Alternatively, each proxy may be capturing different parts of a complex transition, depending on the proxy systematics, marine residence time, reduction potential and sampling density. Here, we critically evaluate current proxy evidence for Neoproterozoic–Palaeozoic oxygenation, attempt to reconcile the various records and compare them to the latest biogeochemical modelling results.
2. Evaluation of current geochemical evidence
2.1. Local marine geochemical proxies
Local marine redox proxies record progressive changes within a single basin [5,22], but if those changes are driven by local hydrodynamics or changes in productivity, they may not reflect global changes in oxygen availability. When sufficient local proxy data are collected from multiple basins, the compiled data may record a statistically significant change in the average oxidation state of the ocean. However, these proxy records are necessarily biased towards shelf and slope environments, as Proterozoic sediments from the abyssal plain are rarely preserved. Proxies preserved in carbonates, such as I/Ca and Ce anomalies, are further biased towards warm, shallow shelf environments at low latitudes.
2.1.1. Iron speciation
The ratio of highly reactive to total iron preserved in carbonates and shales is indicative of the redox chemistry in the water column directly above the accumulating sediments [23]. Robust calibrations of the proxy in modern sediments allow the differentiation of oxic (FeHR/FeT < 0.22) and anoxic water masses (FeHR/FeT > 0.38), although ambiguous ratios may be generated under high sedimentation or mixing rates (FeHR/FeT 0.22–0.38). For anoxic water masses, the proportion of pyrite in the highly reactive iron phase can distinguish between Fe-bearing (ferruginous) and sulfidic (euxinic) anoxia (table 1). Therefore, ‘oxic’ conditions identified by iron speciation could potentially incorporate suboxic and well-oxygenated conditions. Systematic diagenetic biases could be introduced to the iron speciation record through transformation of unsulfidized highly reactive iron minerals to less reactive sheet silicates, producing a false oxic signal.
Table 1.
proxy | responds to | redox sensitivity | archives | systematic bias? | |
---|---|---|---|---|---|
local/regional marine | iron speciation | integrated regional water column redox conditions above accumulating sediments | ferruginous anoxia and euxinia | shales, carbonate | variable |
I/Ca ratios | upper ocean oxygen gradients | hypoxic (<70 µM O2) to suboxic (between manganous and nitrogenous) | carbonates | false anoxic | |
Ce anomalies | local–regional water column redox at site of carbonate precipitation | suboxic (manganous) | carbonates, phosphorites, iron formation | false anoxic | |
∑Fe3+/Fe | regional deep water oxygen concentrations | progressive with increasing O2(aq) | basalts | false anoxic | |
marine red beds | regional deep ocean oxygen concentrations following periods of anoxia | ferruginous anoxia | marine red beds | ||
global marine | δ238U | area of global seafloor bathed in anoxic waters | anoxia | carbonates, shales | false oxic |
δ98Mo | area of global seafloor bathed in anoxic waters | euxinia | shales | false anoxic | |
RSE enrichments | area of global seafloor bathed in anoxic waters | euxinia (Mo); ferruginous anoxia (Cr, Re, U, V) | euxinic shales | false anoxic | |
δ82Se | local redox conditions and size of global–regional oxidized SeOx2−reservoir | ferruginous anoxia | shales | ||
δ34S | size of global marine sulfate reservoir and global proportional pyrite burial flux | euxinia, atmospheric O2 | carbonates, evaporites | variable | |
atmospheric | δ53Cr | atmospheric oxygen | >0.1–1% PAL | shales, ironstones | |
wildfire record | atmospheric oxygen | >70% PAL | charcoal |
A transition towards oxic Fe speciation signals approximately 580 Ma, recorded in shales deposited on a continental slope, was thought to pinpoint permanent oxygenation of the deep ocean [5]. However, as more data have been collected, an increasingly complex picture of spatial and temporal heterogeneity has emerged. For example, data from basins of the same age in the Canadian cordillera show no such oxygenation [21,24], and younger basins record anoxic waters impinging onto the shelf [25]. A recent statistical analysis of 4700 Fe speciation measurements from deep water settings across a range of ages and locations has revealed no significant long-term (i.e. 100 Myr) trend towards more oxic conditions across the Neoproterozoic and early Palaeozoic (figures 1 and 2) [14]. This study has good spatial and temporal coverage from approximately 2.1 Ga to 440 Ma, although Silurian–Devonian data come from just two studies and may be subject to sampling biases (figure 2) [7,32].
2.1.2. Iodine to calcium ratios
Iodine to calcium ratios in carbonate rocks reflect local water column redox conditions. Since the reduction of iodate to iodide (I−) has a relatively high reduction potential, the I/Ca proxy is sensitive to intermediate redox conditions, from hypoxic (less than 70–100 µM O2) to suboxic (manganous–nitrogenous conditions) [33] (table 1). Iodate is incorporated into carbonate rocks, and so I/Ca ratios reflect the oxidized iodate concentration in the local water column at the depth of carbonate formation, which varies with the concentration of oxygen in surface waters and the depth of the top of the oxygen minimum zone (OMZ) [10]. Due to the slow kinetics of iodide oxidation, water masses with fluctuating redox conditions, or anoxia nearby, may retain a low iodate signature, biasing primary signatures towards anoxic conditions. In addition, diagenesis can reduce the I/Ca ratio, but not increase it, systematically biasing the rock record towards anoxic conditions [26].
I/Ca data span a large range at any given location, but if there are sufficient data, then an increase in the maximum I/Ca may indicate oxygenation. Long-term compilations reveal variable but low I/Ca across the Neoproterozoic and Early Palaeozoic [26] (figure 2), with notable peaks during the Bitter Springs (approx. 810–800 Ma) [28] and the Shuram excursion (approx. 560 Ma) [26,34]. I/Ca ratios show a significant peak in the Devonian, between approximately 400 and approximately 350 Ma, but a return to lower values in the Carboniferous and Permian (figures 1 and 2) [10]. There is no permanent change towards higher I/Ca ratios until the early Mesozoic. The maximum I/Ca recorded in any given time window may evolve as more data are collected.
2.1.3. Cerium anomalies
Negative Ce anomalies in rare earth element patterns are indicative of locally oxic water column conditions. Under oxidizing conditions, Ce(III) is oxidized to Ce(IV) on the surface of Mn (oxyhydr)oxide minerals, resulting in relative depletion in shale-normalized seawater Ce concentrations compared with the other rare earth elements. The generation of Ce anomalies requires oxidation of Mn and Ce, both of which have relatively high reduction potentials (+1.23 mV and +1.44 mV, respectively). Therefore, Ce anomalies are responsive to the onset of manganous conditions, which may overlap with low oxygen concentrations (less than 10 µM). Ce anomalies can respond to redox changes over metre scales [35], although in the open ocean, local signals may be overprinted by basin-wide signals due to slow kinetics [29] (table 1). The magnitude of any Ce anomaly may correspond to the concentration of oxygen or the thickness of the oxic layer, but can also be influenced by other factors such as local Mn oxide fluxes [36]. Rare earth elements, and associated Ce anomalies, substitute for Ca2+ in the carbonate mineral lattice, and as such, can faithfully record seawater rare earth elements at the site of carbonate formation and are relatively robust to diagenesis and even dolomitization [30,37].
A progressive increase in the magnitude of the Ce anomaly after 551 Ma in carbonate rocks from South China was interpreted to record an increase in oxygen levels in the shallow marine environment during the late Ediacaran [22]. However, reducing signals have since been recorded in contemporaneous rocks from the Nama Group, Namibia [31], suggesting oxygenation was not a global phenomenon. Further, long-term compilations of Ce anomaly data from 18 formations show no significant change until the Late Devonian (approx. 383 Ma; figures 1 and 2) [29]. However, this broad compilation includes large sample gaps. For example, there is only one sample between approximately 600 Ma and approximately 550 Ma.
2.1.4. Fe3+/∑Fe ratio of submarine basalts
As oxygenated water circulates through seafloor basalts, reduced iron is oxidized to Fe3+. Therefore, the Fe3+/∑Fe ratio of submarine basalts varies with the magnitude of hydrothermal fluxes and with the oxygen content of bottom waters. As such, seafloor basalts, preserved as ophiolites, can provide a direct record of deep water oxygen concentrations (table 1). Metamorphism acts to reduce Fe3+ and so could systematically bias the Fe3+/∑Fe ratio towards lower values.
Long-term compilations of Fe3+/∑Fe data show no significant change across the Archean and Proterozoic (Archean = 0.20 ± 0.04; Palaeo–Mesoproterozoic = 0.26 ± 0.02; Neoproterozoic = 0.26 ± 0.05), but a progressive increase across the Early Palaeozoic (0.34 ± 0.08), Late Palaeozoic (0.47 ± 0.10) and Mesozoic–Cenozoic (0.58 ± 0.11) (figure 2) [15]. This indicates a progressive increase in oxygen content of the deep ocean from 11 ± 17 µmol kg−1 in the Neoproterozoic, to 29 ± 29 µmol kg−1 in the Early Palaeozoic, 55 ± 42 µmol kg−1 in the Late Palaeozoic and 80 ± 53 µmol kg−1 in the Mesozoic–Cenozoic (figure 1). Due to the distribution of rare ophiolites in the geological record, there are large gaps where no data are available, as well as large uncertainties in the age of some samples. For example, there are no data between 736 ± 1.7 Ma and 554.5 ± 136.5 Ma. In the Stolper & Keller [15] study, the Neoproterozoic time bin is dominated by samples greater than 700 Ma, but samples between 555 and 541 are within range of the Early Palaeozoic average (this is reflected in figure 1).
2.1.5. Red beds
The distribution of iron rich rocks through the geological record may reflect ocean redox dynamics and Fe2+ concentrations [13]. Iron formation requires Fe2+ concentrations greater than 50 µM, whereas marine red beds, which are thinner and have lower %Fe, only require greater than 4 nM. Major periods of marine red bed deposition occurred in the mid-Ediacaran, Cambrian and Late Devonian, with a possible event in the late Silurian [13] (blue on figure 1). These sporadic events indicate lower deep water Fe concentrations following anoxic events, which could be consistent with more oxygenated deep oceans. This record is biased towards preserved shelf sediments and may evolve if more examples are documented.
2.2. Global marine geochemical proxies
2.2.1. Uranium isotopes
The uranium isotope ratio of seawater (δ238U) is sensitive to the global proportion of seafloor overlain by anoxic bottom waters. During reduction of soluble U(VI) to insoluble U(IV) under anoxic conditions, sedimentary U(IV) is enriched in 238U, leaving seawater depleted in 238U. Therefore, when the anoxic sink expands, seawater δ238U decreases, and this signal can be preserved in carbonates. Organic-rich mudrocks also track changes in seawater δ238U, but the signal is offset by a variable local fractionation factor [38] (table 1). δ238U data can be used to calculate the proportion of anoxic seafloor, although these estimates rely on several calibration factors that were determined in modern lakes (e.g. the Black Sea [39]). In particular, the calculations are sensitive to the isotope fractionation during U reduction, but more work is needed to explore how this varies under euxinic and anoxic ferruginous conditions. Above approximately 20% seafloor anoxia, the proxy begins to saturate [40], and large changes in the proportion of seafloor anoxia only translate into small changes in δ238U. These small changes are within the error introduced by diagenesis [41], which can result in positive δ238U offsets of less than 0.3‰.
Uranium isotope data are available for parts of the Neoproterozoic–Cambrian record (the post-Sturtian interval, and approximately 560 to approximately 510 Ma). These data show large oscillations between high, modern-like δ238U, and very low δ238U, suggesting that long-term anoxia was punctuated by ocean oxygenation events at approximately 660, 560, 540 and 520 Ma (figure 1) [9,18,19,40,42,43]. Some of these oscillations are confirmed by multiple studies in different basins [9,18,19]. Short-term switches towards anoxic conditions are recorded approximately 497 Ma [44] and 372 Ma [45]. Placing δ238U into a quantitative model suggests seafloor anoxia oscillated from greater than 30% during periods of quiescence, to less than 1% during oxygenation events [18].
2.2.2. Molybdenum isotopes
High δ98Mo values preserved in shales indicate globally widespread oxic conditions, under which large negative isotope fractionations occur during adsorption of Mo onto Mn oxides, leaving seawater isotopically enriched (table 1). By contrast, under euxinic conditions, Mo is rapidly and quantitatively removed. Since all known sedimentary Mo sinks have a δ98Mo below contemporaneous seawater, δ98Mo measurements only provide a minimum constraint on δ98MoSW. Further, interpretations of sedimentary δ98Mo rely on independent proxy evidence for local redox conditions. Changes in δ98Mo could also result from a switch from euxinic to ferruginous anoxia, with no overall increase in oxygenated waters.
Pulses in δ98Mo are recorded between 550 and 520 Ma, each one reaching progressively higher δ98Mo maxima [6]. This was interpreted to indicate progressive marine oxygenation across the Cambrian, but the data contain a lot of scatter and could also be consistent with discrete oxygenation pulses at approximately 552, 540, 530 and 521 Ma (figure 1) [6,7,9]. Distinguishing between these two scenarios is difficult because the rarity of black shales deposited under fully euxinic conditions limits the resolution of the record. The magnitude of δ98Mo enrichments increases through time, suggesting each oxygenation event was more significant than the last [6]. δ98Mo reaches stable, modern-like levels between the mid-Silurian and mid-Devonian (approx. 430–390 Ma) [7]. Modelling calculations suggest that oxygenation events in the Neoproterozoic were limited (33% oxic seafloor) [6,7], but reached greater than 97% oxic seafloor by approximately 520 Ma, although many of the parameters in these models are poorly constrained.
2.2.3. Redox sensitive elements
Because Mo is scavenged from seawater under euxinic conditions, and V, U, Re and Cr are scavenged under ferruginous conditions, an increase in the concentration of redox sensitive elements (RSE) in seawater can indicate the global retreat of anoxic sinks. RSE concentrations in shales are controlled by the size of the global RSE reservoir and an enrichment factor, which varies with the local redox conditions. RSE concentrations are commonly analysed in sediments where there is independent evidence for local euxinia, to ensure a consistent local enrichment factor, meaning any enrichments in RSE can be attributed to an expanded global marine RSE reservoir (table 1). RSE data typically show large amounts of scatter, but an increase in the average or maximum concentration can be interpreted as evidence for an increase in the area of oxic seafloor.
Long-term compilations appeared to show an abrupt increase in Mo, V and U concentrations between 663 and 551 Ma [3,46], interpreted to mark widespread oxygenation of the oceans [2]. A recent re-analysis of the U record shows that there is a statistically significant increase in average U concentrations between the Cambrian–Silurian and Devonian–Permian, suggesting any step change towards more permanently oxygenated oceans occurred in the Palaeozoic (figure 1) [14,46]. The precise timing of any change will depend on the positions of relatively long time-scale bins used for data analysis. However, a more complete stratigraphic record with higher sampling density, from a demonstrably open ocean section in Wuhe, South China, has revealed pulses of RSE enrichment at regular intervals, representing ocean oxygenation events at 635, 580, 560, 540, 530 and 522 Ma (figure 1) [17]. Similar enrichments are observed in other sections located on different cratons, suggesting a truly global signal [7,20,21]. In between these oxygenation events, the widespread anoxia that characterizes much of the Proterozoic returns. Modelling efforts suggest that relatively limited seafloor euxinia (1–10%) and more extensive seafloor anoxia (greater than 30–40%) are needed to crash the global Mo and Cr reservoirs, respectively [47].
2.2.4. Selenium isotopes
Se isotopes (δ82Se) in marine shales are a novel tracer for ocean–atmosphere oxygenation. Se has a reduction potential between S(–II)/S(IV) and Fe(III)/Fe(II) and a relatively short marine residence time (1100–26 000 years) [48]. During oxyanion reduction under anoxic conditions, isotopically light Se is sequestered into the sediments, driving surface waters isotopically heavy. In addition, an increase in the size of the reservoir correlates with larger fractionations in locally suboxic sediments (table 1). Sediments deposited in oxic open oceans, or below well-connected OMZs, have lower δ82Se than those from restricted anoxic basins, due to the larger reservoir. δ82Se yields insight into the local water column redox conditions, with an additional global control. The signal may be further complicated by variations in riverine input, locally enhanced productivity, or basin restriction.
A progressive decrease in δ82Se is recorded in shales across the Ediacaran, reaching a minimum around the end of the Ediacaran [12]. For the pre-Gaskiers record, the signal is confirmed in multiple sections, suggesting a global control. This is probably a reflection of an increasing reservoir, which could reflect ocean oxygenation. Overall, the record is difficult to interpret, but suggests a slow but steady shift from fully anoxic to fully oxic deep waters between 750 and 540 Ma.
2.2.5. Sulfur isotopes
Under euxinic conditions, microbial sulfate reduction converts sulfate into sulfide (HS−), which may be buried as pyrite. The δ34S of seawater sulfate is sensitive to the global pyrite burial flux, and the isotope fractionation associated with that pyrite burial. Both of these parameters are closely tied to ocean–atmosphere redox (table 1). The δ34S signature of seawater is complex [49], but higher δ34SSO4 could indicate enhanced pyrite burial, which may be driven by expanded euxinia. Large offsets between δ34SSO4 and δ34Spyr (Δ34SSO4−pyr) have been interpreted to result from a larger marine sulfate reservoir, as well as complex sulfur cycling associated with oxidative side of the S cycle, both of which are associated with higher oxygen levels. At modern marine sulfate concentrations, the δ34S of seawater should be globally homogeneous and is preserved in carbonate rocks and evaporites.
Sedimentary records show a progressive increase in Δ34SSO4−pyr across the Ediacaran (635 to approximately 550 Ma) [8], interpreted to represent an increase in the marine sulfate reservoir, and then the onset of oxidative sulfur cycling. The Δ34SSO4−pyr decreases again in the latest Ediacaran (approx. 550 Ma), along with an increase in δ34SSO4, suggesting increased pyrite burial and a return to anoxia [50]. However, subsequent work has questioned the link between Δ34SSO4−pyr and oxidative sulfur cycling [51]. A series of rapid oscillations in δ34SSO4 are recorded 524–512 Ma [16], coincident with excursions in δ13Ccarb, where the rising limbs are associated with periods of ocean anoxia and increased pyrite burial. This increase in net pyrite burial would produce a pulse of atmospheric oxygen, in turn driving anoxia from the shelf. Further δ34SSO4 oscillations are recorded at around 500 Ma [44]. Sulfur isotopes therefore support dynamic redox conditions into the Cambrian and beyond.
2.3. Constraints on atmospheric oxygen
2.3.1. Chromium isotopes
The oxidation and reduction of Cr between Cr(III) and Cr(IV) result in large fractionations. Cr oxidation occurs through dissolution of Cr(III) in soils and reaction with Mn oxides, the presence of which is linked to free O2. This yields dissolved Cr(VI) species ( and ) that are more soluble and enriched in the heavy isotope, compared with Cr(III). Therefore, under reducing conditions, the marine Cr record in shales and ironstones will be dominated by unfractionated crustal Cr(III), whereas under an oxidizing atmosphere, the Cr record will be isotopically enriched.
The long-term δ53Cr record shows a marked enrichment between 800 and 750 Ma [11], recorded in both shales and ironstones, and interpreted to indicate a rise in atmospheric O2 levels. Although the pre-800 record is dominated by low δ53Cr, isolated examples of 53Cr enrichments have been recorded [52]. Cr(III) oxidation during weathering is dependent on Mn oxide availability. Quantitative modelling suggests Mn oxide formation occurs at low O2 (greater than 0.1–1% present atmospheric levels (PAL)), providing a maximum constraint on the pre-800 Ma atmosphere [11] and suggesting a modest increase in atmospheric O2 around 800–750 Ma.
2.3.2. Wildfire record
Wildfires can only be sustained when atmospheric oxygen levels are high (greater than 15–17%) [53]. Charcoal, the geological expression of palaeo-wildfires, is present in the geological record from the latest Silurian onwards [54]. Charcoal is low in abundance across the Silurian and Devonian, but increases by 1–2 orders of magnitude in the late Devonian [55]. This suggests oxygen crossed a critical threshold in the Late Silurian (greater than 15%), but rose further in the Late Devonian (greater than 17%). Wildfires are dependent on the presence of land plants, which evolved approximately 470 Ma, so the charcoal record cannot constrain pre-Ordovician pO2.
3. Reconciling proxy records
Direct proxies for atmospheric oxygen are scarce. Chromium isotopic fractionations indicate that O2 rose above 0.1–1% PAL at around 800 Ma [11]; however, earlier evidence for fractionation of chromium has been recorded [52]. More certain is a rise in O2 to greater than 70% PAL during the Late Silurian and a final rise towards modern levels in the Devonian (greater than 80% PAL or above) [55,56]. Regardless of atmospheric oxygen concentrations, substantial spatial and temporal variability is expected in marine redox conditions, as water column O2 is controlled by a balance between the oxygen supply and its utilization during remineralization. Modelling calculations suggest that widespread deep ocean oxygenation requires atmospheric oxygen to exceed 30–40% PAL, but this depends on the availability of the limiting nutrient phosphate [57], and on the model itself. That said, to first order, deep water oxygenation would be expected to track a substantial rise in atmospheric oxygen levels.
Some global marine geochemical proxies record a permanent change towards widespread oxygenation in the late Palaeozoic, including δ98Mo and U enrichments [7,14,46]. Similarly, compilations of local marine redox proxies do not detect any statistically significant change in oxygen availability across the Neoproterozoic, and instead pinpoint widespread marine oxygenation later, in the Late Palaeozoic–Mesozoic: post-Ordovician for Fe speciation [14], Late Devonian for Ce anomalies [29], Late Palaeozoic for Fe3+/∑Fe ratios [15] and Early Devonian for I/Ca [10]. There is some variability in the precise timing recorded by each proxy, which may be accounted for by their different sensitivity to the spatial extent or location of anoxia, or to increasing redox state. More importantly, the timing of oxygenation in long-term data compilations is highly sensitive to sampling density as well as the boundaries of data bins. For example, Fe3+/∑Fe ratio data are necessarily sparse as they are derived from rare ophiolites. Therefore, these techniques can only be used to make broad comparisons between, for example, the Early Palaeozoic and Late Palaeozoic. Four compilations of local proxy data, re-analysed using consistent time bins, all show a significant increase in oxygenation in the period 420–250 Ma compared with 580–420 Ma (figure 2).
Broadly anoxic Neoproterozoic–Early Palaeozoic oceans could manifest as oxic surface waters overlying fully anoxic deep waters in a ‘pancake’ structure (figure 3a), or as shallow, expanded OMZs (figure 3b and c). A four-dimensional transect of local redox conditions across a shelf suggests that OMZ-like structures were established by the Cambrian [58], implying that the deep ocean contained low levels of oxygen. This is consistent with Fe3+/∑Fe ratios [15] and the marine red bed record [13], which support low levels of oxygen in deep waters from the mid-Ediacaran onwards. A shallower OMZ could be a reflection of lower atmospheric oxygen levels, but could also result from differences in carbon cycling.
If there were indeed mildly oxidizing conditions in the Neoproterozoic-Early Palaeozoic ocean, then how do we reconcile this with global redox proxies that suggest widespread marine anoxia? Global redox proxies tend to record the percentage of seafloor, globally, that is overlain by anoxic bottom waters, but do not provide insight into the location of those anoxic waters. This is further complicated by the lack of information available on marine productivity, sinking fluxes and ocean circulation, which are key controls on OMZ characteristics. Shallowing of OMZs can result in a much larger contact area between anoxic waters and the continental shelf, translating into a larger area of anoxic seafloor, despite no change in the thickness of the OMZ [59] (figure 3c,d). If the OMZ also expanded in thickness, the combined effect could result in the estimated 10–30% seafloor anoxia and 1% seafloor euxinia required to generate anoxic δ98Mo, δ238U and U-enrichment signals (figure 3b). Furthermore, if bottom waters in the deep ocean were oxic, but contained only low levels of oxygen (less than 10 µM), then shallow pore waters would be commonly driven anoxic, which may further contribute to anoxic draw down of RSE such as Mo and U.
Although large areas of the seafloor remained anoxic or contained only low levels of oxygen through the Neoproterozoic–Lower Palaeozoic, some proxy systems suggest conditions were dynamic, with brief ocean oxygenation events (OOEs). Some OOEs are recorded independently by multiple proxy systems. For example, the transition back towards anoxic conditions following the 550 Ma OOE is recorded by δ98Mo, δ238U, RSE enrichments, I/Ca ratios and δ34S (figure 1) [8,9,17,18,26,50]. By contrast, OOEs are not detected in any compilations of local proxy data. For I/Ca ratio and Ce anomaly data, this is likely because sample coverage is too sparse to detect them. For Fe speciation or Fe3+/∑Fe ratio data, OOEs would not be detected as data are binned into periods orders of magnitude longer than the duration of OOEs, so OOEs are averaged out or not sampled. Therefore, global redox proxies, analysed in continuous, high-resolution sections, detect variability that can be missed by compilations of local redox proxies.
4. Modelling the long-term redox transition
Global biogeochemical models can be used to evaluate the processes which have caused the observed oxygenation pattern. The COPSE model [60] is a non-dimensional system (or ‘box model’), which computes the operation of the global C-O-P-S cycles over geological timescales and is based on the pioneering GEOCARB models [61,62]. Like GEOCARB, the key considerations for COPSE are the global weathering, burial and degassing processes that control the transfer of key species between the hydrosphere and the crust. The long-term O2 sources are burial of either organic carbon or pyrite sulfur in sediments (removal of a reductant leads to net oxygenation), and the O2 sinks are the uplift and weathering, or subduction and degassing, of these reduced species which consumes O2. Importantly, COPSE differs from the GEOCARB models in that it is a ‘forwards’ model, meaning that it computes all processes via an internally consistent set of biogeochemical rules [63,64], rather than seeking to infer them directly from the geological record. This means that COPSE can produce estimates of key geochemical proxies such as carbonate δ13C, sulfate δ34S and strontium 87Sr/86Sr, which are then used to test the ‘skill’ of the model by comparing to geological data.
The model is subject to ‘external forcings’: the rate of tectonic CO2 input, continental uplift and palaeogeography, exposed lithological classes, and a variety of switches that represent the evolution of different modes of life which affect global biogeochemistry. Recent reviews are available that describe the latest version of the model [65,66]. Originally COPSE was built for reconstructing the Phanerozoic Earth system, but in the last decade, there may have been extensions to apply the model to the late Precambrian. These extensions have tended to focus on single events such as snowball Earth termination [67] or the Shuram negative carbon isotope excursion [68]. We now bring together the key modifications of the model to produce a complete suite of simulations over the Neoproterozoic and Palaeozoic (see electronic supplementary material for full explanation of model parameters and differential equations).
We begin from the model of Mills et al. [66], which extended the latest major model release [65] by updating the rates of CO2 degassing and tectonic uplift with new estimates, as well as revising the link between global climate and chemical weathering rates, informed by Phanerozoic temperature and CO2 proxies. We then add a function for the evolution of bioturbation during the early Cambrian [69]; a function that represents input of reduced species from the mantle [70]; a deep ocean reservoir of dissolved organic carbon [68]; and an uplift-weathering event of evaporite sulfate coincident with the Shuram negative carbon isotope anomaly [68]. Each of these additions has been made to the model previously in isolation and the reader is referred to the cited work for more details. To summarize: bioturbating animals are assumed to evolve by 520 Ma and are presumed to increase the re-oxidation of sedimentary organic matter and drawdown of the nutrient phosphorus; reductant input is assumed to scale with the ridge generation rate and consumes O2; a deep ocean reservoir of dissolved organic carbon (DOC) is assumed to have built up over the Precambrian and is rapidly oxidized when the deep ocean becomes oxic––driving a sharp negative carbon isotope excursion; and a large sulfate input event occurs at 580 Ma due to the uplift and weathering of Tonian-age evaporite giants. Debate continues about whether an enlarged marine DOC reservoir is required in order to explain Neoproterozoic C isotope dynamics [71] and around the timing of the effects of bioturbation [72]. It is hoped that further analytical and modelling efforts will help to fully resolve these questions. Incorporating these mechanisms into a single consistent model is a part of this process.
Figure 1 shows the combined COPSE model predictions for atmospheric O2 and seafloor anoxia over the Neoproterozoic and Palaeozoic and compares them to the proxies discussed earlier. The brown shaded area represents the boundaries of a suite of 10 000 model sensitivity analyses in which the major external forcings (uplift, degassing, lithology) are varied by ±20%. There is some agreement with the proxies for atmospheric O2: COPSE predicts (far) above 0.1% PAL for the entire Neoproterozoic, a rise to greater than 70% PAL by the Silurian, and to 100% PAL in the Devonian. This broad pattern is controlled by the evolution of land plants, which are assumed to increase the weathering delivery of the nutrient phosphate (which drives marine productivity), and also the burial of terrestrially derived organic carbon [55]. Other key features of the atmospheric O2 predictions are a spike between 580 and 570 Ma, caused by uplift and weathering of evaporite sulfate which stimulates pyrite burial [68], and a drop during the Cambrian coincident with the evolution of significant bioturbation, which limits organic carbon preservation [69]. The only area of substantial disagreement with proxies is that COPSE does not produce lower atmospheric O2 before approximately 800 Ma, whereas the lack of fractionation in the chromium isotope record suggests O2 might be below 1% PAL [11]. It is not currently clear how strong the constraint from the Cr isotope record is, given that fractionations have been found in several pre-800 Ma samples [52], but it is also possible that a major process is still missing from COPSE, which if included, would result in lower atmospheric O2. There are several candidates here, including the lack of explicit productivity-remineralization dynamics in the ocean, or a better representation of Precambrian tectonics. Research is ongoing.
The seafloor anoxia prediction from COPSE follows the transitions in atmospheric O2, with more than 50% of the seafloor anoxic during the Neoproterozoic, and full ventilation during the Devonian. In general agreement with the proxies, there is a period of expanded oxic seafloor immediately post-Gaskiers, which then returns to almost entirely anoxic by the later Cambrian. But there are three major discrepancies between the model predictions and the proxies for seafloor anoxia. First, the model does not produce any of the rapid variability attested to by the proxies (OOEs). Second, the model fails to reproduce longer term oxygenation surrounding the Sturtian and Marinoan glaciations. Finally, the model predicts very large anoxic seafloor areas during the later Cambrian and Ordovician, which are not directly supported by any proxies.
The inability of the COPSE model to reproduce the OOEs in the later Ediacaran and Cambrian is probably due to the model's use of a single-box ocean. In COPSE, the shelf environments and (much more vast) deeper ocean are considered to be a single system. This adds a huge amount of buffering capacity, which may not be realistic. A more sophisticated biogeochemical model [73,74] splits the ocean into multiple boxes representing areas of the shelf, open ocean and deep ocean. This model shows that OOEs can occur due to feedbacks between the marginal phosphorus and oxygen cycles, and thus the lack of OOEs in COPSE may be a consequence of limited representation of shelf environments.
The lack of any appreciable oxygen changes around the Sturtian and Marinoan glaciations is also relatively easily explained, as this version of the COPSE model still does not incorporate any of the processes associated with either the initiation or termination of these snowball Earth events. Looking to the model outputs for sedimentary isotope ratios (figure 4), it is clear that while the post-Gaskiers predictions are within reason, the model is missing major aspects of Earth system function pre-600 Ma, especially in the carbon cycle. Here, the large and sustained positive carbon isotope excursions that occur before the Sturtian, and during the aftermath of both glaciations, may represent increased productivity and oxygen production, which is supported by the O2 proxies.
An argument could be made that the break-up of the Rodinia supercontinent was underway by approximately 750 Ma [75] and led to enhanced continental weathering [76], high rates of organic carbon burial and high δ13C, before driving the system towards the Sturtian snowball Earth. It is then possible that CO2 rose to extremely high levels during the glaciations, meaning that the super-greenhouse period that followed glaciation lasted several tens of millions of years before CO2 could be reduced to background levels [67]. Adding these ideas into the COPSE model is possible, but in order to reproduce the timing of isotope excursions, the weathering response to temperature and the effect of erosion on weathering must be very carefully chosen. Thus, we defer further investigation of the dynamics and timing of global glaciations and weathering events in the Cryogenian to spatial models with a better approximation of continental weathering (e.g. GEOCLIM [77,78]).
The large areas of anoxic seafloor during the Cambrian–Ordovician coincide with carbonate δ13C predictions that sit generally below the data, indicating that the model may be underestimating oxygen production (or incorrectly simulating organic C weathering [79]). This may be due to an over-estimate of the importance of bioturbation in re-oxidizing sedimentary organic carbon and burying phosphate. New reaction–transport models of the bioturbation process will hopefully help test this.
5. Assessing the role of oxygen in early animal evolution
The hypothesized rise in oxygen levels across the Neoproterozoic–Palaeozoic has been repeatedly linked to the origin and radiation of early animals [5–7,11,16,80]. Given that oxygen is required by all extant animals, this hypothesis seems intuitive and has proved rather attractive. But a large body of recent work has shown that the role of oxygen in early animal ecosystems is more complex than previously thought [18,81,82]. One issue is that not all geochemical data provide the information needed to address ecologically relevant questions, such as the precise oxygen levels. Waters containing 100 µM or 1 µM O2 would be indistinguishable in many proxy systems, but the first could host a complex ecosystem containing skeletal animals and motile predators, and the second would be largely uninhabitable [83,84]. These issues can be partly resolved by considering the systematics of each geochemical proxy, and exactly what information they provide about the redox structure of ancient environments.
Minimum oxygen levels are necessary, but not sufficient, to explain the appearance of new species or ecological traits. Simple sponge-grade animals have very low oxygen demands (1–10 µM) [81], and these requirements appear to have been met continuously in surface waters from at least 800 Ma onwards [11]. During the Neoproterozoic, there may have been progressive increase in the maximum dissolved O2, enabling the development of more aerobically demanding traits, such as motility and bioturbation. However, for most of the Ediacaran, many proxies suggest widespread anoxic deep waters [18,19]. Ecosystem dynamics, animal distributions and migration patterns will be influenced by this reduction in habitable space, but clearly, early animal communities continued to thrive in shallow, well-oxygenated shelf environments where their oxygen demands were met [25,31]. It is therefore important to constrain the maximum O2(aq) available in shelf environments, as well as the spatial extent of inhospitable environments.
The marine redox landscape in the Cryogenian and Ediacaran appears to have been highly dynamic. It has been suggested that OOEs could have stimulated evolution, and their frequency appears to increase in the late Ediacaran and Cambrian, coincident with an intense period of diversification [17]. Periods of anoxia in between OOEs could even stimulate the development of genetic diversity [82]. Geochemical data and model results suggest that although the Neoproterozoic redox landscape was dynamic, there was no permanent change towards stable, well-oxygenated oceans until at least the Devonian, likely assisted by the evolution of land plants [7,10,14,15,29,55].
6. Conclusion and future directions
The proxy data are best reconciled in the following way: atmospheric O2 reached a concentration of greater than 0.1% PAL by around approximately 800 Ma and potentially earlier. Surface waters in contact with this atmosphere contained low levels of dissolved oxygen, but the deep oceans remained anoxic. Atmospheric oxygen probably rose in steps or pulses throughout the Cryogenian and Ediacaran, associated with major events such as the break-up of Rodinia, and the Sturtian, Marinoan and Gaskiers glaciations. The post-Sturtian is also marked by the first brief OOEs, which continue into the Cambrian. There is some evidence for OOE magnitude increasing over time [6], and a gradual rise in oxygen over the Neoproterozoic is also consistent with selenium isotope data [12]. By the start of the Cambrian, pO2 surpassed 30–40% PAL, but oxygen concentrations in much of the deep ocean remained low and the OMZ was thick and shallow. Atmospheric oxygen rose again in the Late Silurian, surpassing 70% PAL, and rose to modern-like levels in the Devonian, pushing the OMZ back off the shelf and establishing modern, well-oxygenated oceans (figure 3d). The COPSE model is unable to reproduce the full complexity revealed by geochemical data, but does capture first-order patterns of atmospheric and marine oxygenation from the Ediacaran onwards, giving confidence that the behaviour we see in the proxies is reasonable. The hypothesized NOE would be more accurately described as a Neoproterozoic Oxygenation Window, featuring dynamic pulses of oxygenation against a background of gradually rising oxygen levels, and any step change towards stable, well-oxygenated conditions appears to have been delayed until the Palaeozoic Oxygenation Event.
Moving forward, we need to consider which geochemical data can best capture this transition. To understand the timing, frequency and duration of OOEs, we need to target high-resolution continuous successions and analyse multiple global redox proxies. To meaningfully address questions surrounding the role of oxygen in early animal ecosystems, we need to focus on developing quantitative constraints on maximum O2(aq). These could include proxies for atmospheric oxygen, such as Cr isotopes, or marine redox proxies that respond to intermediate redox conditions, such as Ce anomalies and I/Ca. Detailed four-dimensional maps across shelf ecosystems can reveal the structure of marine anoxia (i.e. pancake versus OMZ) and be tied directly to the fossil record.
Supplementary Material
Acknowledgements
We are grateful to Zunli Lu and Noah Planavsky for reviews that helped to improve the manuscript. We thank the Royal Society for supporting us to attend a meeting in London where these ideas were discussed.
Data accessibility
The geochemical data are all published elsewhere and discussed in full in the relevant references. Differential equations and fixed parameters from the model are available in the electronic supplementary material. All modelling code and outputs can be obtained from B.J.W.M. on request.
Authors' contributions
R.T. compiled proxy data, and B.J.W.M. modified the COPSE biogeochemical model. R.T. and B.J.W.M discussed the results and wrote the manuscript together.
Competing interests
The authors declare no competing interests.
Funding
R.T. is supported by a grant from the DSI-NRF Centre of Excellence in Palaeosciences and B.J.W.M is funded by the UK Natural Environment Research Council (NE/R010129/1 and NE/S009663/1) and by a University of Leeds Academic Fellowship.
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Data Availability Statement
The geochemical data are all published elsewhere and discussed in full in the relevant references. Differential equations and fixed parameters from the model are available in the electronic supplementary material. All modelling code and outputs can be obtained from B.J.W.M. on request.