Significance
The rise of atmospheric oxygen over Earth’s history has received much recent interdisciplinary attention. However, the puzzle of when and how atmospheric oxygen reached modern levels remains unresolved. Many recent studies have argued for a major oxygenation event—of uncertain cause—in the Neoproterozoic Era >541 Ma, enabling the rise of animals. Previous modelling work has predicted a late Paleozoic oxygen rise (<380 Ma) due to the rise of forests. Here we show that neither scenario is correct. Instead, the earliest plants, which colonized the land from 470 Ma onward, first increased atmospheric oxygen to present levels by 400 Ma, and this instigated fire-mediated feedbacks that have stabilized high oxygen levels ever since, shaping subsequent evolution.
Keywords: oxygen, Paleozoic, phosphorus, plants, weathering
Abstract
The progressive oxygenation of the Earth’s atmosphere was pivotal to the evolution of life, but the puzzle of when and how atmospheric oxygen (O2) first approached modern levels (∼21%) remains unresolved. Redox proxy data indicate the deep oceans were oxygenated during 435–392 Ma, and the appearance of fossil charcoal indicates O2 >15–17% by 420–400 Ma. However, existing models have failed to predict oxygenation at this time. Here we show that the earliest plants, which colonized the land surface from ∼470 Ma onward, were responsible for this mid-Paleozoic oxygenation event, through greatly increasing global organic carbon burial—the net long-term source of O2. We use a trait-based ecophysiological model to predict that cryptogamic vegetation cover could have achieved ∼30% of today’s global terrestrial net primary productivity by ∼445 Ma. Data from modern bryophytes suggests this plentiful early plant material had a much higher molar C:P ratio (∼2,000) than marine biomass (∼100), such that a given weathering flux of phosphorus could support more organic carbon burial. Furthermore, recent experiments suggest that early plants selectively increased the flux of phosphorus (relative to alkalinity) weathered from rocks. Combining these effects in a model of long-term biogeochemical cycling, we reproduce a sustained +2‰ increase in the carbonate carbon isotope (δ13C) record by ∼445 Ma, and predict a corresponding rise in O2 to present levels by 420–400 Ma, consistent with geochemical data. This oxygen rise represents a permanent shift in regulatory regime to one where fire-mediated negative feedbacks stabilize high O2 levels.
After the well-defined “Great Oxidation Event” 2.45–2.32 Ga, the trajectory of atmospheric oxygen is deeply uncertain (1, 2). Many recent studies, reviewed in refs. 3–5 have argued for a Neoproterozoic oxygenation event (>550 Ma)—of uncertain cause—and have linked it to the rise of animals, but this has been questioned given a lack of change in iron speciation ocean redox proxy data (6). Some models predict pO2 ∼1 present atmospheric level (PAL) already in the Early Paleozoic (7, 8), but this is at odds with data for widespread ocean anoxia (6, 9). The COPSE model we adapt here (10) predicts Early Paleozoic pO2 ∼0.2–0.5 PAL consistent with redox proxy data but, like the other models (7, 8), it does not predict a rise in oxygen until the advent of forests starting ∼385 Ma, and continuing until ∼300 Ma, which is too late to explain marked changes in geochemical data that occur before ∼390 Ma (Fig. 1). The first appearance of fossil charcoal in the Late Silurian (11) and its ongoing occurrence through the Devonian (12) (Table S1), albeit rare and at low concentrations, indicates O2 > 15–17% (vol) of the atmosphere (13) (or O2 > ∼0.7 PAL assuming a constant N2 reservoir) already by ∼420–400 Ma. [Under ideal conditions of ultradry fuel and forced airflow, smoldering fires may be sustained at O2 > 10%, but this is not believed to be possible under natural conditions (14).] The molybdenum isotope record (9) indicates a fundamental shift in the redox state of the deep ocean from widespread anoxia to widespread oxygenation sometime during 435–392 Ma (between the Early Silurian and the Middle Devonian). This ocean oxygenation is also supported by a Silurian increase in the C/S ratio of shales (15), and a shift in iron speciation data sometime during 435–387 Ma (6).
Table S1.
Ref(s). | 2° | Type | Stratigraphy | Stage | Age, Ma | Location | N | Inertinite, % mmf |
11 | 12, 44 | Fossils | Platyschima Shale Mbr, Downton Fm | Basal Pridoli | 423.0–419.2 | Ludford Lane, Ludlow, United Kingdom | ||
48, 49 | 12, 44 | Fossils | Ditton Gp | Early Lochkovian | 419.2–410.8 | N. Brown Clee Hill, United Kingdom | ||
50, 51 | 12 | Fossils | Pragian/Emsian | 410.8–393.3 | KTB core, Bavaria, Germany | |||
28 | Coaly shale | Val d’Amour Fm | Pragian | 410.8–407.6 | New Brunswick, Canada | 4 | 0.8 | |
28 | Coaly shale | Campbellton Fm | Emsian | 407.6–393.3 | New Brunswick, Canada | 4 | 0.0 | |
45 | 45 | Coal | L’Anse-a-Brillant coal | Early Emsian | 407.6–393.3 | Tar Point, Gaspe, Canada | 1 | 0.2 |
52 | 46 | Fossil | Emsian | 407.6–393.3 | Bad Munstereifel, Germany | 1 | 1.5 | |
53 | 47 | Coal | Wapsinicon Fm, Davenoport Mbr | Eifelian | 393.3–387.7 | IL | 3 | 0.0 |
54–57 | 45, 46 | Coal | Barzas coal | Eifelian–Givetian | 393.3–382.7 | Barzas, Estonia | 4 | 1.5 |
58 | 47 | Coal | Nannyara Sandstone | Givetian | 387.7–382.7 | Carnarvon Basin, Australia | 1 | 2.0 |
58 | 47 | Coal | Nannyara Sandstone | Givetian | 387.7–382.7 | Carnarvon Basin, Australia | 1 | 0.0 |
59 | 47 | Coal | Hujiersite Fm | Givetian | 387.7–382.7 | North Xinjiang, China | 1 | 0.0 |
60 | 45 | Coal | Givetian | 387.7–382.7 | China | 0.0 | ||
61 | 45, 46 | Coal | Givetian | 387.7–382.7 | Luquan, Yunnan, China | 8 | 0.1 | |
52 | 45, 46 | Coal | Givetian–Frasnian boundary | 382.7 | Mimerdalen, Spitsbergen | 1 | 0.0 | |
62–65 | 12, 44, 45 | Coal | Weatherall Fm | Late Givetian–Middle Frasnian | 387.7–372.2 | W. Melville Island, Canada | 8 | 1.3 |
62–65 | 12, 44, 45 | Coal | Hecla Bay Fm | Late Givetian–Middle Frasnian | 387.7–372.2 | W. Melville Island, Canada | 13 | 2.3 |
62–65 | 12, 44, 45 | Coal | Beverley Inlet Fm | Early–Middle Frasnian | 382.7–372.2 | W. Melville Island, Canada | 6 | 0.7 |
66 | 47 | Coal | Roedvika Fm, Tunheim Mbr, seam A | Late Famennian | 372.2–358.9 | Bjornoya, Norway | 11 | 36.7 |
66 | 47 | Coal | Roedvika Fm, Tunheim Mbr, seam B | Late Famennian | 372.2–358.9 | Bjornoya, Norway | 7 | 61.9 |
67 | 12 | Black shale | Huron Shale Mbr, New Albany Shale | Famennian (oldest) | 372.2–358.9 | D6 core, KY | 40 | 10.3 |
67 | 12 | Black shale | Three Lick Bed, New Albany Shale | Famennian (middle) | 372.2–358.9 | D6 core, KY | 3 | 17.8 |
67 | 12 | Black shale | Cleveland Shale Mbr, New Albany S. | Famennian (youngest) | 372.2–358.9 | D6 core, KY | 17 | 23.7 |
44 | 44 | Black shale | New Albany Shale, Ohio Shale | Famennian | 372.2–358.9 | IRQ, D4, D6, OHLO2 cores | ||
68 | 44 | Black shale | Hangenberg Black Shale | Latest Famennian | 372.2–358.9 | Kowala Quarry, Poland | ||
44 | 44 | Fossils | Hampshire Fm | Famennian | 372.2–358.9 | Elkins, WV | ||
69 | 12, 44 | Fossils | Duncannon Mbr, Catskill Fm | Famennian 2c | 372.2–358.9 | Red Hill, PA | ||
70 | 12 | Fossils | Hangenberg Sandstein | Late Famennian | 372.2–358.9 | Oese, Sauerland, Germany | ||
71 | 12, 44 | Fossils | Knoppenbissen Fm | Famennian | 372.2–358.9 | Refrath 1 Borehole, Germany | ||
72 | 44 | Fossils | Evieux Fm, Condroz Gp | Late Famennian | 372.2–358.9 | Three quarries, Belgium |
Fm, formation; Gp, group; Mbr, member.
The persistent oxygenation of the ocean and appearance of charcoal can be explained by a rise in atmospheric oxygen occurring by ∼400 Ma; this could be due to a persistent increase in oxygen source—considered here—or a decrease in oxygen sink (16), leading to a reorganization of the Earth’s surface redox balance at a higher steady-state level for atmospheric O2. The major long-term source of oxygen to the atmosphere is the burial of organic carbon in sedimentary rocks (which represents the net flux of photosynthesis minus various pathways of respiration and oxidation). Increases in global organic carbon burial are recorded as positive shifts in the isotopic composition of carbonate rocks (δ13C). Consistent with a rise in oxygen, the carbon isotope record (17) (Fig. 1) indicates a fundamental shift in baseline from ≤0‰ before the Late Ordovician to ∼2‰ from ∼445 Ma onward. Though there are many subsequent δ13C fluctuations, including drops back to 0‰, for example, at ∼400 Ma, the long-term mean δ13C remains ∼2‰ throughout the rest of the Paleozoic, the Mesozoic, and the Early Cenozoic (17), indicating a sustained increase in global organic carbon burial. Such a permanent shift requires a unidirectional driver that kicked in during the mid-Paleozoic. The evolution of land plants is the obvious candidate, with the first nonvascular plants (ancestors of extant mosses, liverworts, and hornworts) colonizing the land in the Middle to Late Ordovician (∼470–445 Ma), followed by the first vascular plants in the Silurian (∼445–420 Ma) and Early Devonian (∼420–390 Ma; Fig. 1) (18, 19).
Here we hypothesize that the evolution of these earliest land plants permanently increased organic carbon burial, causing atmospheric oxygen to approach modern levels by ∼400 Ma and creating a new dynamically stable steady state for the oxygen cycle (where the major long-term O2 sink from oxidative weathering of ancient organic carbon increased to counterbalance the increased O2 source). In simple terms, on long timescales, the global organic carbon burial flux is determined by the supply flux of the ultimate limiting nutrient phosphorus from weathering and the (molar) ratio of carbon-to-phosphorus in material that is buried
Land plants typically have a much higher molar C/P ratio (∼1,000) than marine organic matter (∼100) due to carbon-rich but phosphorus-poor structural compounds such as sporopollenin, lignin, and, in their fungal mycorrhizal symbionts, chitin; therefore, they can support an increased organic carbon burial flux for the same P weathering flux. The P weathering flux is partly tied to bulk silicate weathering, for example, due to the dissolution of apatite inclusions in silicate rocks, and the silicate weathering flux of alkalinity is in turn set by negative feedback in the long-term carbon cycle, so is ultimately controlled by the degassing input of CO2 on timescales ≥1 My (7, 10). However, plants and their associated mycorrhizal fungi can increase phosphorus weathering (20–22), and this could be sustained on longer timescales if they preferentially weather phosphorus relative to alkalinity.
In existing models, the evolution of trees starting ∼385 Ma is assumed to have led to the burial of high C/P organic material in coal swamps (7, 8, 10), potentially augmented by increased phosphorus weathering rates (10). The Carboniferous–Permian peak in coal production has often been attributed to the evolution of lignin synthesis and a lag before the evolution of fungal degradation of lignin (23), but recent work has questioned this (24). Earlier plants possessed lignified “woody” tissue (25), with precursor structures existing in marine algae before the transition to land (26), and lignin-degrading fungi potentially present before the Carboniferous (24). Carboniferous coals are not dominated by lignin; instead, their accumulation was controlled by a combination of climate and tectonics supporting the creation and sedimentary preservation of peat bogs (24, 27). Given that earlier plants developed peatlands (28), and had rock-weathering capabilities (20, 21), they could also have affected the global carbon cycle (18, 20).
Results and Discussion
To test our hypothesis, we revised the COPSE biogeochemical model (10) to better capture the early rise of plants and examine under what conditions it could explain the geochemical data (persistent rise to δ13C ∼2‰ and the appearance of charcoal). The original baseline model (10) predicts early Paleozoic O2 ∼0.23 PAL at a reference time of 445 Ma, supported by an organic carbon burial flux of ∼4 × 1012 mol⋅y−1 (about half the present-day value) with δ13C = 0.03‰. In this stable state, oxidative weathering of ancient organic carbon is correspondingly reduced and its sensitivity to changes in O2 provides a key negative feedback stabilizing O2. Key assumptions going into altering the forcing of the model are the global extent and associated productivity of early plants, the C/P ratio of plant material that was buried, and their effect (if any) on phosphorus weathering. To help parameterize these factors we drew on a mixture of experiments, existing data, and more detailed spatial modeling.
We used a trait-based spatial model of cryptogamic vegetation (i.e., bryophyte and lichen) cover (29, 30) driven by Late Ordovician climate simulations (31) at different atmospheric CO2 levels to predict the potential global net primary productivity (NPP) of the early plant biosphere (32). At atmospheric CO2 = 8 PAL, consistent with Late Ordovician glaciations (20), predicted global NPP is ∼19 GtC⋅y−1 (GtC, billion metric tons of carbon) (Fig. 2), ∼30% of today. Predicted NPP is sensitive to variations in CO2 and climate (Fig. S1), ice sheet cover (Fig. S2), and O2 (Table S2), but is consistently higher than the 4.3 GtC⋅y−1 (7% of today) estimated elsewhere (33). In the original COPSE model (10), predicted NPP only reaches ∼5% of today’s value in the Late Ordovician and Silurian, but when we assume a stronger Late Ordovician phase of land colonization by nonvascular plants (following ref. 20; SI Materials and Methods), then COPSE predicts global NPP 30–40% of today (Fig. 3A), consistent with the detailed spatial model. In COPSE, this advent of early land plants alone, with no assumed effect on weathering fluxes, and assumed C/P = 1,000, increases total organic carbon burial by ∼25%, δ13C by 0.5‰, and atmospheric O2 by 0.11 PAL (Fig. 3, blue).
Table S2.
CO2, PAL | O2, PAL | ||
0.2 | 0.6 | 1.0 | |
4 | 8.0 | 7.8 | 7.7 |
8 | 19.4 | 18.7 | 18.3 |
16 | 28.1 | 27.1 | 26.5 |
We undertook a literature review of molar C/P ratios in extant bryophytes (Table S3) to test whether C/P = 1,000 is a reasonable assumption for early plants, and this gives a range of C/P = 800–4,300 with a mean of C/P ∼1,900. Furthermore, Early Devonian coaly shales indicate extensive peatlands 410–400 Ma and have C/N of 44–119 (28), comparable to that in modern peatlands where N/P and C/P ratios tend to increase with depth to C/P > 3,000 (34). Taken together, these data suggest that assuming C/P = 1,000 for early plants is conservative. If instead we assume that buried early plant matter had C/P = 2,000, then given their productivity, even with no effect on weathering fluxes, this increases global organic carbon burial by ∼50%, δ13C by 1.1‰, and atmospheric O2 by 0.27 PAL (Fig. 3, cyan).
Table S3.
Species/identifier | N | Mg P/g biomass | Mg C/g biomass | C/P mass | C/P molar | Ref. |
Aulacomnium spp. | 6 | 0.8 | 430* | 540 | 1,400 | 80 |
Polytrichum spp. + Pogonatum spp | 6 | 0.7 | 430* | 610 | 1,600 | 80 |
Aulacomnium turgidum | 1 | 430* | 430 | 1,100 | 81 | |
Hylocomium splendens | 0.9 | 430* | 480 | 1,200 | 81 | |
Aulacomnium turgidum | 4 | 1.2 | 430* | 360 | 920 | 82 |
Hylocomium splendens | 4 | 1.1 | 430* | 390 | 1,000 | 82 |
Sphagnum rubrum | 4 | 0.8 | 430* | 540 | 1,400 | 82 |
Bryophyte tussock site | 1 | 430* | 540 | 1,400 | 83 | |
Bryophyte shrub site | 0.8 | 430* | 330 | 850 | 83 | |
Bryophyte wet site | 1.3 | 430* | 310 | 790 | 83 | |
Bryophyte heath site | 1.4 | 430* | 860 | 2,200 | 83 | |
Sphagnum spp. | 43 | 0.56 | 430* | 770 | 2,000 | 84 |
Warnstorfia fluitans | 0.5–2.4 | 410–470 | 550–950 | 1,400–2,400 | 85 | |
12 species across altitudes and soil ages | 0.33–0.63 | 729–1,550 | 1,900–4,000 | 86 | ||
Sphagnum spp. | 0.6–0.8 | 700–1,000 | 1,800–2,600 | 87 | ||
Sphagnum spp. foliage | 794 | 2,050 | 34 | |||
Sphagnum spp. litter | 911 | 2,350 | 34 | |||
Sphagnum spp. peat | 1285 | 3,310 | 34 | |||
Sphagnum meadow | 1 | 515 | 1,330 | 88 | ||
Sphagnum mesotrophic fen flark | 1.6 | 414 | 1,070 | 88 | ||
Sphagnum mesotrophic fen hummock | 0.8 | 733 | 1,890 | 88 | ||
Sphagnum oligotrophic fen flark | 0.6 | 722 | 1,860 | 88 | ||
Sphagnum oligotrophic fen hummock | 0.5 | 999 | 2,580 | 88 | ||
Sphagnum fen-bog transition flark | 0.4 | 1,376 | 3,550 | 88 | ||
Sphagnum fen-bog transition hummock | 0.3 | 1,655 | 4,270 | 88 |
Mean value across six bryophyte species from ref. 89.
Early plants could also have had a significant effect on weathering fluxes (20), because they and their fungal mycorrhizal symbionts evolved means of accessing rock-bound nutrients, notably phosphorus. Experimental work (20) has shown that a modern nonvascular plant, the moss Physcomitrella patens, amplifies the weathering of Ca ions 1.4- to 3.6-fold and Mg ions 1.5- to 5.4-fold from silicate rocks (granite–andesite), and amplifies the weathering of phosphorus from granite ∼24-fold (range 15–43; Materials and Methods). Subsequent experiments (21) with the modern liverwort Marchantia paleacea found a 2.5- to 7-fold amplification of Ca weathering and a 9- to 13-fold amplification of P weathering from basalt. Both studies thus indicate preferential weathering of P relative to Ca and Mg (and corresponding alkalinity). The presence of these rock-weathering capabilities in two early diverging lineages (mosses and liverworts) suggests it is an ancestral trait. It has been argued (21, 33) that such large measured local effects would not have scaled up to significant global effects, because of low global NPP (33) and a limited depth of influence in the soil (21). However, we estimate much higher global NPP (Fig. 2) and weathering potential (32). We also note that extensive shallow water phosphate deposits in the Late Ordovician (35) indicate a marked increase in phosphorus input to the ocean (20).
If we include in COPSE an effect of early plants on silicate weathering following ref. 20, assuming C/P = 1,000, this increases organic carbon burial by ∼35%, δ13C by 0.7‰, and O2 by 0.18 PAL (Fig. 3, magenta). The effect on O2 is constrained because atmospheric CO2 and temperature are reduced (20) such that the silicate weathering flux (and associated phosphorus flux) continues to match the degassing flux of CO2 (Fig. S3). However, increases in carbonate weathering (enhanced by plants) and oxidative weathering (due to the rise in O2) increase the overall phosphorus weathering flux, roughly doubling the O2 rise due to terrestrial production of high C/P material alone. Assuming that buried early plant matter had a higher C/P = 2,000 causes larger increases in total organic carbon burial ∼60%, δ13C + 1.2‰, and atmospheric O2 + 0.35 PAL (Fig. 3, green).
However, to reproduce the observed δ13C +2‰ shift requires the inclusion of some selective weathering of phosphorus by early plants. Assuming that early plants caused a sustained 50% increase in phosphorus weathering relative to bulk rock dissolution, with C/P = 1,000, increases total organic carbon burial by ∼95%, δ13C by 2.2‰, and O2 by 0.74 PAL (to 0.97 PAL at 417 Ma; Fig. 3, yellow). Assuming a sustained 25% increase in phosphorus weathering relative to bulk rock and C/P = 2,000 increases organic carbon burial by ∼90%, δ13C by 2.1‰, and O2 by 0.67 PAL (Fig. 3, red). Alternatively, a series of P weathering spikes designed to reproduce the observed sequence of positive δ13C excursions (Fig. 1), combined with C/P = 2,000, produces a series of spikes in organic carbon burial and a peak increase of O2 of 0.72 PAL at 407 Ma (Fig. 3, black). We hypothesize that these assumed weathering spikes could reflect phases of plant colonization (20, 36) followed by the establishment of phosphorus recycling ecosystems (20). However, direct evidence linking a phase of land colonization to enhanced weathering and a positive δ13C excursion has only thus far been established for the Silurian–Devonian boundary excursion (36). Therefore, alternative hypotheses for short-lived positive δ13C excursions should also be considered.
Regarding the simulated long-term ∼2‰ rise in δ13C, this is smaller than would be expected from standard application of the simplified formula: δ13C(ocean) = δ13C(river) + forg∙ε, where forg is the fraction of carbon buried as organic matter, ε is the fractionation between carbonates and organic matter, and both ε and δ13C(river) are usually assumed to be constant. In our COPSE simulations there is a fully interactive isotope mass balance, and these terms are not constant. The approximate doubling of organic carbon burial (with roughly constant carbonate burial) represents an increase from forg = 0.18 to forg = 0.31. However, the increase in burial of isotopically light organic carbon is counteracted by an increase in the oxidative weathering of isotopically light organic carbon, which lowers the δ13C of riverine input to the ocean from approximately −5‰ to approximately −7.5‰, which is in turn partially counteracted by an increase in fractionation between carbonates and organic matter from ε ∼27 to ∼30‰, due to increasing O2 (somewhat counteracted by declining CO2).
Sensitivity analyses (SI Materials and Methods) indicate that our results are robust. Varying the uplift and degassing forcing of the model within plausible bounds only causes ±0.08 PAL variation in O2 about the initial state (Fig. S4), although it does cause the effect of the same early plant forcing scenario to range over +0.4 to 1.0 PAL O2 (Table S4). Including an additional negative feedback on O2, from increased marine organic C/P burial ratios under anoxic waters (37), increases its initial early Paleozoic level to 0.54 PAL and reduces the effect of the same biological forcing scenarios on O2 by ∼10–30%, giving a maximum increase of +0.63 PAL (Table S5). However, because the initial O2 is now higher, the final O2 is also higher in all cases, and even scenarios without selective weathering of phosphorus could explain the appearance of charcoal (O2 > ∼0.7 PAL).
Table S4.
Forcing scenario | Uplift | Degassing | Biology | FOrg-C, mol/y | Δδ13C, ‰ | ΔCO2, PAL | ΔO2, PAL |
445 Ma | 445 Ma | 445 Ma | 410 Ma | ||||
Original baseline | B | B | B | 4.1 × 1012 | 0 | 0 | 0 |
New baseline | R | R | B | 4.4 × 1012 | −0.1 | −1.3 | −0.01 |
Strong uplift | R + 20% | R | B | 4.7 × 1012 | −0.2 | −3.3 | −0.04 |
Weak uplift | R − 20% | R | B | 4.1 × 1012 | 0.0 | 1.4 | 0.03 |
Strong degassing | R | R + 20% | B | 5.0 × 1012 | 0.0 | 0.8 | 0.04 |
Weak degassing | R | R − 20% | B | 3.8 × 1012 | −0.2 | −3.7 | −0.05 |
Strong U, weak D | R + 20% | R − 20% | B | 4.0 × 1012 | −0.3 | −5.4 | −0.08 |
Weak U, strong D | R − 20% | R + 20% | B | 4.7 × 1012 | 0.1 | 3.8 | 0.08 |
Original baseline | B | B | E + W + F(i) | 8.0 × 1012 | 2.2 | −8.4 | 0.74* |
New baseline | R | R | E + W + F(i) | 8.3 × 1012 | 2.0 | −9.6 | 0.72 |
Strong uplift | R + 20% | R | E + W + F(i) | 8.9 × 1012 | 1.7 | −11 | 0.60 |
Weak uplift | R − 20% | R | E + W + F(i) | 7.6 × 1012 | 2.3 | −8.0 | 0.85 |
Strong degassing | R | R + 20% | E + W + F(i) | 9.5 × 1012 | 2.3 | −8.3 | 0.89 |
Weak degassing | R | R − 20% | E + W + F(i) | 7.1 × 1012 | 1.7 | −11 | 0.51 |
Strong U, weak D | R + 20% | R − 20% | E + W + F(i) | 7.5 × 1012 | 1.4 | −12 | 0.40 |
Weak U, strong D | R − 20% | R + 20% | E + W + F(i) | 8.7 × 1012 | 2.6 | −6.5 | 1.01 |
B, baseline; R, Royer et al. (91).
With the original geologic forcing, this peak increase in O2 occurs earlier at 417 Ma.
Table S5.
Feedback structure | Biology scenario | FOrg-C, mol/y | Δδ13C, ‰ | ΔCO2, PAL | ΔO2, PAL | O2, PAL |
445 Ma | 445 Ma | 445 Ma | Peak* | Peak* | ||
Original baseline | B (baseline) | 4.1 × 1012 | 0 (0.03) | 0 (17.2) | 0 | (0.23) |
E | 5.1 × 1012 | 0.5 | −0.6 | 0.11 | 0.34 | |
E + CP | 6.1 × 1012 | 1.1 | −1.5 | 0.27 | 0.50 | |
E + W | 5.6 × 1012 | 0.7 | −7.5 | 0.18 | 0.41 | |
E + CP + W | 6.5 × 1012 | 1.2 | −8.0 | 0.35 | 0.58 | |
E + W + F(i) | 8.0 × 1012 | 2.2 | −8.4 | 0.74 | 0.97 | |
E + CP + W + F(ii) | 7.8 × 1012 | 2.1 | −8.5 | 0.67 | 0.90 | |
E + CP + W + F(iii) | 6.6 × 1012† | 1.2† | −7.9† | 0.72‡ | 0.97‡ | |
(C/P)org = f(O2) | B (baseline) | 6.1 × 1012 | 0.7 | 0.2 | 0.31 | 0.54 |
E | 6.6 × 1012 | 1.0 | −0.6 | 0.38 | 0.61 | |
E + CP | 7.3 × 1012 | 1.5 | −1.2 | 0.49 | 0.72 | |
E + W | 7.1 × 1012 | 1.2 | −7.2 | 0.47 | 0.70 | |
E + CP + W | 7.7 × 1012 | 1.6 | −7.5 | 0.57 | 0.80 | |
E + W + F(i) | 9.4 × 1012 | 2.9 | −7.9 | 0.96 | 1.19 | |
E + CP + W + F(ii) | 9.0 × 1012 | 2.5 | −7.9 | 0.84 | 1.07 | |
E + CP + W + F(iii) | 7.7 × 1012† | 1.5† | −7.4† | 0.92‡ | 1.17‡ |
Typically occurs during 430–415 Ma.
This is just before a sharp peak in FOrg-C and δ13C, and a sharp minimum in CO2.
Peak occurs at 407 Ma when baseline O2 = 0.25 PAL.
Our model makes additional predictions that can be tested against geochemical data—notably, it predicts a decline in pyrite sulfur burial and associated drop in δ34S and increases in seawater SO4 concentration and C/S burial ratio with the rise of the earliest plants (Fig. S5). This finding is broadly consistent with the sulfur isotope (δ34S) record (38–40), which shows a marked decline through the Silurian–Early Devonian from ∼30 to ∼18‰, although available data also suggest an earlier Late Ordovician–Early Silurian rise from ∼25 to ∼30‰, which the present model does not capture. The model is consistent with proxy reconstructions of seawater SO4 concentration, which suggest an Ordovician–Silurian rise from ∼6 to ∼10 mM (41), and with a Silurian increase in the molar C/S ratio of shales from ∼5 to ∼16 (15).
Other processes not yet included in the model warrant future consideration—for example, the effect of increasing atmospheric mass on climate (42) and the effect of weathering forcing scenarios on δ7Li and 87Sr/86Sr, which enable additional tests against data.
SI Materials and Methods
Biological Forcing Scenarios.
We use several different runs of the COPSE model, in which we alter individually and in combination the different biological forcing factors, to explore the potential effects of early plants. The scenarios are based on previous work (20) but updated and extended to span the interval of the Late Ordovician–Silurian–Early Devonian. Our reference scenario is as follows:
(B) Baseline run: This is the original model (10) prescription of changing solar, geological, and biological forcing over the focal interval; this includes very subtle early plant colonization E = 0→0.02 over 465–440 Ma, constant until 420 Ma, then E = 0.02→0.15 over 420–400 Ma, which is combined with W = 0→0.02 over 465–440 Ma, constant until 420 Ma, then W = 0.02→0.1 over 420–400 Ma. Because E and W are effectively multiplied together in the weathering equations of the model (10), the resulting effects on weathering are tiny. However, the rise of E combined with C/P = 1,000 causes a small burial flux of terrestrial organic matter ∼0.2 × 1012 mol/y up to 420 Ma, rising to ∼1.2 × 1012 mol/y at 400 Ma and ∼1.5 × 1012 mol/y at 390 Ma; this has no significant effect on O2 until after 420 Ma, but it does cause O2 to rise from 0.22 to 0.23 PAL at 420–410 Ma to ∼0.26 PAL at 400 Ma and ∼0.31 PAL at 390 Ma. (For this reason, the effect of the following scenarios on O2 tends to be greatest at 420–410 Ma.)
In adjusting from the reference scenario, we first add
(E) Early plant colonization: The forcing parameter E was altered to explore the effects of early plant evolution/colonization. We assume: E = 0 up to 465 Ma, then linear rise to E = 0.15 at 445 Ma, remaining constant until 400 Ma, where it joins with the original scenario: this is the same magnitude of change in E as in ref. 20 but is slightly later in timing (previously the increase in E was imposed over 475–460 Ma), partly reflecting updates to the geologic timescale for this interval.
We then add the following different biological effects to scenario (E), either individually or in combination:
(CP) Effects on C/P burial ratio: The molar C/P burial ratio of terrestrially derived organic matter was altered to explore the effects of the high C/P ratio observed in extant bryophytes and the peats that they produce (Table S3). We assume an increase from C/P = 1,000 to C/P = 2,000 over 465–445 Ma, constant thereafter, which rejoins the original scenario at 345 Ma. (Later on, C/P declines to 1,000, which is assumed to be due to the evolution of lignin degrading fungi and a decline in coal-producing peatlands.)
(W) Effects on silicate (and carbonate) weathering: The forcing parameter W was altered to explore the effects of early plant enhancement of silicate (and carbonate) weathering. We assume W = 0 up to 465 Ma, then linear rise to W = 0.75 at 445 Ma, then constant, rejoining the original scenario at ∼300 Ma; this is the same increase in W as in ref. 20, just somewhat later in timing.
(F) Effects on phosphorus weathering: The forcing parameter F was increased to explore the effects of selective weathering of phosphorus by early plants in an attempt to try and reproduce the timing of key changes in the δ13C record. We explore several variants:
-
i)
In an attempt to capture the +2‰ plateau in δ13C, we assume F = 1 up to 465 Ma, then linear rise to F = 1.5 at 445 Ma, held constant over 445–410 Ma, then a linear reduction back to F = 1 at 400 Ma.
-
ii)
As i but increasing to F = 1.25 (for use with C/P = 2,000).
-
iii)
Spikes of phosphorus weathering. Sharp increases then decreases of phosphorus weathering were introduced to reproduce the positive excursions in the δ13C record known as the GICE, HICE, Ireviken, Mulde, Lau, and Klonk events, and a pronounced Early Devonian positive excursion. These short duration perturbations are conceived here as possible phases of land colonization involving weathering of relatively bare rock terrains, followed by the establishment of phosphorus recycling soil systems with an attendant drop in the flux of phosphorus weathering. Their timing and duration was based on the latest carbon isotope stratigraphy (17). The spikes we impose are: (GICE) F = 1→2.5→1 over 453→452.5→452 Ma, (HICE) F = 1→3.5→1 over 445→444.5→444 Ma, (Ireviken) F = 1→2→2→1 over 433.25→433→432→431.5 Ma, (Mulde) F = 1→1.5→1 over 430→429→428 Ma, (Lau) F = 1→3→1 over 424.75→424.25→423 Ma, (Klonk) F = 1→2.25→1 over 420→419→418 Ma, (early Devonian) F = 1→1.5→1.5→1 over 416→415→408→404 Ma. (The early GICE and HICE spikes contrast in timing and duration somewhat from ref. 20. where F = 1→2→1 over 460→458→456 Ma, and F = 1→3→1 over 447→445→443 Ma, due to updates of the geological timescale and carbon isotope stratigraphy in this interval.)
Results for these scenarios are given in Fig. 3 and Figs. S3 and S5, and some are given in Table S5, where changes in total organic carbon burial flux (FOrg-C), δ13C, and atmospheric CO2 are given at 445 Ma, which is typically a minor peak in FOrg-C, and the time of maximum change in δ13C and atmospheric CO2, whereas quoted peak changes in atmospheric O2 occur later.
Geological Forcing Sensitivity Analysis.
The original geologic forcing scenario over the Late Ordovician–Silurian–Early Devonian (460–400 Ma) has a generally high level of degassing (D) ∼1.5 (with a slight rise and then fall) relative to today, consistent with it being an interval of high levels of volcanic activity and formation of subduction zones. The original uplift forcing (U) is more variable, dropping from U ∼1.08 at 470 Ma, to a minimum U = 0.84 at 440 Ma, increasing to a maximum U = 1.04 at 410 Ma, then dropping again to U ∼0.8 at 390–380 Ma. This two-peak structure can be related to the main phases of mountain building of the Taconic orogeny and the Caledonian (Acadian) orogeny, separated by a more quiescent interval in the Early Silurian. However, the imposed drop in uplift U in the Middle to Late Ordovician was originally inferred from a significant drop in the 87Sr/86Sr composition of seawater, which could also have been due to extensive weathering of volcanic rocks with low 87Sr/86Sr composition, at a time of significant ongoing uplift associated with the Taconic orogeny.
To explore the consequences of uncertainty in the geologic (degassing and uplift) forcing of the model, we undertake a sensitivity analysis based on that conducted by Royer et al. (91) using the GEOCARBSULF model, but with an expanded uncertainty range; their uncertainty range on spreading rate over time, which is equivalent to degassing, is ±17.5%, whereas for dependence of weathering on relief, which is equivalent to uplift, it is only ±8% (because the GEOCARBSULF model tends to crash under wider ranges in input parameters). We opt for a consistent ±20% uncertainty range on both parameters, D and U, either side of the best-guess trajectories for them from ref. 91. The default degassing trajectory is similar to the original COPSE degassing forcing, whereas the default uplift trajectory is much smoother and only captures very long timescale variation with the supercontinent cycle. Nevertheless, a ±20% uncertainty range produces an envelope which encompasses the more temporally variable original COPSE uplift forcing (Fig. S4 A and B).
With the central estimates for degassing and uplift forcing from Royer et al. (91), the baseline run of the model is subtly altered during the focal interval 480–380 Ma (Fig. S4 C–F), due to the smoothing out of the uplift forcing, but the effects on organic carbon burial δ13C (<0.1‰) and atmospheric O2 (∼0.02 PAL) are small. Results of the sensitivity analysis for varying geological forcing are summarized in Table S4, where all results are given relative to the original baseline (including the effects of the new baseline geological forcing relative to the original baseline). Again, changes in total organic carbon burial flux (FOrg-C), δ13C, and atmospheric CO2 are given at 445 Ma, whereas changes in atmospheric O2 are given at 410 Ma, which is typically close to the time of maximum change in O2.
Sensitivity to Initial O2 Level (and Feedback Structure).
To explore the consequences of uncertainty in the feedback structure of the model, which in turn affects the initial atmospheric O2 level, we include an anoxia sensitivity of the C/P burial ratio of marine organic matter (37); this acts as a negative feedback on variations in atmospheric O2, and is equivalent to “run 2” of the original model (10). Including this feedback increases the baseline Paleozoic atmospheric O2 level in the model by ∼0.3 PAL (e.g., from 0.23 to 0.54 PAL at 420 Ma), by increasing organic carbon burial (and with that δ13C). From this alternative baseline O2 (and corresponding feedback structure), we explore the same range of biological forcing scenarios detailed above and in the main text, with the results presented in Table S5.
Conclusion
Our model can only reproduce Paleozoic geochemical data if the rise of the earliest land plants caused a major oxygenation event of the Earth’s atmosphere and oceans by ∼400 Ma. We attribute this mid-Paleozoic oxygenation event to a persistent global increase in organic carbon burial supported by the high C/P ratio of early land plant material, augmented by a plant-driven increase in P weathering flux relative to the weathering flux of alkalinity. The δ13C record suggests this increase in organic carbon burial was essentially permanent, producing a new dynamically stable state for atmospheric O2. In this new steady state, oxidative weathering was increased (becoming less sensitive to variations in O2) and new fire-mediated negative feedbacks on O2 were instigated that have played a key role in stabilizing atmospheric O2 concentration up to the present day (22, 43). For the earliest land plants to be responsible for such a major mid-Paleozoic oxygenation event requires that they were much more productive and globally extensive than has been previously assumed (7, 10, 33). This hypothesis makes testable predictions with regard to effects on other biogeochemical cycles, notably sulfur; if it stands up to further scrutiny, we can then infer that the earliest land plants created a stable oxygen-rich atmosphere that was necessary for the subsequent evolution of large, mobile, intelligent animals with a high respiratory oxygen demand, including ourselves.
Materials and Methods
Data Compilation.
The early charcoal record (Table S1) was compiled from the literature (11, 12, 28, 44–72) using existing compilations (12, 44–47) and checking them where possible against the original sources. This process involved some reconciling of disparate results between existing compilations and revision of some erroneous quoted values. Where recalculations were warranted, inertinite percentages were calculated on a mineral matter-free (mmf) basis, following refs. 45 and 47.
The molybdenum isotope record from marine shales was updated from ref. 9 with data from refs. 73 and 74. Uncertainties shown in Fig. 1 represent 2 SD of the mean (analytical precision) plus the propagated uncertainty from matching in-house reference materials to the universal standard NIST SRM 3136 where seawater display δ98/95Mo = 2.3‰ (75, 76). The redox state of the host shales was determined using either Fe speciation or Mo enrichment proxies. Euxinic shales are defined (77) by the Fe speciation proxy when FeHR/FeT > 0.38 and FeP/FeHR > 0.7 (black circles in Fig. 1). Euxinic shales are defined (78, 79) by the Mo enrichment proxy when Mo > 25 ppm (white circles in Fig. 1). Ferruginous shales (77) are defined by the Fe speciation proxy when FeHR/FeT > 0.38 and FeP/FeHR < 0.7.
The carbon isotope record (17) was fitted with a smoothed spline function in MATLAB; spline = csaps(age, δ13C, ρ), where ρ = 0.99 (close to data, but the curve in Fig. 1 does not go through each data point).
The C/P ratio of extant bryophytes (Table S3) was compiled from data in the literature (34, 80–88). Where only values of mg P/g biomass were available, a value of mg C/g biomass = 430 was assumed based on the mean value across six bryophyte species from ref. 89. Results for molar C/P ratios are given to two significant figures, given the uncertainty in the input data, except where authors themselves provide more precise values.
Ecophysiological Model of Cryptogamic Vegetation.
We used a trait-based spatial model of cryptogamic vegetation (i.e., bryophyte and lichen) cover to estimate the potential global NPP of the early nonvascular plant biosphere (29, 30). The Late Ordovician (445 Ma, Hirnantian stage) setup of the model is fully described elsewhere (32). The model is driven by existing Late Ordovician climate simulations (31), conducted at a range of different atmospheric CO2 and O2 concentrations. Initially, we assume atmospheric O2 = 0.6 PAL (∼14 vol.%) at 445 Ma, which is consistent with COPSE model simulations (Fig. 3D) that go on to produce O2 levels consistent with the fossil charcoal record. We also initially assume atmospheric CO2 = 8 PAL, which is a widely quoted value consistent with the occurrence of Hirnantian glaciations at 445 Ma (20), and consistent with COPSE model simulations that assume an effect of early plants on silicate weathering following ref. 20. We explored the sensitivity of predicted global NPP to variations in atmospheric CO2 and corresponding climate state (Fig. S1), to constraining vegetation cover with extensive Late Ordovician ice sheet cover (Fig. S2), and to varying O2 in combination with CO2 (Table S2). The relatively high global NPP results obtained are consistent with present-day cryptogamic covers providing ∼7% of global NPP, despite making up only 1% of terrestrial vegetation by mass (90) and being restricted to relatively resource-poor habitats, while also operating in an atmosphere with a low CO2/O2 ratio.
Experimental P Weathering Calculation.
In our previously reported (20) weathering experiments with granite, the mean amounts of phosphate weathered into aqueous solution were as follows: control microcosms = 0.0137 μmol P, biotic microcosms = 0.0726 μmol P. The mean moss biomass in the biotic microcosms was 14.390 mg, which assuming 0.43 gC/g biomass and C/P = 2,000 (Table S3) suggests 0.26 μmol P in biomass, or for C/P = 1,000–4,000, 0.13–0.52 μmol P in biomass; this gives a biotic P weathering amplification factor ∼24 (range 15–43), whereas previously we suggested up to 60 (20). Clearly these estimates are dominated by the unmeasured P content of biomass. However, the P weathering amplification factor has to be >5.3 (the ratio of dissolved phosphate entering solution in microcosms with moss to those without), which is already considerably greater than the amplification factors for Ca = 1.4 and Mg = 1.5 from granite, indicating selective weathering of P.
COPSE Model.
We used the COPSE model (10, 20) to study the effects of the early rise of land plants on the coupled biogeochemical cycles of C, O, N, P, and S, including the δ13C record. The model is described in full in ref. 10, and the version used here incorporates the changes in model structure described in ref. 20. The model has several forcing parameters, including solar luminosity; the geological factors degassing (D) and uplift (U); and the biological forcing factors evolution/colonization (E), enhancement of weathering (W), selective phosphorus weathering (F), and changes to the C/P burial ratio of terrestrially derived material (CP). The geologic and biologic forcing factors are all normalized to 1 at the present day, except C/P = 1,000 at present day. Our overall modeling strategy was to try and reproduce key changes in the δ13C record with plausible biological and geological forcing scenarios, constrained where possible by available data. We focused initially on altering the biological forcing scenario while using the original geological forcing scenario. Then, in a sensitivity analysis, we considered uncertainty in geologic forcing (91), and alternative initial conditions (altering the feedback structure of the model). The forcing scenarios and sensitivity analyses are detailed in the SI Materials and Methods.
Acknowledgments
We thank two anonymous referees for insightful comments that improved the manuscript. Support for this work was provided by Leverhulme Trust Grant RPG-2013-106 (to T.M.L., S.J.D., and B.J.W.M.); NERC Grant NE/I005978/2 (to T.M.L.); a Royal Society Wolfson Research Merit Award (to T.M.L.); a University of Leeds Academic Fellowship (to B.J.W.M.); and VILLUM Foundation Grant VKR023127 (to T.W.D.).
Footnotes
The authors declare no conflict of interest.
This article is a PNAS Direct Submission.
This article contains supporting information online at www.pnas.org/lookup/suppl/doi:10.1073/pnas.1604787113/-/DCSupplemental.
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