Abstract
Characterised by long term cooling and abrupt ice sheet expansion on Antarctica ~14 Ma ago, the mid Miocene marked the beginning of the modern ice-house world, yet there is still little consensus on its causes, in part because carbon cycle dynamics are not well constrained. In particular, changes in carbonate ion concentration ([CO32−]) in the ocean, the largest carbon reservoir of the ocean-land-atmosphere system, are poorly resolved. We use benthic foraminiferal B/Ca ratios to reconstruct relative changes in [CO32−] from the South Atlantic, East Pacific and Southern Oceans. Our results suggest an increase of perhaps ~40 μmol/kg may have occurred between ~15 and 14 Ma in intermediate to deep waters in each basin. This long-term increase suggests elevated alkalinity input, perhaps from the Himalaya, rather than other shorter-term mechanisms such as ocean circulation or ecological changes and may account for some of the proposed atmospheric CO2 decline before ~14 Ma.
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Introduction
The mid Miocene, including the mid Miocene climate transition (MMCT) at ~13.8 Ma1, represents one of the three most significant cooling episodes of the Cenozoic2,3, along with the Eocene-Oligocene transition4 (~34 Ma) and onset of Northern Hemisphere Glaciation (~2.7 Ma). Yet in contrast to these events, comparatively little is known about the causes and feedbacks of this mid Miocene cooling. Set within a long term cooling trend from 15 to 10 Ma, the rapid expansion of the East Antarctic ice sheet at 13.8 Ma3,5 is associated with a sea level fall in the order of ~60 m6,7 and a coeval drop in deep ocean temperature of ~2°C2,8. This glacial expansion was accompanied by the extinction of Antarctic tundra9, a ~6–7°C fall in sea surface temperature in the high latitude southwest Pacific10, the development of perennial sea ice in the Arctic11,12, the development of significant temperate terrestrial biotic provinces including the early expansion of C4 grasses13 and significant tectonic events that would have impacted on the global carbon cycle (see Supplementary Information). Hypotheses for the causes of this transition include CO2 drawdown, perhaps from a cessation of mid Miocene volcanism14 or enhanced terrestrial weathering and erosion15, priming the climate system for ice sheet growth during low amplitude orbital eccentricity at 13.8 Ma1. Alternatively the onset of a deep Antarctic Circumpolar Current may have thermally isolated Antarctica due to tectonic subsidence in the Scotia Sea16.
There have been numerous efforts to reconstruct atmospheric CO2 through the Miocene14,17,18,19 and in contrast to previous suggestions that temperature may have become decoupled from CO2 during the mid Miocene17,18, a recent study suggests a decline of ~100 ppm may have occurred between ~15 and 14 Ma before the MMCT14. As surface ocean CO2 is in approximate steady state with the atmosphere and the relatively small surface ocean reservoir is continuously replenished by the much larger deep ocean reservoir (>1 km), the speciation of dissolved inorganic carbon (DIC) of the deep ocean is linked to atmospheric CO2 (refs 20,21) and therefore a ~100 ppm decrease in CO2 should be documented within deep sea sediments. In the ocean, DIC occurs as several species that maintain acid/base equilibrium:
As the ratio of ocean water alkalinity (ALK; the sum of bases in solution, in sea water predominantly: [HCO3−] + 2[CO32−] + [B(OH)4−]) to DIC increases (for example from increased continental weathering or increased biological productivity), the proportion of the DIC pool present as sea water [CO32−] increases, thus shifting the balance away from [CO2(aq)] and potentially drawing down atmospheric CO2 to recover equilibrium20,21. Previous attempts to constrain past ocean carbonate chemistry have focused on reconstructions of the calcite compensation depth (CCD) linked to [CO32−], which are of low resolution and subject to significant complications22, or reconstructions of [CO32−] directly with benthic foraminiferal shell Li/Ca and Mg/Ca7, also subject to complications such as a temperature effect7 (Supplementary Information).
Recent studies23,24 on core top samples from several ocean basins have shown a strong quantitative relationship between benthic foraminiferal B/Ca ratios and deep water [CO32−], which has been further supported by subsequent down-core studies25,26,27. Here, we reconstruct deep and intermediate water [CO32−] from six Ocean Drilling Program (ODP) core sites in three ocean basins (Fig. 1) using B/Ca of the epifaunal benthic foraminifera Cibicidoides mundulus (Fig. 2, see Methods). The species C. mundulus is unique in being long-ranging, allowing the use of this proxy as far back as the mid Miocene.
Results
Cibicidoides mundulus B/Ca
In the ~1 Ma lead up to the MMCT (~15.5–14 Ma), benthic foraminiferal B/Ca ratios from all six sites increase (Fig. 2, Supplementary Table S1), indicating a probable increase in deep water [CO32−]. All samples have low Al/Ca values well below 100 μmol/mol (Supplementary Table S1), indicating little potential clay contamination7,24. In the South Atlantic (Fig. 2b) the deepest Site 1226 (~3.6 km palaeo-water depth) shows a larger increase in B/Ca over this interval than shallower Site 1264 (2.3 km), indicating a possible greater increase in [CO32−] in deep waters relative to intermediate waters. In the East Pacific (Fig. 2d) and Southern Ocean (Fig. 2e), the magnitude of the B/Ca increase at both the shallow and deep sites appears to be comparable, with a slightly larger overall increase in the East Pacific perhaps due to a modified ocean circulation pattern. In the ~1 Ma after the MMCT (~14–13 Ma) deeper sites in the East Pacific (Site 1237, 2.8 km) and Southern Ocean (Site 1168, 2.3 km) exhibit further increased benthic B/Ca, whilst at nearby shallower Sites 1236 (0.9 km) and 1171 (2 km) benthic B/Ca is seen to drop slightly. This B/Ca decrease at the shallower sites may be explained by either a decrease in global intermediate water [CO32−] perhaps due to changes in ocean circulation, or more likely, localised depletions in [CO32−] due to expansion of the oxygen minimum zones associated with enhanced primary productivity (both sites are situated in proximity to the modern depth of [CO32−] and oxygen minima; Supplementary Fig. S1).
Miocene oceanic [CO32−]
B/Ca ratios from all sites were converted to [CO32−] using the 0.69 μmol/mol per μmol/kg sensitivity obtained from a global core-top calibration23, past water depth estimates and mid Miocene estimates of seawater boron and calcium ratios (B/Casw) and concentrations (Supplementary Information). There is yet to be a consensus on mid Miocene boron and calcium concentrations28,29 and future estimates may therefore change, although the relative changes in [CO32−] inferred from our records (Fig. 3) may not be greatly affected. It is likely that the B/Casw ratio changed over the interval 15.5–13 Ma, even considering the long residence times of boron (20 Ma)30 and calcium (1.1 Ma)31 in the oceans. It is difficult to estimate these potential changes, but the dominant source of oceanic boron is considered to be continental discharge from weathering of silicates, carbonates and evaporites32 and changing Himalayan erosion has been identified as an important variable on Cenozoic boron flux28. To test the sensitivity of our [CO32−] estimates to a changing flux of boron to the oceans, we consider the effect of a 10% increase in B/Casw given that sedimentation rates from Asian basins are estimated to have increased by ~10% due to Himalayan erosion between 15.5 and 13 Ma33 (Supplementary Fig. S2). A 10% increase in oceanic boron whilst calcium remained stable (conservatively assuming the majority of weathering products were silicates34), would have increased B/Casw by ~3 μmol/mol, impacting [CO32−] estimates by only ~4 μmol/kg (included in the error on Fig. 3). Calcium concentrations of the oceans between 15.5–13 Ma are actually estimated to have increased in the order of 50%29, largely from exposure of shelf carbonates as sea level fell particularly after ~13.8 Ma29. Since the B/Ca of the exposed carbonates is unknown, the impact on B/Casw is unknown. However if calcium concentrations drove B/Ca changes, then we would expect to see similar changes in Mg/Ca and Li/Ca (Supplementary Table S1), which we do not. With the exception of the two data points from the shallowest sites (Sites 1236 and 1171) showing a decrease at ~13.5 Ma, we estimate deep water [CO32−] to have increased by an average of perhaps ~40 μmol/kg between ~15.5 and 13 Ma, with the largest increase occurring between ~15 and 14 Ma (Fig. 3d).
Over the interval ~15.5–13 Ma, deep water CaCO3 preservation may have increased in the South Atlantic, East Pacific and Southern Ocean (Fig. 2b, d and e), possibly reflecting the increasing [CO32−] (from B/Ca) and inferred deepening of the CCD. Carbonate preservation proxies in the North Atlantic (Fig. 2c, wt% CaCO3), Indian Ocean (Fig. 2f, % CaCO3 coarse fraction), West Pacific (Supplementary Fig. S3, CaCO3 fragmentation) and Southwest Pacific (Supplementary Fig. S3, wt% CaCO3) show a long term increase, suggesting possible increases in [CO32−] in these locations also. There are significant uncertainties with using these records to infer preservation, as we do not yet have detailed sedimentation rate or CaCO3 rain rate data22, but taken together the CaCO3 trends are fairly consistent. The consistency of our [CO32−] reconstruction and CaCO3 preservation records (Figs 2,3d) appears to point to a global increase in [CO32−] of deep (>1 km) waters particularly from ~15–14 Ma, as our records cover a large depth range (~0.9–3.8 km) and geographic distribution of the major ocean basins (Fig. 1) and include both glacial and interglacial measurements (Fig. 3d). A study from ODP Site 761 at 2.2 km water depth in the Indian Ocean also concluded that there was an increase in local [CO32−] between ~15 and 14 Ma7.
We recognise that there is substantial variability within our dataset, partly because the measurements come from various sites and from various times corresponding to both glacial and interglacial intervals and oceanic [CO32−] may be expected to have decreased during interglacials26. However the long term increase in [CO32−] from ~15 to 14 Ma presented here is superimposed onto these shorter time-scale variations. Significant basin partitioning of CaCO3 may not be expected since similar values of benthic δ13C in both the Pacific and Atlantic Oceans between 15 and 12 Ma (Supplementary Fig. S4) suggests a relatively homogenous deep water mass may have been present in the Southern Ocean3 and possibly the South Atlantic. Modelling experiments suggest that ocean circulation was dominated by Southern Ocean deep water mass formation35 and sedimentological proxies document increasing influence of a deep Pacific southern water mass after ~15 Ma36. Miocene Tethys Indian Saline Water, a significant component of deep and intermediate water bathing the Indian and Pacific Oceans (Fig. 1) and possibly warming Antarctica, appears to have diminished by ~15 Ma37 likely due to the shoaling of the Tethys Ocean basin37. Northern Component Water is not thought to have played a prominent role in ocean circulation until after ~12 Ma35,38, possibly due to the shoaling of the Greenland-Scotland Ridge. Neodymium isotopes from Walvis Ridge (used as an ocean circulation tracer) show no increased stratification and therefore North Atlantic deep water formation before ~10.7 Ma39.
Discussion
A long-term, whole ocean increase in [CO32−] at >1 km water depth and apparently enhanced CaCO3 preservation (Fig. 2), particularly apparent between ~15 and 14 Ma (Fig. 3d), implies an increase in the whole ocean ratio of alkalinity to dissolved inorganic carbon (ALK:DIC), as a charge imbalance driven by ALK is balanced by the speciation of DIC away from [CO2] towards [CO32−] (ref. 21). ALK is largely supplied to the ocean by continental weathering of emergent carbonates and silicates on land and removed from the ocean by burial of CaCO3 on the sea floor20. DIC is added and removed by these processes, but also removed by burial of organic carbon (Corg) in ocean sediments and by air-sea exchange. There are several ways of causing increases in deep ocean [CO32−], including a lowering of the CaCO3/Corg rain ratio of primary export production20, increased shelf to basin fractionation from sea level fall and exposure and erosion of carbonate shelves4,20,26,27,40, changes in ocean circulation20,26, increased high latitude nutrient utilization increasing the [CO32−] of preformed surface water20,41 and increased continental weathering15,20,33,42. Processes such as ocean circulation and nutrient utilization can produce large short-term excursions in seawater [CO32−], but are less likely to account for the long-term change observed from ~15.5 to 13 Ma. This is because carbonate compensation, the process by which an elevation in deep water [CO32−] increases the area of CaCO3 burial on the sea floor and the subsequent removal of ocean water [CO32−], would bring the ocean to the initial steady-state on a timescale of several thousand years43.
Increased shelf to basin fractionation was proposed as the major cause of the widespread CCD fall during ice sheet expansion at the Eocene-Oligocene transition, as sea level fall drove carbonate deposition deeper into basins and raised oceanic δ13C4,40. However there is no evidence for a long-term sea level fall6 or long term δ13C increase (Fig. 3c) prior to 14 Ma, when we infer a notable [CO32−] increase (Fig. 3d). If a large, long-term decrease in the CaCO3/Corg ratio were to account for some of the [CO32−] variability from ~15.5–13 Ma, as has been suggested to account for the short-term δ13C maxima at ~13.7 Ma44, we would expect to see increasingly organic-rich sediments in marine sediment cores. In fact, the interval ~16–14 Ma is associated with episodic increases in organic rich sediments around the Pacific margin45 that are associated with global δ13C and δ18O maxima (Fig. 3) and higher productivity along the west coast of Africa46 before ~14 Ma, indicating that changes in the CaCO3/Corg ratio may account for part the observed changes in [CO32−] particularly before 14 Ma. However, no long-term secular increase in δ13C, consistent with a sizeable increase in productivity, is apparent in any records (Fig. 3c, Supplementary Fig. S4).
We believe that the most plausible explanation for the long-term increase in [CO32−] suggested by our records, particularly before 14 Ma, was increased continental weathering and erosion15. Uplift and erosion of the Himalaya, which has been linked to Cenozoic climate change via the erosion and weathering of silicates which consumes CO2 (refs 33,34), would also have added ALK to the ocean. The Greater Himalaya experienced enhanced exhumation rates during the mid Miocene33 (Supplementary Fig. S2c) and plate configuration reconstructions indicate the Himalaya met with the Intertropical Convergence Zone of high precipitation in the mid Miocene42. Several mineralogical proxies associated with monsoonal intensity also point to an increase in Himalayan regional chemical weathering in the mid Miocene33 (Fig. 3e). Mounting evidence in support for enhanced weathering rates and ultimately delivery of ALK to the oceans, is consistent with a peak in bulk sediment accumulation rates in the major clastic basins around Southeast Asia33 (supplied by the Himalaya) and high fluxes of Sr from the Ganges-Brahmaputra Rivers47 during the mid Miocene (Supplementary Fig. S2e). Although dating is not yet able to precisely constrain the timings of all these events, if enhanced silicate weathering and erosional deposition from the Himalaya was responsible for global cooling during the mid Miocene, as has been previously suggested15,33,42, then an increase in ocean ALK and hence [CO32−] would be expected to be coeval. Other possible terrestrial sources of ALK were the Tethys Ocean, which underwent uplift and intermittent closure in the mid Miocene48 and the East Africa Plateau which also experienced peak uplift in the mid Miocene49 (Supplementary Fig. S2c), although the timing and magnitude of these events are even less well constrained. Whichever the source, enhanced continental weathering, consuming atmospheric CO2 and transporting ALK to the ocean, is consistent with our interpretation of elevated seawater [CO32−] during the mid Miocene.
In summary, our new reconstruction of deep ocean [CO32−] (>1 km water depth) provides a tantalising insight into potential changes in the carbonate system during the mid Miocene. Comparison of these records with published δ18O, δ13C and CO2 proxy records (Fig. 3, Supplementary Fig. S5) indicates enhanced input of ALK to the oceans as a possible contributor to mid Miocene climate change before the MMCT at 13.8 Ma. A likely source could have been the Himalaya which experienced increased uplift, weathering and erosion centred at ~15–14 Ma (Supplementary Fig. S2). Whilst our records demonstrate that carbonate chemistry in the world's oceans changed during the mid Miocene, they also highlight the need to better resolve deep and intermediate water [CO32−] to fully understand the roles of weathering, ocean circulation and the carbon cycle during this complex episode of climatic change. However, taking our data at face value, we performed simple sensitivity calculations of the effect a hypothetical addition of ALK to achieve the estimated [CO32−] increase of 40 μmol/kg (Fig. 3d) may have had on ocean water CO2, using modelled estimates of initial Miocene ocean water ALK, DIC and temperature (Supplementary Information). Although necessarily subject to significant uncertainties such that absolute values must be considered speculative, if the deep ocean [CO32−] increase was mixed to surface water, it may have drawn down atmospheric CO2 in the region of ~16–25% (Supplementary Table S2). This is broadly in the range of atmospheric CO2 reconstructions from fossil leaf stomatal frequency19 and planktonic foraminiferal δ11B (Fig. 3a)14. Further, in agreement with δ11B reconstructions, the timing of our increase in deep ocean [CO32−] and putative drawdown in atmospheric CO2 is consistent with the largest drawdown in CO2 taking place between ~15 and 14 Ma before the abrupt MMCT at 13.8 Ma14 and comparison of these two records does indicate a possible coupling between atmospheric CO2 and deep ocean [CO32−] (Supplementary Fig. S5). Atmospheric CO2 may have also been affected by other mechanisms such as volcanism14,47 and our reconstructions contain too much uncertainty to indicate how much CO2 was removed by the oceans. However, the general increase in deep ocean [CO32−] over the mid Miocene presented here does indicate a drawdown of atmospheric CO2 into the ocean may have occurred and highlights the importance of constraining deep ocean changes when assessing mid Miocene carbon cycle dynamics.
Methods
Analytical procedures
Deep sea sediment samples of ~40 cc volume were washed through a 63 μm sieve with deionised water and oven dried at <30°C. A total of 10–25 specimens of the benthic foraminifera Cibicidoides mundulus were picked from the 250–350 μm fraction in each sample and cleaned using the standard ‘oxidative’ treatment protocol50,51. Elemental/Ca ratios were analyzed by inductively coupled plasma mass spectrometer (ICP-MS) according to methods described elsewhere23,51. For the ICP-MS, the B blank is <2% of the consistency standard (B/Ca = 150 μmol/mol). Recent detailed work on the foraminiferal genus Cibicidoides indicates that different morphospecies produce a certain degree of variation in B/Ca (ref. 24). To minimise possible error, we strictly selected only ‘typical’ C. mundulus using a conservative species concept (see Supplementary Information), from the 250–350 μm size fraction and a relatively high number of specimens (>20 individuals where available). Replicate analysis carried out on two samples showed variability of <4 μmol/mol, in line with published replicate analyses of standards and samples giving precisions of <2% (RSD) for B/Ca23.
Miocene [CO32−] estimates
Values for Δ[CO32−] were calculated by modifying the equation: B/Ca = aΔ[CO32−] + b (ref. 23), where a = 0.69 and b = 119.1. To estimate mid Miocene B/Casw values (modern B = 415 μmol/kg; modern Ca = 0.01 mol/kg), we assumed B to be ~1.07 times the modern value28 and Ca to be ~1.12 times the modern value29. The resulting value for Miocene B/Casw is ~96% of modern, which was used to modify the equation: B/Ca(Miocene)= 0.96 * aΔ[CO32−] + 0.96 * b. The calculated Δ[CO32−] was converted to [CO32−] by adding the [CO32−]sat of the pressure equivalent to estimated water depths at ~14 Ma. See Supplementary Information for further details.
Assessment of uncertainty
The error bars associated with B/Ca values (Fig. 2) include an analytical precision of ±1.5 μmol/mol and a replicate error of ±2 μmol/mol. The error bars associated with [CO32−]sw (Fig. 3d) include the analytical precision of ±2.2 μmol/kg, the replicate error of ±2.9 μmol/kg, a calibration uncertainty of ±10 μmol/kg (2 σ)23, a sea level uncertainty of ±0.5 μmol/kg (from ~50 m change) and a mid Miocene ΔB/Casw uncertainty (from increased terrestrial erosion) of ±2 μmol/kg.
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Acknowledgements
We thank M. Leng for stable isotope analysis and K. Johnson for sample processing. This study is part of the Palaeoclimate and Palaeoenvironment core science programme at the British Geological Survey, funded by the Natural Environment Research Council (S.K., V.P.) and by grant ARC DP140101393 (J.Y.). S.K. publishes with permission of the Executive Director of the British Geological Survey (NERC).
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S.K., V.L.P. and J.Y. conceived and designed the project, J.Y., S.K. and V.L.P. generated data and S.K., J.Y. and V.L.P. wrote the paper.
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Kender, S., Yu, J. & Peck, V. Deep ocean carbonate ion increase during mid Miocene CO2 decline. Sci Rep 4, 4187 (2014). https://doi.org/10.1038/srep04187
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DOI: https://doi.org/10.1038/srep04187
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