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Proceedings of the National Academy of Sciences of the United States of America logoLink to Proceedings of the National Academy of Sciences of the United States of America
. 2017 Aug 21;114(36):9647–9652. doi: 10.1073/pnas.1618765114

Emerging role of wetland methane emissions in driving 21st century climate change

Zhen Zhang a,b,c,1, Niklaus E Zimmermann a,d, Andrea Stenke d, Xin Li c,e, Elke L Hodson f, Gaofeng Zhu g, Chunlin Huang c, Benjamin Poulter c,h
PMCID: PMC5594636  PMID: 28827347

Significance

Conventional greenhouse gas mitigation policies ignore the role of global wetlands in emitting methane (CH4) from feedbacks associated with changing climate. Here we investigate wetland feedbacks and whether, and to what degree, wetlands will exceed anthropogenic 21st century CH4 emissions using an ensemble of climate projections and a biogeochemical methane model with dynamic wetland area and permafrost. Our results reveal an emerging contribution of global wetland CH4 emissions due to processes mainly related to the sensitivity of methane emissions to temperature and changing global wetland area. We highlight that climate-change and wetland CH4 feedbacks to radiative forcing are an important component of climate change and should be represented in policies aiming to mitigate global warming below 2°C.

Keywords: global warming potential, climate feedbacks, inundation, radiative forcing, climate mitigation

Abstract

Wetland methane (CH4) emissions are the largest natural source in the global CH4 budget, contributing to roughly one third of total natural and anthropogenic emissions. As the second most important anthropogenic greenhouse gas in the atmosphere after CO2, CH4 is strongly associated with climate feedbacks. However, due to the paucity of data, wetland CH4 feedbacks were not fully assessed in the Intergovernmental Panel on Climate Change Fifth Assessment Report. The degree to which future expansion of wetlands and CH4 emissions will evolve and consequently drive climate feedbacks is thus a question of major concern. Here we present an ensemble estimate of wetland CH4 emissions driven by 38 general circulation models for the 21st century. We find that climate change-induced increases in boreal wetland extent and temperature-driven increases in tropical CH4 emissions will dominate anthropogenic CH4 emissions by 38 to 56% toward the end of the 21st century under the Representative Concentration Pathway (RCP2.6). Depending on scenarios, wetland CH4 feedbacks translate to an increase in additional global mean radiative forcing of 0.04 W·m−2 to 0.19 W·m−2 by the end of the 21st century. Under the “worst-case” RCP8.5 scenario, with no climate mitigation, boreal CH4 emissions are enhanced by 18.05 Tg to 41.69 Tg, due to thawing of inundated areas during the cold season (December to May) and rising temperature, while tropical CH4 emissions accelerate with a total increment of 48.36 Tg to 87.37 Tg by 2099. Our results suggest that climate mitigation policies must consider mitigation of wetland CH4 feedbacks to maintain average global warming below 2 °C.


Terrestrial wetlands are among the largest biogenic sources of methane contributing to growing atmospheric CH4 concentrations (1) and are, in turn, highly sensitive to climate change (2). However, radiative feedbacks from wetland CH4 emissions were not considered in the Coupled Model Intercomparison Project Phase 5 (CMIP5), and Integrated Assessment Models (IAM) assumed anthropogenic sources to be the only driver responsible for the increase of atmospheric CH4 burden since the 1750s (3). The role of wetland CH4 emissions, however, may play an increasingly larger role in future atmospheric growth of methane because of the large stocks of mineral and organic carbon stored under anaerobic conditions in both boreal and tropical regions. Paleoclimatological and contemporary observations of the climate sensitivity of wetland methane emissions suggest the potential for a large feedback (4), but there remains large uncertainty in quantifying the actual range of the response (5, 6).

Increasing air temperature is linked to the thawing of permafrost and to increased rates of soil microbial activity (7), which directly lead to greater CH4 production in soils due to thaw-induced change in surface wetland areas (8). In the tropics, wetland areal extent is also influenced by precipitation, which affects the area of surface inundation, water table depth, and soil moisture that, in turn, promote methanogenesis. Elevated CO2 concentrations can increase ecosystem water use efficiency and thus soil moisture, and also increase soil carbon substrate availability for microbial activities (9). Tropical wetlands, for which a decline in inundation was observed in recent decades (10), are already exposed to increasing frequencies in extreme climate events, e.g., heat waves, floods, and droughts, and changes in rainfall distribution (11) and variability in methane emissions (12). Meanwhile, northern high-latitude ecosystems are experiencing a more rapid temperature increase than elsewhere globally and with increased rates of soil respiration (13), yet, locally at least, no response in methane emissions (14). Despite the importance of these feedbacks noted by the Intergovernmental Panel on Climate Change Fifth Assessment Report (IPCC AR5) (15), a comprehensive assessment of long-term global CH4 feedbacks from changing wetland CH4 emissions is still lacking.

To address uncertainties related to climate−wetland CH4 feedbacks, we simulated an ensemble of wetland CH4 emissions for the 21st century, and then quantified the wetland CH4 contribution to radiative forcing (RF). Global mean air temperature change was estimated using the reduced complexity carbon cycle and climate model Model for the Assessment of Greenhouse-Gas Induced Climate Change Version 6 (MAGICC6) (16) and a sustained pulse−response model (17). A state-of-the-art land surface model, Lund–Potsdam–Jena Dynamic Global Vegetation Model (LPJ-DGVM) Wald Schnee und Landscaft version (LPJ-wsl), was used to quantify terrestrial wetland CH4 emissions, in which permafrost and wetland area distribution and dynamics were estimated prognostically (18). Simulated global CH4 emissions, calibrated such as to minimize the discrepancy between contemporary global annual CH4 emissions, were estimated as a function of substrate, soil temperature, and soil moisture (19). Statistically representative estimates of mean and variance of future CH4 emissions outputs were generated from 112 climate projections originating from 38 climate models of the CMIP5 ensemble (SI Appendix, Table S1) covering four Representative Concentration Pathway (RCP) storylines (20).

Materials and Methods

Wetland Definition.

Wetlands are defined here as the land area that is either permanently or seasonally saturated, excluding small ponds, lakes, and coastal wetlands. Permanent wetlands comprise three general types: mineral wetlands (swamps and marshes), peatlands (permafrost, bog, fens), and seasonally flooded shallow water (floodplains). The methane-producing area is thus linked to inundation and freeze−thaw dynamics, which change geographically and temporally in response to soil water dynamics.

Model Description.

The LPJ-wsl model is a process-based dynamic global vegetation model developed for carbon cycle applications based on development of the LPJ-DGVM (21). LPJ-wsl includes land surface processes, such as water and carbon fluxes, as well as vegetation demography and dynamics that are represented by plant functional types (PFTs) (22). The distribution of PFTs is simulated based on a set of bioclimatic limits and by plant-specific parameters that govern their physiological behavior and their competition for resources. Soil hydrology is modeled using a two-layer bucket model for hydrology and is coupled to an eight-layer freeze−thaw scheme and one-layer snow model to determine permafrost extent and ice content (23, 24) (SI Appendix, Methods).

Wetland area and dynamics were simulated following a modified version of the topography-based hydrological model (TOPMODEL) using a prescribed high-resolution topographic index based on a mapping product, hydrological data and maps based on shuttle elevation derivatives at multiple scales (HydroSHEDS) (25). HydroSHEDS was shown to agree most closely with observed wetland area in a comparison with existing global elevation datasets and parameterization schemes (18). Our TOPMODEL approach was optimized by calibrating parameters to match observations from a hybrid wetland area dataset (26) and a regional remote sensing surface inundation dataset (27).

We modeled net wetland CH4 emissions to the atmosphere restricted to land areas where anaerobic soil conditions create low redox potentials required for methanogenesis. Net CH4 emissions are estimated daily by combining wetland area (A) within a grid cell (x) with two soil temperature- and moisture-dependent scaling factors (rCH4:C and fecosys) applied to heterotrophic respiration (Rh),

E(x,t)=rCH4:Cfecosys(x)A(x,t)Rh(x,t), [1]

where E(x,t) is the net wetland CH4 flux, rCH4:C is a fixed ratio of soil C to CH4 emissions, and fecosys is a modifier that varies the CH4 emission intensity for different biomes, which is optimized to match average annual emissions from an atmospheric inversion model (28). This approach thus estimates net methane emissions directly, and indirectly accounts for the individual processes of production and consumption of methane, and the various transport processes from the soil to the atmosphere. The comparisons of global and regional net CH4 emissions between LPJ-wsl and other biogeochemical models are listed in SI Appendix, Table S2.

RF Calculations.

Two methodologies for calculating RF were used to quantify the climate feedback from additional changes in CH4 emissions from wetlands. The first method uses the carbon cycle climate model MAGICC6 (16), and the second method uses an emission-driven sustained pulse−response model (17), both relative to a reference year 1765. Because of the challenge to isolate the effect of anthropogenic forcing from wetland forcing in MAGICC6, the simple sustained pulse−response model was used to assess the impact of wetlands on RF by using prescribed anthropogenic sources since 1765 and adding the estimated total wetland emissions from LPJ-wsl. Before 1961, wetland CH4 emissions were generated, following a uniform distribution, by randomly selecting emissions from 1961 to 1990 to bring the RF value into equilibrium.

In MAGICC6, the lifetime of tropospheric methane is calculated by integrating the effects of hydroxyl radicals (OH) with the temperature-based chemical reaction rates. The observed CH4 concentration changes over time are more accurately quantified by the net result of variations in emissions of multiple chemical compounds that affect the OH chemical sink, such as ozone, nitrogen oxides, carbon monoxide, and volatile organic compounds. In addition, the net atmospheric lifetime of CH4 is determined by lifetimes of tropospheric OH, upland soil uptake, and the stratospheric losses. We prescribed the wetland CH4 concentrations and corresponding anthropogenic CH4 emissions for each RCP from IPCC AR5 (20).

In contrast, the sustained pulse−response model applies the perturbation lifetime of methane, which is designed to describe the overall long-term RF from CH4 reactions with OH in the atmosphere (e.g., water vapor in stratosphere), as a constant value of 12.4 y (15). The instantaneous RF from CH4 contributions at year t since the reference year t′, here the year 1765, is given by

RFCH4(t)=ξCH4ACH40tΦ(t)e(tt)/τdt, [2]

where ξCH4 is a multiplier for CH4 set to be 1.3; ACH4 is the greenhouse-gas radiative efficiency (1.3 × 10−13 W⋅m−2⋅kg−1); and τi is the fixed perturbation lifetime for CH4 (12.4 y). Φ(t) is a first-order decay function representing the lifetime of an individual net input of CH4 into the background atmosphere according to IPCC 2013 (15),

Φ(t)=r0etτ, [3]

where r0 is the initial perturbation, and τ is the perturbation lifetime of CH4. To estimate RF of equal mass of CO2 in the atmosphere, five CO2 decay pools with different fractions fi(26%, 24%, 19%, 14%, and 18%) and adjustment times τi (3.4 y, 21 y, 71 y, 421 y, and 108 y) are applied to describe the more complicated behavior of CO2 (17). Thus the total CO2 RF is given by

RFCO2(t)=i=04εiAifi0tΦi(t)e(tt)/τidt. [4]

To quantify the global warming effect of wetland and anthropogenic CH4 sources, we used a modified metric Sustained Global Warming Potential (SGWP) [unit: kilograms CO2-equivalents per year (kg CO2-eq·y−1)] (29) to evaluate the total cumulative RF effect from a persistent individual CH4 source, which was defined as the sum of the time-integrated total RF (unit: watts per square meter), from Eqs. 2 and 4, over a given time horizon due to a sustained pulse emission of annual CH4 emission (unit: teragrams) relative to a sustained pulse emission of an equal mass of CO2 under present-day background conditions. This equation is given by

SGWPCH4(H)=0HRFCH4(t)dt0HRFCO2(t)dt, [5]

where H represents a certain time horizon. The SGWP for wetland and anthropogenic emissions was calculated with an initial year of 1765.

To quantify the total global warming contribution of wetland CH4 emissions compared with anthropogenic counterpart, a Wetland Dominance Index (WDI) (unit: percent) was defined using following equation:

WDI=(SGWPwetlandSGWPanth1)×100, [6]

where SGWPanth represents SGWP caused by anthropogenic activities.

Input Data and Model Experiments.

As input to LPJ-wsl, the simulated meteorology, air temperature, total precipitation, and cloud cover from each of the CMIP5 models available from the Earth System Grid Federation was spatially downscaled and bias-corrected to match the spatial resolution (0.5°) and historical period of overlap (1960–1990) from Climatic Research Unit Time Series (CRU TS) Version 3.2.2. We conducted two sets of simulations for each of the climate projections, (i) a single spin-up simulation for 1,000 y with randomly selected, detrended 1961–1990 climate, and a constant atmospheric CO2 concentration of 303 ppm by volume (the average for 1961–1990) and (ii) a combined historical and future simulation with time-varying CO2 and climate data as defined by the corresponding RCP (20).

Uncertainty Analysis.

A statistical emulation of LPJ-wsl was parameterized to quantify model structural uncertainty and evaluate how it affected the simulated CH4 fluxes. We adapted the multiple regression approach from ref. 30 and applied this within a Monte Carlo (MC) analysis to estimate the distribution of CH4 emissions for each simulation. Parameters in the statistical model were fitted for each RCP. We assumed the parameters of the statistical model followed a normal distribution and used a 2D Latin Hypercube Sampling algorithm to generate 10,000 sets of parameters for each climate projection (SI Appendix, Fig. S7). We then conducted MC simulations with Eq. 1, for a total of 40,000 calculations, to derive the range of CH4 emissions for each RCP (SI Appendix, Fig. S8). These ranges were only applied in MAGICC6 and the simple sustained pulse−response model, to include the impact of model structural uncertainty on RF and SGWP calculations.

Results and Discussion

Mean global annual CH4 emissions from natural wetlands were projected to increase from 172 Tg CH4⋅y−1 (1σ SD, ±12 Tg CH4⋅y−1) at present to 221.6 ± 15, 255 ± 20, 272 ± 21, and 338 ± 28 Tg CH4⋅y−1 in RCP2.6, RCP4.5, RCP6.0, and RCP8.5, respectively, by 2100 (Fig. 1A). In the strong climate mitigation scenario (RCP2.6), which includes the possibility of reaching the policy-relevant 2 °C target, wetland CH4 emissions peak around the 2050s, with an average of ∼225 Tg CH4⋅y−1, and decline thereafter. In contrast, RCP4.5 reveals wetland CH4 emissions to increase to ∼246 ± 21 Tg CH4⋅y−1 before the 2070s and then keep constant, with slightly lower emissions than the RCP6.0 scenario. In the “business-as-usual” scenario, RCP8.5, wetland CH4 emissions roughly double by the 2090s relative to present-day emissions, with an increasing trend throughout the century. Based on the MAGICC6 approach, we find a 21st century wetland CH4 RF feedback ranging from 0.04 ± 0.002 W⋅m−2 in RCP2.6, to 0.08 ± 0.003 W⋅m−2 in RCP4.5, to 0.11 ± 0.004 W⋅m−2 in RCP6.0, to 0.19 ± 0.01 W⋅m−2 in RCP8.5 (Fig. 1B). These CH4 RFs estimated by MAGICC6 are equivalent to 0.04 ± 0.001 °C, 0.07 ± 0.004 °C, 0.08 ± 0.006 °C, and 0.12 ± 0.01 °C increases in global mean temperature (Fig. 1C) under RCP2.6, RCP4.5, RCP6.0 and RCP8.5, respectively. Compared with the anthropogenic CH4 emissions, wetlands account for 14.6 to 25.1% of the total projected RF change.

Fig. 1.

Fig. 1.

Simulated future wetland CH4 emissions, net RF, and net increase in global mean temperature using the simple carbon cycle climate model MAGICC6. Colored lines represent ensemble average estimates from using CMIP5 model outputs, and shaded areas represent the upper and lower range of estimates (Left). Mean and one-SD at the end of the 21st century (mean over AD 2099) for each metric are given by the bars (Right). (A) Simulated wetland CH4 emissions driven by CMIP5 datasets for four RCPs. (B) Net RF from anthropogenic emissions with consideration of wetland CH4 emissions feedback (solid lines) calculated by MAGICC6 and original projected RCPs without wetland CH4 feedback (dashed lines) in IPCC AR5 and CMIP5, as well as observed RF (black solid line) based on atmospheric measurement from National Oceanic and Atmospheric Administration (NOAA) Annual Greenhouse Gas Index (AGGI). (C) Change in global mean temperature caused by wetland CH4 feedback from MAGICC6 model.

The ensemble estimates of SGWP demonstrate the possibility that wetlands overwhelm anthropogenic CH4 emissions in driving future climate impacts under RCP26 (Fig. 2B). The wetland SGWP remains relatively constant at equilibrium state, and then varies with climate scenario (9.7 ± 0.3 kg CO2-eq⋅y−1, 10.7 ± 0.3 kg CO2-eq⋅y−1, 11.2 ± 0.4 kg CO2-eq⋅y−1, and 12.9 ± 0.7 kg CO2-eq⋅y−1 at the end of the 21st century for RCP26, RCP45, RCP60, and RCP85, respectively) (Fig. 2A). The constant SGWP represents an equilibrium state of the global methane budget before 1765, as assumed by IAM whereby chemical sinks balance most of natural emissions. The WDI exhibited large variation driven by RCP scenario, for example, for RCP2.6, natural wetlands clearly play a dominant role by the end of the 21st century, with WDI of −47 ± 9%. In contrast, the WDI kept a relatively constant value (55 ± 8%) since the 2050s under RCP8.5, suggesting that climate impact by wetlands is just half of the effect relative to increased anthropogenic emissions. Additionally, the climate feedback parameter, λ, from wetlands CH4 is ∼0.03 ± 0.001 W⋅m−2⋅K−1 under RCP85 (SI Appendix, Fig. S6), which falls within the range of previous estimates (2) and is approximately one tenth of the surface albedo feedback from melting snow and ice cover (31).

Fig. 2.

Fig. 2.

Evolving pattern of wetland and anthropogenic CH4 C change over varying time horizon since 1765 using simple sustained pulse−response model. (A) Time series of SGWP for wetland and anthropogenic CH4 emissions. (B) Comparison of RF dominance between wetland and anthropogenic emissions. Here RF dominance is defined as a ratio of SGWP from wetlands to SGWP from anthropogenic sources. Shaded areas represent the upper and lower range of wetland estimates. Here the SGWPs from wetland and anthropogenic emissions were calculated as integrated RF of CH4 since preindustrial time (1765).

Changes in 21st century wetland CH4 emissions are strongly linked to the climate response wetland area extent and seasonality, which showed a diverse response across biomes (SI Appendix, Fig. S1). Ignoring potential human modification of wetlands, e.g., peatland drainage, the mean annual maximum global wetland area is expected to be 13% larger (∼0.72 ± 0.19 Mkm2) in the 2090s for RCP8.5 scenario (SI Appendix, Fig. S2), whereas earlier studies have assumed no significant change in wetland area (32). Regionally, reduced precipitation causes a small decrease (∼0.06 ± 0.01 Mkm2 for RCP85) in tropical wetland area, whereas thawing of the near-surface permafrost stimulates a large increase (∼0.58 ± 0.15 M⋅km2 for RCP85) in boreal wetland area. However, despite decreasing tropical wetland extent and increased frequency of tropical drought, tropical wetlands remain the world’s largest natural source responsible for ∼53.2 ± 0.7% by the end of the 21st century in RCP8.5. The annual contribution of boreal wetlands increases by ∼3.6 ± 0.5% from the present to the end of the 21st century, indicating higher sensitivity to climate change-driven CH4 emissions in boreal regions because of thawing permafrost.

The increase in methane-producing wetlands in boreal regions was due primarily to increased near-surface soil moisture following permafrost thaw. More than half of global wetland area is positively correlated with air temperature while ∼40% is negatively correlated (SI Appendix, Fig. S3). For instance, the West Siberian Lowland (WSL), one of the largest boreal wetlands, comprising ∼12.9% of the global peatland area, exhibits an increase in CH4 emissions during the transition from winter to spring, i.e., December to May (SI Appendix, Fig. S4). This originates from an increase in the thaw period and from higher heterotrophic respiration induced by higher soil temperatures. Projected thawing of permafrost and associated wetland expansion will largely affect CH4 emissions from the taiga forest region in the WSL. From around the mid-2040s, a strong linear increase (R2 = 0.93, P < 0.01) of CH4 emissions with time, at a rate of 0.16% per year from winter to spring seasons, will occur under RCP8.5, despite environmental conditions changing more slowly in the WSL (R2 < 0.21, P > 0.01) under all scenarios (Fig. 3A).

Fig. 3.

Fig. 3.

Regional changes in wetland area extent and CH4 emissions. (A) Contribution of CH4 emissions from cold seasons (December to May) in boreal wetlands in WSL. Thick lines correspond to linear regression fits of ensemble anomalies. ΔCH4 represents increasing contribution of CH4 emission from cold seasons as percentage. (B) Annual variability in CH4 emissions for the Amazon basin, which is defined as SDs of CH4 fluxes within a year.

Long-term simulated tropical CH4 emission changes are mainly associated with a shift in precipitation patterns. The partial correlation between global CH4 emissions and climatic variables shows that spatial variation of CH4 emissions is associated mainly with precipitation, and that this is especially important in tropical regions where the annual cycle of wet to dry seasons varies considerably. Consistent with an observed increase in the dry season in Amazonia since 1979 (11), our ensemble estimates predict a slightly negative trend in the basin-wide annual areal maximum of Amazonian wetlands by ∼4% by the 2090s under RCP8.5. Despite there being no significant change in the proportion of CH4 emissions from dry seasons across all RCP scenarios, we did find a steady increase in annual variability of CH4 emissions (Fig. 3B).

We found a statistically significant relationship between seasonal wetland area variability and the increase in annual CH4 emissions, despite diverse mechanisms driving large-scale CH4 emission changes among wetlands (Fig. 4A). In addition, we show that seasonality of wetland area is an indicator for monitoring the long-term dynamics of CH4 emissions at continental scale. Altered patterns in the trend of wetland variability coincide with the onset of a strong linear increase in CH4 emissions in boreal wetlands, which suggests that CH4 emissions are largely increased during cold seasons (December to February, March to May) afterward (SI Appendix, Fig. S5). The net growth rate of CH4 emissions from the summer to autumn seasons is larger than that from the winter to spring seasons after the 2040s. In addition, the growth rates measured by regression lines among all regions characterize the strength of emitting CH4 among major regions, where tropical wetlands show higher contributions than the other regions.

Fig. 4.

Fig. 4.

Role of regional wetlands in changing wetland status and CH4 emissions. (A) Scatterplot shows relationship between ensemble anomalies of annual wetland variability and anomalies of annual CH4 emissions relative to 1960–1990 average levels for regional wetlands under RCP8.5. The linear least square regression fits represent the evolving trajectories of CH4 emissions with increasing CH4 emissions. The horizontal arrow represents the direction of increasing wetland CH4 emissions with shifting patterns of inundation seasonality. The vertical arrow represents the evolving directions of both CH4 emissions and inundation seasonality with time. (B) Increment of CH4 emissions with rising temperature for regional wetlands. Background colors represent increases of global temperature from ensemble estimate of CMIP5 models under RCP8.5. Dots indicate regional increase of temperature at certain time. Details of calculation are provided in SI Appendix, Methods.

Our CH4 RF estimates are subject to considerable uncertainties associated with estimation of natural sources and the resulting climate feedback. The representation of processes in LPJ-wsl assumes no effect of shifting spatial pattern of vascular plants on CH4 transport from soil into atmosphere, which could lead to an underestimation of CH4 emissions. Furthermore, microbial community composition might play an important role in driving CH4 fluxes, but the biogeographical distribution of methanogen communities and their metabolic processes at ecosystem-scale are poorly understood due to the lack of observational data. In addition, uncertainties in RF estimates are also associated with the parameter values of the CH4 lifetime and variations of global chemical CH4 sinks, e.g., OH concentrations. To better understand the evolution of atmospheric CH4 concentrations in the future, comprehensive in situ and remote sensing monitoring of CH4 emissions and changes in wetland area are required.

The potential sensitivity of wetland CH4 emissions to rising temperature highlights the need for limiting global warming below the 2 °C target. Climate-driven CH4 emission feedbacks were positive for each wetland region (Fig. 4B), with large variability related to the different sensitivities of methanogenesis, freeze−thaw dynamics, and surface inundation. The timing of feedbacks was also variable, with increases in tropical wetlands emissions appearing to have a fairly abrupt response once global mean temperature approached 2 °C warming, whereas boreal wetlands, especially boreal North America, had more gradual increases in emissions due to expanding wetland area (33). Taking into account these additional changes in RF caused by increasing wetland CH4 emissions emphasizes the need to consider wetland CH4 feedbacks in IAM and to develop comprehensive greenhouse gas mitigation strategies. In addition, policy-relevant temperature targets must continue to incorporate assessments of feedbacks from terrestrial and oceanic systems for both CO2 and non-CO2 gases, like methane and nitrous oxide. With atmospheric methane concentrations now tracking the more fossil fuel-intensive scenarios (34), further insight into the climate sensitivity of methane sources and their chemical sinks remains of high importance.

Supplementary Material

Supplementary File

Acknowledgments

We thank Benjamin D. Stocker, Thomas Peter, Joeri Rogelj, and Leonardo Calle for constructive comments on the manuscript. We also thank Wolfgang Lucht and the anonymous reviewers for their detailed comments on the manuscript. We acknowledge the World Climate Research Programme’s Working Group on Coupled Modeling, which is responsible for CMIP, and we thank the climate modeling groups for producing and making available their model outputs. Computational efforts were performed on the Hyalite High-Performance Computing System, operated and supported by Montana State University Information Technology Research Cyberinfrastructure. This study was funded by the Competence Center Environment and Sustainability (CCES) Project Modeling and Experiments on Land-Surface Interactions with Atmospheric Chemistry and Climate Phase 2 (MAIOLICA2) 42-01, Chinese Academy of Sciences (CAS) Project Big Earth Data Engineering, and the National Natural Science Foundation of China (Grants T411391001 and 91425303). This paper does not reflect the official views or policies of the United States Government or any agency thereof, including the Department of Energy.

Footnotes

The authors declare no conflict of interest.

This article is a PNAS Direct Submission. W.L. is a guest editor invited by the Editorial Board.

This article contains supporting information online at www.pnas.org/lookup/suppl/doi:10.1073/pnas.1618765114/-/DCSupplemental.

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