Abstract
The land and ocean act as a sink for fossil-fuel emissions, thereby slowing the rise of atmospheric carbon dioxide concentrations1. Although the uptake of carbon by oceanic and terrestrial processes has kept pace with accelerating carbon dioxide emissions until now, atmospheric carbon dioxide concentrations exhibit a large variability on interannual timescales2, considered to be driven primarily by terrestrial ecosystem processes dominated by tropical rainforests3. We use a terrestrial biogeochemical model, atmospheric carbon dioxide inversion and global carbon budget accounting methods to investigate the evolution of the terrestrial carbon sink over the past 30 years, with a focus on the underlying mechanisms responsible for the exceptionally large land carbon sink reported in 2011 (ref. 2). Here we show that our three terrestrial carbon sink estimates are in good agreement and support the finding of a 2011 record land carbon sink. Surprisingly, we find that the global carbon sink anomaly was driven by growth of semi-arid vegetation in the Southern Hemisphere, with almost 60 per cent of carbon uptake attributed to Australian ecosystems, where prevalent La Niña conditions caused up to six consecutive seasons of increased precipitation. In addition, since 1981, a six per cent expansion of vegetation cover over Australia was associated with a fourfold increase in the sensitivity of continental net carbon uptake to precipitation. Our findings suggest that the higher turnover rates of carbon pools in semi-arid biomes are an increasingly important driver of global carbon cycle inter-annual variability and that tropical rainforests may become less relevant drivers in the future. More research is needed to identify to what extent the carbon stocks accumulated during wet years are vulnerable to rapid decomposition or loss through fire in subsequent years.
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Main
Each year, on average, land and ocean carbon sinks absorb the equivalent of about half of the global fossil fuel emissions, thereby providing a critical service that slows the rise in atmospheric CO2 concentrations1. Emissions from fossil fuels and land-use change now exceed ten billion tons or petagrams (Pg) of carbon per year, tracking the most carbon intense emission scenarios of the Intergovernmental Panel on Climate Change4. Even with this acceleration, the fraction of anthropogenic emissions that accumulates in the atmosphere (the airborne fraction) has remained largely unchanged since 1959 at 44% (ref. 2) (P = 0.36 for slope of linear regression). This implies that the uptake of carbon by ocean and terrestrial processes has, to some extent, kept pace with accelerating emissions owing to a range of possible factors, such as the fertilization effect of increased CO2 and atmospheric nitrogen deposition on plant growth, changes in growing season length, and land management5. In addition to the continued uptake of CO2, the airborne fraction exhibits large variability on interannual timescales, ranging between 18% and 79% during the past 54 years (ref. 2). This high interannual variability is primarily driven by terrestrial processes, which must be better understood in order for us to be able to forecast long-term biospheric responses to climate change3.
High uncertainties in quantifying ecosystem processes mean that the global terrestrial carbon sink is often estimated as the residual between emissions from the combustion of fossil fuels, cement production and net land-use change, and sinks combining accumulation in the atmosphere and uptake by the ocean6. Using this method, the Global Carbon Project reported in their annual assessment a 2011 residual land sink of 4.1 Pg C yr−1 (standard deviation ± 0.9 Pg C yr−1), representing an unusually large increase compared with the 2.6 ± 0.8 Pg C yr−1 decadal average and the largest reported residual land carbon sink since measurements of atmospheric CO2 began in 1958. The 2011 residual land sink is indicative of several aspects of the debate surrounding the fate of terrestrial ecosystems under environmental change. First, the large uptake of carbon in 2011 continues a trend of increasing strength in the land carbon sink over at least one decade1,7. Second, the large annual growth anomaly in the land carbon sink raises questions regarding the growth rate of atmospheric CO2 in coming years and how this is affected by the allocation of sequestered carbon to either labile or more stable pools. Lastly, increasing uncertainty in other terms of the global CO2 budget has direct consequences on land sink estimates, for example, an overestimate of anthropogenic emissions would be assigned (owing to mass conservation and current accounting schemes) as an erroneously large land sink. Thus, attributing changes in net carbon uptake to carbon cycle processes requires a range of methodological approaches.
Here, we investigate the evolution of the terrestrial carbon sink over the past 30 years and the underlying mechanisms of the exceptionally large 2011 residual land carbon sink in a long-term context using (1) a ‘bottom-up’ process-oriented terrestrial biosphere model, (2) a ‘top-down’ atmospheric CO2 inversion and (3) satellite observations of photosynthetic activity and vegetation structure. We allocate net land carbon uptake among specific geographic regions and provide a mechanistic explanation for the climatic and CO2 response of net primary production (NPP), heterotrophic respiration (Rh), and disturbance that sum up to define net ecosystem exchange (NEE).
We find excellent agreement among the three different terrestrial carbon sink estimates that robustly support record 2011 land carbon uptake (Fig. 1a; with uncertainty presented as ±1 standard deviation). The Lund–Potsdam–Jena (LPJ) dynamic global vegetation model (DGVM; ref. 8) estimates a 2011 land sink of 3.9 ± 1.3 Pg C yr−1, a 1.3 ± 0.6 Pg C yr−1 anomaly compared to the 2003–2012 mean sink of 2.6 ± 0.9 Pg C yr−1 (Fig. 1a and Extended Data Table 1). Our atmospheric inversion (using the Monitoring Atmospheric Composition and Climate (MACC-II) inversion system; ref. 9) yields a 3.7 ± 0.4 Pg C yr−1 2011 land sink, equivalent to a 1.0 Pg C yr−1 anomaly above the 2.7 ± 0.4 Pg C yr−1 inversion average for 2003–2012. The 2011 land sink estimates by the LPJ DGVM and MACC II inversion were greater than the 97.5th percentile over the period 1981–2012, suggesting a convergence of particularly novel ecosystem and climate states.
a, Annual NEE, where positive values represent carbon uptake, blue is LPJ, red is MACC-II, and the residual land sink is in grey. The standard deviations are ±0.58 Pg C yr−1 for LPJ, ±0.4 Pg C yr−1 for the inversion, and ±0.8 Pg C yr−1 for the residual (see Methods). b, Average, 2003–2012, annual NEE for the Northern and Southern hemispheres, estimated by LPJ and the inversion. c, AVHRR FPAR anomalies for the southern (S) and northern (N) hemispheres with respect to the 1982–2011 long-term average where the seasonal anomalies were calculated as the z score for each season (s) and each grid cell (i,j) for each year (y);
.
Both the atmospheric inversion and the DGVM demonstrate an increased contribution from Southern Hemisphere ecosystems to global net carbon uptake in 2011 (Fig. 1b). These patterns are supported by a large observed positive anomaly in the 2010–2011 interhemispheric CO2 concentration gradient between Mauna Loa (19° N) and the Cape Grim (40° S) monitoring stations10. An increase in global NPP appears to be the main driving mechanism behind the 2011 land sink. Global NPP anomalies within the range of 1.7 Pg C simulated from the LPJ model forced with monthly climatic variables from the Climatic Research Unit (CRU) TS3.21 data set (ref. 11) and 1.6 Pg C by the Moderate Resolution Imaging Spectroradiometer (MODIS) NPP algorithm (Fig. 2a), using National Center for Environmental Prediction (NCEP) Reanalysis climate data and a light use-efficiency model12 provide parallel support for this conclusion. Further investigation shows 79% (MODIS) to 87% (LPJ) of the global NPP anomaly is explained by just three semi-arid regions, Australia, temperate South America and southern Africa, where ecosystem respiration tends to lag productivity, inducing large net carbon uptake (regions AUST, SAmTe and SAf in Fig. 2b and Extended Data Fig. 1)13,14,15. In Australia, for example, compared with the 2003–2012 average, LPJ simulated a 45% increase in NPP for 2011, from an average of 1.75 to 2.54 Pg C yr−1, but only a 9% increase in Rh (from 1.48 to 1.61 Pg C yr−1). Moreover, wetter conditions decreased modelled fire-emissions by 29% (from 0.13 to 0.09 Pg C yr−1) yielding a net 0.84 Pg C 2011 sink. Similarly, we find our conclusions for the greater sensitivity of NPP to precipitation, and lags in Rh, extend to southern Africa and temperate South America. In fact, 51% of the global 2011 net carbon sink was attributed to the three Southern Hemisphere semi-arid regions (Extended Data Table 2), and Australia alone contributed to 57% of the total global LPJ NEE anomaly.
a, Annual NPP anomaly, as z score (defined in Fig. 1), estimated by the MOD17A3 algorithm that uses the MODIS leaf area index (MOD15 Collection 5)12. b, Annual NEE anomaly, as z score, estimated by the LPJ DGVM, where a positive z score equals a larger sink; the reference period is 2000–2011. c, Spatial pattern of the contribution of precipitation to net ecosystem exchange in 2011 calculated as the difference between NEE with the all climate forcing varied and NEE simulated with the precipitation climatology (see Extended Data Fig. 6a and b for the NPP and Rh component fluxes).
In addition to MODIS, the fraction of photosynthetic active radiation (FPAR) determined from the satellite-borne Advanced Very High Resolution Radiometer (AVHRR), AVHRR-FPAR3g (ref. 16), provides a long-term record of space-borne observations of the fraction of photosynthetic active radiation absorbed. Vegetation greening was widespread globally in 2011, with austral winter (June–August; JJA) FPAR reaching the highest values ever observed in the entire satellite period (1982–2011). In the Southern Hemisphere, record greening (Fig. 1c) was centralized over the same three Southern Hemisphere semi-arid regions (AUST, SAmTe and SAf) and was sustained for nine months spanning 2010 to 2011 (December–February, DJF; March–May, MAM; and JJA). Seasonal FPAR increases over Australia ranged from 4.6% in DJF and 8.7% in MAM to 5.1% in JJA, with all anomalies being prominent extremes in the context of an observed 0.8–1.9% interannual variability over the past 30 years. Notably, 46% (or 34%) of the land area in Australia experienced increases in FPAR in 2011 of more than 2.5 (or 3.0) standard deviations from normal in MAM, with positive FPAR anomalies first developing in eastern Australia in DJF, extending to all of Australia in MAM, then remaining in northern Australia in JJA (Extended Data Fig. 2).
To identify proximate causes for the role of semi-arid regions in the 2011 global sink, we performed a full set of LPJ factorial model simulations to isolate the temperature, precipitation, cloud cover and CO2 contribution to NEE (Extended Data Table 1; Methods). An additional ‘memory’ simulation was conducted to evaluate previous-year climate effects that might have contributed to the extraordinary sink in 2011; the 2010 climate was replaced with a near-neutral year (2009) for the El Niño Southern Oscillation (Extended Data Fig. 3). With respect to pre-industrial CO2 concentrations (287 parts per million, p.p.m.), the LPJ simulations suggest that CO2 fertilization enhanced the 2011 net carbon uptake by 4.8 Pg C. High precipitation during 2010 and 2011 contributed to 0.62 Pg C and 0.52 Pg C of the global sink, respectively (Fig. 2c), or about 12%, thereby helping to offset land-to-atmosphere CO2 fluxes driven by long-term negative temperature (−0.84 Pg C) and direct radiative contributions (−0.32 Pg C). In addition, ‘memory’ effects from 2010 added to the 2011 sink, with the largest difference being a threefold increase in tropical South American NEE when using 2009 climate before 2011. The increase in Amazonian NEE in 2011 was mainly due to recovery from the 2010 Amazon drought17, which caused a reduction in LPJ NPP and an increase in LPJ Rh in 2010, leading to reduced short-lived litter carbon pools available for respiration and fire in 2011. Although 2011 precipitation explained most of the NEE increase in Australia (a 0.56 Pg C yr−1 contribution), the climate memory effect also explained 0.21 Pg C of the 2011 Australian sink because of high precipitation in 2010 that recharged soil moisture and plant carbohydrate reserves to the benefit of NPP in 2011. Among an ensemble of climate indices, the Multivariate El Niño Index (MEI; ref. 18) consistently explained the highest amount of year-to-year variability over Australia for annual carbon uptake (correlation coefficient r = −0.49, P < 0.01) and DJF FPAR greening (r = −0.52, P < 0.01) between 1981 and 2011 (Extended Data Fig. 4a–d). This extends earlier findings that found Pacific sea surface temperature as a significant predictor of precipitation-driven greening anomalies as far as South Africa and Australia19,20. Notably, the 2010/2011 La Niña—that is, the MEI negative phase—took place over an especially long time period, as observed from multiple satellite, rain gauge and reanalysis data sources (the Tropical Rainfall Measurement Mission (TRMM), CRU and NCEP-DOE; Extended Data Fig. 5a and b), and even lowered global sea levels21, in addition to altering global carbon uptake12.
The available evidence points towards an enhanced climatic effect of the 2010/2011 La Niña from interactions with long-term semi-arid region greening trends since the early 1980s at the latest. For example, since 1982, we found an expansion of vegetation across the Australian landscape (P < 0.01 for one-sided Kolmogorov–Smirnov test) where land area with FPAR >20% (or 30%) increased by 5.6% (or 3.5%) in the MAM growing season. The greening trend in semi-arid regions has been previously associated with a range of drivers that include altered precipitation frequency and intensity22, increased water-use efficiency due to elevated CO2 effects on leaf stomatal conductance23, and woody encroachment following land-use and grazing22,24. Over the same 1982–2011 time period, we observed a statistically significant increase in the sensitivity of LPJ net carbon uptake (P < 0.001) and AVHRR-FPAR3g vegetation activity (P < 0.02) to austral-autumn precipitation for the Australian continent (Fig. 3a). The observed change in ecosystem sensitivity over Australia meant that an additional 100 mm of growing season (MAM) precipitation led to a fourfold increase in net carbon uptake when comparing sensitivities before (0.2 Pg C yr−1 per 100 mm) or after (0.8 Pg C yr−1 per 100 mm) 1997, the midpoint of current observational records (1982–2011). An independent data-driven model of net ecosystem production25, which excluded disturbance processes, confirmed the same statistically robust increase over time in carbon uptake per unit precipitation for Australia (Fig. 3b, P < 0.001). Long-term observations from passive-microwave vegetation optical depth (VOD)26 suggest that the enhanced sensitivity of vegetation to climate is a result of both increases in grass cover as well as from woody encroachment (Fig. 3c).
a, Climate sensitivity of annual LPJ NEE anomalies to MAM precipitation anomalies for Australia. The open circles and dashed line are the points and regression line for 1982–1996 (
) and the closed circles and solid line are for 1997–2011 (
+
), from the following linear regression model using NEE and precipitation anomalies (Panomaly) where A is an indicator variable for the different time periods: (
). b, Climate sensitivity of annual NEE from the MACC-II inversion (black symbols) and the upscaled NEP product (grey symbols) using the same linear model as in a. c, Climate sensitivity of annual VOD (light green symbols) and MAM FPAR (dark green symbols) also using the model described in a.
The 2011 land carbon sink anomaly indicates a novel climate-driven response of the biosphere where interactions between extremes in austral precipitation27 and changes in land cover23 (both possibly caused by humans) are contributing to non-analogue ecosystem behaviour with global biogeochemical significance. We propose that the current paradigm, whereby tropical rainforest El Nino/Southern Oscillation coupling dominates interannual variability of the atmospheric CO2 growth rate3,28, may become less relevant in the future. We explored whether semi-arid carbon-cycle climate sensitivity feedbacks exist among an ensemble of 15 Earth system models contributed to the Coupled Model Intercomparison Project Phase 5 (CMIP5; ref. 29). In contrast to our observations, we found that for semi-arid regions, modelled carbon uptake and precipitation sensitivity remains relatively stable over the 1990 to 2090 period for the CMIP5 ensemble (P = 0.33, one-sided Student’s t-test, Fig. 4). This suggests that processes contributing to the novel ecosystem dynamics identified here may be overlooked in future climate change scenarios. As the dynamics of dryland systems, which cover 45% of the Earth’s land surface, increase in global importance, more research is needed to identify whether enhanced carbon sequestration in wet years is particularly vulnerable to rapid decomposition or loss through fire in subsequent years, and is thus largely transitory. Such behaviour may already be reflected by the larger-than-average atmospheric growth rate in 2012 (ref. 30) that was associated with a return to near-normal terrestrial land sink conditions (Fig. 1a).
Distribution of the change in sensitivity between the periods 1979–2005 and 2069–2095 in net biome production to annual precipitation for four biomes (n = 15 CMIP5 Earth System Models). Precipitation sensitivity was estimated as
while controlling for changes in sensitivity due to CO2 and air temperature
. The different lines refer to tropical (green), temperate (brown), semi-arid (tan), and boreal (purple) biomes.
Methods Summary
We use multiple data sources, including carbon accounting methods, carbon-cycle model simulations, and satellite-based vegetation products to investigate the magnitude and mechanisms driving variability in the terrestrial carbon sink. NPP (the total photosynthesis minus plant autotrophic respiration losses) is simulated by the LPJ DGVM and also estimated independently with the MODIS NPP algorithm, MOD17A3. The balance between carbon uptake from NPP and losses from soil respiration and disturbance (NEE) is quantified from the Global Carbon Project, the LPJ DGVM, and the MACC-II atmospheric inversion system (http://www.copernicus-atmosphere.eu/). NEP (the balance between gross carbon inputs from photosynthesis and losses from ecosystem respiration, excluding disturbance) is estimated from upscaled gridded flux tower observations. Optical and passive microwave satellite data are employed to assess vegetation greenness trends (AVHRR FPAR3g) and vegetation structure or vegetation optical depth (VOD). Monthly and seasonal precipitation fluctuation is quantified from TRMM 3B43v7 (http://mirador.gsfc.nasa.gov) and NCEP-DOE Reanalysis II (http://www.esrl.noaa.gov), and the Climatic Research Unit (CRU) TS3.21 (http://www.cru.uea.ac.uk/). Regional summaries of the global gridded data followed boundaries from the eleven land regions specified in the TRANSCOM atmospheric inversion experiment. We further differentiate North and South Africa to distinguish between wet and semi-arid climates with the ratio of precipitation to potential evaporation set to 0.7. Historical (1860–2005) simulations of net biome production, equivalent to NEE, from the Fifth Coupled Model Intercomparison Project (CMIP5) are merged with the Representative Concentration Pathway 8.5 (RCP8.5) to create temporal composites spanning 1860–2099 for 15 Earth system models.
Online Methods
Carbon fluxes and their uncertainties
We follow the carbon-cycle definitions summarized by ref. 31 when describing the net land carbon sink in terms of NEE or NEP and associated component fluxes. Data for estimating the airborne fraction, the residual land sink and its anomalies were obtained online from the Global Carbon Project2 (version 1.5) for the years 1959–2011. Uncertainties are presented as ±1 standard deviation (σ), assuming Gaussian error and a 68% likelihood that the true value is within this range. The LPJ DGVM was run with the GlobFirm fire module enabled and fully prognostic dynamic natural vegetation (excluding land-cover change). The CRU TS3.21 climate data set11 was used for LPJ model simulations starting in 1901 and ending in 2012 with observed rising CO2 concentrations from ice-core measurement of CO2 and then the Mauna Loa Observatory after 1958. Uncertainty in LPJ NEE was estimated using a Latin hypercube approach to generate 200 parameter sets and corresponding simulations at 1-degree spatial resolution for 13 of the most important parameters32. The observed linear relationship between the Latin hypercube model ensemble global mean NEE and its standard deviation (R2 = 0.62) was used to predict the 2011 land sink uncertainty for the 0.5-degree simulation. Uncertainty from climate forcing was considered by comparing different climate data sets (see below) and is not likely to affect annual anomalies or trends in carbon fluxes33. LPJ simulates semi-arid plant functional types by a mix of grasses with C3 and C4 photosynthetic pathways and, in lesser abundance, tropical and temperate trees. Carbon cycle fluxes simulated by LPJ were in close agreement with regionally parameterized models for Australia, such as CABLE14, and regional NPP from satellite-based estimates of MODIS (Extended Data Table 2). Simulated losses of carbon from fire and their anomalies were benchmarked with the GFAS v1.0 (ref. 34) and GFED v3.1 (ref. 35) data sets that use satellite-observed fire radiative power and burned area, respectively, to estimate carbon emissions (Extended Data Table 3). The atmospheric inversion was based on the MACC-II inversion system version 12.1, described in ref. 9, using atmospheric CO2 data sets from a global network (NOAA/ESRL, WDCGG, CarboEurope and RAMCES) of continuous and discrete flask samples, with a climatological prior for NEP land-surface carbon fluxes from the ORCHIDEE DGVM9 and fire emissions from GFED v2.1 (ref. 36) until 2011, and the long-term mean substituted for 2012. The inversion is applied on a 3.75 × 2.5 degree grid with fluxes inverted at weekly resolution and night-time and daytime fluxes separated. The MACC-II inversion minimizes a Bayesian objective function, assuming errors are Gaussian (posterior errors presented here as ±1 standard deviation), and error correlation implied by off-diagonal elements in the posterior error covariance matrix. Upscaled flux tower observations were the basis for the data-derived NEE model of ref. 25, representing monthly 0.5-degree fluxes from 1982 to 2011. The MODIS (MOD17A337) product provided annual NPP data at 1-km resolution and was resampled to a resolution of 8 km to match AVHRR-FPAR3g before analysis. Net biome production from the CMIP5 RCP8.5 ensemble29,38 was merged with the corresponding historical simulations to create temporal composites covering the years 1860–2099 for 15 Earth system models (Extended Data Table 4).
Vegetation activity
Measurements of FPAR were modelled from surface reflectance observed aboard the AVHRR and incorporated into the FPAR3g16 data set (1981–2011). The FPAR3g bimonthly data set was first filtered for low values, within the range of uncertainty (<2.5%), before compositing to monthly values using a maximum values approach. Gridded passive microwave measurements of VOD from39 were aggregated from 0.25-degree resolution to each of the thirteen regional means at a monthly resolution from 1988 to 2011. The VOD is an indicator of water content in both woody and leaf components of aboveground biomass. The VOD time series is based on a multi-source data set consisting of harmonized passive microwave measurements from SSM/I (Special Sensor Microwave Imager, 1988–2007) and AMSR-E (the Advanced Microwave Scanning Radiometer – Earth Observing System, July 2002–September 2011) sensors39.
Climate data sets
Precipitation data from satellite (TRMM 3B43v7), reanalysis (NCEP-DOE Reanalysis II40, 1979-2012), and ground-based observations (CRU TS3.2111) were compared with one another for annual and seasonal similarities (Extended Data Fig. 5a and b). Over Australia, annual precipitation was observed as up to +205 ± 54 mm (in 2010) and +178 ± 71 mm (in 2011) above the long-term annual average of 555 ± 23 mm yr−1, with uncertainties presented as the standard deviation of the three products. An ensemble of climate indices were evaluated (Extended Data Fig. 4a–d) with data for the MEI from ref. 18, where negative values indicate the La Niña climate mode.
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Acknowledgements
We acknowledge support from the EU FP7 GEOCARBON programme (283080), and thank the researchers involved with collecting and maintaining the climate data at the Climate Research Unit, University of East Anglia, UK, and the National Center for Atmospheric Research, USA. We also acknowledge the World Climate Research Programme’s Working Group on Coupled Modelling, which is responsible for CMIP. We thank the climate modelling groups for producing and making available their model output. For CMIP the US Department of Energy’s Program for Climate Model Diagnosis and Intercomparison provides coordinating support and led development of software infrastructure in partnership with the Global Organization for Earth System Science Portals. We also thank M. Jung for providing the ‘upscaled’ NEE data used in our analysis. J.G.C. acknowledges the support of the Australian Climate Change Science Program. R.B.M. and S.W.R. were funded by the NASA Earth Science Division. C. Le Quéré and L. Cernusak provided comments and suggestions that improved the manuscript. This paper is a contribution to the Global Carbon Budget activity of the Global Carbon Project.
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B.P., D.F., P.C. and R.B.M. designed the analyses. J.B., F.C., G.B., D.F., R.B.M., S.W.R., S.S., G.R.v.d.W., J.G.C., Y.Y.L. and N.A. contributed data to the analyses. B.P., F.C., R.B.M., S.R. and D.F. conducted the analyses. All authors contributed to the writing of the manuscript.
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Extended data figures and tables
Extended Data Figure 1
The thirteen regions used throughout the analysis, 11 from TRANSCOM, and two additional regions for the African continent that are semi-arid (see Methods Summary).
Extended Data Figure 2 Seasonal AVHRR FPAR anomalies (z score) for the year 2011.
The z score is calculated relative to the long-term seasonal mean and standard deviation of FPAR (1982–2011); see legend to Fig. 1c. The seasons DJF, MAM, JJA and SON are defined by the first letter of each month.
Extended Data Figure 3 Forcing contribution to NEE and the MEI and PDO indices.
The full climate attribution of the global land sink simulation by the LPJ DGVM is shown in the bar graph. PDO, Pacific Decadal Oscillation.
Extended Data Figure 4 r and FPAR correlations between climate modes for NEE at given seasons.
Shown is r (on the colour scales) between climate modes and MAM (a), and JJA (b) NEE simulated by LPJ for each of the TransCom regions. FPAR correlations between climate modes are shown for MAM (c) and JJA (d). The correlations were made for 1982–2011. Blank boxes indicate correlation between −0.1 and 0.1.
Extended Data Figure 5 Global climate anomalies for air temperature and precipitation.
a, Global temperature and precipitation anomalies from CRU TS3.21 data. The anomalies are with respect to 1979–2012 seasonal means. b, Seasonal precipitation anomalies (z score) for year 2010. c, Seasonal precipitation anomalies (z score) for year 2011. The z score for b and c is calculated relative to the long-term seasonal mean and standard deviation of precipitation (1979–2011).
Extended Data Figure 6 Spatial pattern of the contribution of precipitation to NEE exchange in 2011.
This is calculated as the difference between NPP (a) and Rh (b) with the all-climate forcing varied and NEE simulated with the precipitation climatology. This is the same as in Fig. 2c but for component fluxes of NEE.
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Poulter, B., Frank, D., Ciais, P. et al. Contribution of semi-arid ecosystems to interannual variability of the global carbon cycle. Nature 509, 600–603 (2014). https://doi.org/10.1038/nature13376
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DOI: https://doi.org/10.1038/nature13376






