Internal climate variability and spatial temperature correlations during the past 2000 years
- 1Department of Earth Sciences, Vrije Universiteit Amsterdam, Amsterdam, the Netherlands
- 2Earth and Life Institute (ELI), UCLouvain, Louvain-la-Neuve, Belgium
- 3Laboratoire des Sciences du Climat et de l'Environnement, LSCE/IPSL, Université Paris-Saclay, Gif-sur-Yvette, France
Correspondence: Pepijn Bakker (email@example.com)
The spatio-temporal structure of natural climate variability has to be taken into account when unravelling observed climatic changes and simulating future climate change. However, based on the comparison of temperature reconstructions and climate model simulations covering the past 2 millennia, it has been argued that climate models are biased. They would simulate too little temporal temperature variability and too high correlations between temperature time series from different continents. One of the proposed causes is the lack of internal climate variability in climate models on centennial timescales, for instance variability related to the Atlantic meridional overturning circulation (AMOC).
We present a perturbed-parameter ensemble with the iLOVECLIM Earth system model containing various levels of AMOC-related internal climate variability to investigate the effect on the spatio-temporal temperature variability structure. The model ensemble shows that enhanced AMOC variability indeed leads to more continental-scale temperature variability, but it also increases the spatio-temporal temperature correlations between different continents. However, combining the iLOVECLIM results with CMIP5 model results and various PAGES-2k temperature field reconstructions, we show overall agreement for the magnitude of continental temperature variability in models and reconstructions, but both the simulated and the reconstructed ranges are large. This is even more true when considering higher-order metrics like inter-continental temperature correlations or temperature variability land–sea contrasts. For such metrics, uncertainties in both model results and temperature reconstructions are so large that they hamper our ability to constrain simulated spatio-temporal structure of centennial temperature variability. As a result, we cannot determine the importance of AMOC variability for the climatic evolution over the past 2 millennia.
Comparing reconstructed and simulated past climate variability helps us to understand natural climate variability, which is important in the light of ongoing climate change (Braconnot et al., 2012; Deser et al., 2012). The most recent 2 millennia form an important period in this respect because they (i) are described by what is probably the highest density of palaeoclimate reconstructions of any past period (Ahmed et al., 2013; PAGES2k-Consortium, 2017); (ii) are a period with relatively weak and well-constrained external forcings, allowing for a better investigation of unforced climate variability (Jungclaus et al., 2017); and (iii) are within a period that is very similar to the present and future climate in terms of mean climate, boundary conditions, and climate forcings (except for human-induced changes) (Schmidt, 2010).
Previous studies looking at temperature temporal variability have suggested that climate models simulate too little regional variability on multi-decadal and longer timescales (Laepple and Huybers, 2014; PAGES 2k-PMIP3 group, 2015). One can also compare reconstructed and simulated climate variability in the spatio-temporal domain, as the covariance varies as a function of the spatial and timescales investigated (Kunz and Laepple, 2021). For instance, PAGES 2k-PMIP3 group (2015) compared the PAGES-2k temperature reconstructions (Ahmed et al., 2013) for seven continental-scale regions with transient climate model simulations over the past 2000 years from the third Palaeoclimate Modelling Intercomparison Projects (PMIP3; Braconnot et al., 2012) and focused on the correlations between temperature time series from different continental-scale regions. Based on this analysis, PAGES 2k-PMIP3 group (2015) found that the reconstructions show weak surface air temperature covariance across continents, in contrast to relatively strong covariance found in climate models.
Several possible causes have been put forward to explain those model–data discrepancies in both the time and spatio-temporal domains. The model–data mismatches could be related to the reconstructions, with proxy-specific uncertainties inherent to the data that lower the reconstructed covariance (Hartl-Meier et al., 2017). Other sources of uncertainty are the model sensitivity to external forcings, such as volcanic eruptions and solar forcing, or the magnitude of the reconstructed external forcings. Interestingly, it has both been argued that the model response to external forcings is too weak, thus explaining the lack of model variability on long timescales (Laepple and Huybers, 2014), and that the model response to external forcings is too strong (Anchukaitis et al., 2010; Braconnot et al., 2012; PAGES 2k-PMIP3 group, 2015; Stoffel et al., 2015), thus explaining the large degree of temperature covariance in the models between different continents. Another explanation that has been put forward to explain model–data mismatches in temperature variability is the lack of models with sufficient internal climate variability (Laepple and Huybers, 2014; Valdes, 2011). The idea behind the latter is that increased internal climate variability would increase temperature variability and potentially weaken temperature covariance across continental-scale regions because it would add “random noise” to the system. On the other hand, modes of internal climate variability have a clear spatial structure and can thus also enhance the spatio-temporal covariance by increasing the strength of climatic teleconnections between regions (PAGES 2k-PMIP3 group, 2015).
Here, we will investigate the impact of ocean-induced multi-decadal to multi-centennial climate variability on the spatio-temporal covariance of the temperature evolution. Hereby, we test if increased internal climate variability can indeed improve the model–data comparison of temperature variability over the last 2000 years. We will specifically investigate the impact of ocean variability driven by the Atlantic meridional overturning circulation (AMOC). To this end, we will present a perturbed-parameter ensemble of climate model simulations for the past 2 millennia that cover a range from very weak to very strong multi-decadal to multi-centennial AMOC variability. We will compare our model results with temperature reconstructions for the past 2 millennia derived with different climate field reconstruction (CFR) methods (Neukom et al., 2019) and a subset of the CMIP5 last millennium simulations (Braconnot et al., 2012; Taylor et al., 2012). We will focus on two different spatial scales to investigate the inter-regional temperature coherency, namely inter-continental and between ocean and land. This will allow us to investigate the role of ocean-induced climate variability in altering spatial temperature variability coherency and to determine which level of ocean variability yields model results that are in best agreement with proxy-based temperature reconstructions.
We limit our analysis of reconstructed temperatures for the past 2 millennia to the data set published by Neukom et al. (2019), but many others exist (e.g. Ljungqvist et al., 2019; Zhang et al., 2018; Wang et al., 2017; Moreno-Chamarro et al., 2017; Franke et al., 2016; Luterbacher et al., 2016). All these temperature reconstructions are affected by, among others, the spatial distribution of the underlying records, their temporal extent, seasonality effects and the climate response of the various proxy types (Anchukaitis and Smerdon, 2022). Given the goals of our study as outlined above, the temperature reconstructions of Neukom et al. (2019) are the most suited as they cover sufficiently large spatial scales and include an estimate of the methodological uncertainties.
The work presented here is based on a perturbed-parameter ensemble of the iLOVECLIM Earth system model, the PAGES-2k temperature reconstructions (Neukom et al., 2019) and a selected number of CMIP5 last millennium simulations.
2.1 The iLOVECLIM perturbed-parameter ensemble
Here, iLOVECLIM (here in version 1.1) is a code fork of the LOVECLIM 1.2 model (Goosse et al., 2010). It consists of a free surface-ocean general circulation model with an approximately 3∘ spatial resolution and 20 vertical layers. It is coupled to a thermodynamical sea ice model and a quasi-geostrophic model atmospheric model solved on a T21 spectral grid.
We performed a 70-member perturbed-parameter ensemble of pre-industrial control simulations with the iLOVECLIM model. From this ensemble, we selected nine parameter sets that yield results that are both reasonable in comparison with present-day observations (not shown) and cover a large range of magnitudes in multi-decadal to multi-centennial AMOC-related ocean variability. These nine parameter sets include our default parameter set (experiment 1). Table A1 lists the values that are used for the 10 perturbed parameters. Parameter selection was done using a Latin hypercube sampling (LHS). The ranges that are used in the LHS are given in Table A2. The choice of parameters to perturb is based on previous research by Loutre et al. (2011) and Shi et al. (2019) and personal experience. Note that for some of the experiments (2–5), a limited number of parameters was excluded from the LHS, and we instead imposed parameter changes based on our knowledge of the relation between those specific parameters and changes in the AMOC behaviour in the model. This is specifically the case for the parameters controlling the size of the imposed precipitation correction between the Atlantic and the Pacific (Tables A1 and A2).
We assessed the degree of agreement with present-day observations for a selection of variables, namely the AMOC strength at 26∘ N (Moat et al., 2020), the Northern Hemisphere (NH) and Southern Hemisphere (SH) sea-ice extent (Niederdrenk and Notz, 2018; Roche et al., 2012), the top-of-the-atmosphere radiative imbalance (Schmidt et al., 2017), and the global mean temperature (Rohde and Hausfather, 2020). Even though all ensemble members, including the default parameter set, show biases with respect to observations, no member of the nine-member ensemble can clearly be discarded as unrealistic, and we deem the perturbed-parameter ensemble suited to investigate the role of AMOC variability on spatio-temporal temperature variability.
Using these nine parameter sets and starting from long pre-industrial control simulations, we performed nine corresponding 2000-year-long experiments covering the past 2 millennia forced with time-varying volcanic and solar forcings, changes in greenhouse gas concentrations and changes in the orbital parameters. We limit our analysis to the period before 1850 in order to exclude the increasingly strong anthropogenic warming signal over the last 150 years. All other boundary conditions are pre-industrial (Goosse et al., 2010).
2.2 PAGES-2k temperature reconstructions
Using a selection of 210 local temperature-sensitive proxies from the PAGES-2k database (Ahmed et al., 2013), Neukom et al. (2019) present six different climate field reconstruction (CFR) methodologies to extend the point data to a full global coverage. In our current study we will use these six different temperature field reconstructions to investigate the robustness of reconstructed temperature variability and spatial covariance and to compare with model results. The CFR methods deployed by Neukom et al. (2019) range from basic proxy composites to advanced statistical techniques that combine the Ahmed et al. (2013) proxy data set with physical constraints and forcing information from climate–model simulations.
Here we will provide a short summary of the six different CFR methods of Neukom et al. (2019) because of their importance for our investigation (further details can be found in the original publication): (1) composite plus scale (CPS) is an index reconstruction method in which the input proxy data are averaged into composite time series, which are in turn scaled to the mean and standard deviation of the reconstruction target over the calibration period. (2) Principal component regression (PCR) reduces the dimensions of both the target field and the proxy data using principal component analysis. In this approach the covariance structure of the temperature grid is based on the instrumental record and assumed to be constant for the whole reconstruction period. (3) Canonical correlation analysis (CCA) uses singular-value decomposition to separately reduce the dimensions of the instrumental temperatures, the proxy data and the regression coefficient matrix that describes their relationships. The main assumption is that the first few leading modes of the empirical orthogonal function contain most of the variance in the target climate field and the multi-proxy network. (4) GraphEM uses the theory of Gaussian graphical models to reduce the dimensionality of the problem. (5) Data assimilation (DA) optimally combines proxy data with climate model states. Here offline data assimilation is used. The climate model provides an estimate of the prior that is updated on the basis of the proxy observations and an estimate of the errors in both the observations and the prior. (6) The analogue method (AM) is a method that requires a pool of plausible climate fields for which simulations from the PMIP3 project are used in this case. In this method the spatial structure of temperature is provided by the different climate models, while the temporal evolution is obtained from the information contained in the proxy data. Generally one can say that three out of six CFRs use observational information to obtain information on the spatial correlation structure (PCR, CCA, GraphEM), two methods base their spatial correlation structure on climate model output (DA and AM) and the sixth method does not use any form of additional spatio-temporal information (CPS).
Following the recommendation by Neukom et al. (2019), we also include the multi-method mean in our analysis. All the CFR-based temperature reconstructions include an uncertainty estimate using a 100-member ensemble. In parts of our analysis we use the ensemble mean, while in other parts the uncertainty is explicitly taken into account. For comparison, we also include the original continental-scale temperature time series from Ahmed et al. (2013), which we will refer to as PAGES2013 data.
By employing a single data set (Ahmed et al., 2013) of 210 local temperature-sensitive proxies in six different CFR methods, the data set of Neukom et al. (2019) allows for a good description of the uncertainties caused by the CFR methods. However, other sources of uncertainties are not (directly) sampled (e.g. spatial distribution, temporal extent, seasonality effects and climate response Anchukaitis and Smerdon, 2022). It is, for instance, important to remember that the spatial distribution is strongly biased towards the mid-latitude of the NH and that the maximum number of 210 records quickly decreases to values below 30 prior to the year 800 CE (Anchukaitis and Smerdon, 2022). The CFR methods that are used to extend the spatially and temporally limited point data to a fully global coverage for the past 2000 years thus become increasingly important going further back in time.
2.3 CMIP5 last millennium simulations
For further comparison we also include results from three randomly selected single-member CMIP5 last millennium simulations (MRI-CGCM3, GISS-E2-R and MIROC5) and the 13 members of the last millennium ensemble with CESM (Otto-Bliesner et al., 2016). Including these CMIP5 simulations allows us to put the results of the iLOVECLIM perturbed-parameter ensemble and the PAGES-2k reconstructions in perspective.
2.4 Observational data sets
Three out of six CFR methods use the observational temperature data set HadCRUT4-GraphEM, a data set that is based on HadCRUT4 (Morice et al., 2012) but that was infilled using the GraphEM method to obtain a complete global coverage over the calibration period over the period 1850–2000 with a resolution of (Neukom et al., 2019). For further comparison of our results with observations, we used the ERA5 observational data set (Copernicus Climate Change Service, 2017), covering the period 1979 to 2019. To remove the anthropogenic global warming signal, the time series are detrended using a second-order polynomial fit. Note that the obtained results are not sensitive to the exact definition of the observational period.
2.5 Data processing
On all temperature time series presented here, a Butterworth filter was applied that effectively removes all variability on timescales smaller than 50 years. We tested the impact on our results of the window size of the Butterworth filter and found that our findings are robust at least within a range of 20–100 years (not shown). Leads and lags at multi-decadal timescales are expected between the response of temperatures at a given location and either temperatures at another location or with the AMOC. We investigate the importance of lead–lag relationships for the resulting correlation factors by allowing leads and lags of a maximum of 100 years and thus finding the highest possible correlation. These results will be referred to as “lagged” in the remainder of the paper, while “non-lagged” refers to a default lag of zero years. This calculation is generally done per continental-scale region, except in Fig. 3 where it is done for all grid cells. Our definition of the continental-scale regions is shown in Fig. A1.
The iLOVECLIM perturbed-parameter ensemble of past 2 millennia simulations allows us to investigate the effect of the amount of ocean-driven internal climate variability on both continental-scale temperature variability and spatial temperature covariance. In the following the results for these two aspects will be presented together with a comparison with the results for CMIP5 last millennium simulations, PAGES-2k temperature reconstructions and observational data sets.
3.1 Temperature variability
The iLOVECLIM ensemble shows a wide range of temperature evolutions for the eight continental-scale regions (Fig. 1). Substantial differences between the ensemble members are simulated for North America, the Arctic, Asia and Europe. For those regions, the amount of variability varies up to a factor of 3 over the ensemble, showing the large impact of AMOC variability on continental-scale temperature variability in the NH. For South America, the Antarctic, Africa and Australasia, the amount of temperature variability is largely unchanged.
Overall, the amount of continental-scale temperature variability in the iLOVECLIM ensemble and the range found over all ensemble members compares favourably with the results of the selected CMIP5 large millennium simulations (Fig. 1). This is especially true for Antarctica, North America, Asia and Europe. For some regions, iLOVECLIM underestimates variability (South America, Australasia and to a lesser extent Africa), while for the Arctic iLOVECLIM overestimates variability.
When comparing the simulated results with the different CFR-based reconstructions of continental-scale temperature variability (including the original PAGES2013 reconstructions; Fig. 1), a complex picture emerges. The range of variability in both the iLOVECLIM and CMIP5 model results is in agreement with the reconstructions for some continental-scale regions (Antarctica, South America, North America, Asia and to some degree also Europe and Africa), while in others either the iLOVECLIM (Australasia) or the CMIP5 (Arctic) are in better agreement.
The importance of the AMOC changes in driving temperatures as simulated with iLOVECLIM differs largely per continental-scale region. We find that for Antarctic, South America and Australasia, the correlation between continental-scale temperature time series and AMOC time series is low to modest, ranging from 0.1 to 0.5 over the ensemble (Fig. 2). For the other regions the temperature–AMOC correlation is higher and ranges from 0.5 up to 0.9. Moreover, it seems that for all continental-scale regions, ensemble members with little AMOC variability (Fig. 3) tend to have smaller temperature–AMOC correlations, and those with higher AMOC variability tend to show higher correlations. However, the relationship is far from straightforward, and this will become more evident in the following section when we look at the corresponding spatial temperature covariance structure.
3.2 Spatial temperature covariance
Inter-continental temperature correlations
The amount and characteristics of AMOC variability in a simulation not only impacts temperature variability on a site-by-site basis but also strongly shapes the spatial temperature covariance structure. The different AMOC time series (Fig. 3) show multi-decadal to multi-centennial AMOC variability in all simulations. However, the magnitude ranges from under 3 Sv in experiment 1 to up to 10 Sv in experiment 7. Moreover, these results show that both the amplitude of the AMOC variations important and the dominant frequency are important. For instance, in ensemble members 3 and 6, we find strong but short-lived variations in the AMOC that only correlate with temperature variations in the northern North Atlantic. In contrast, longer-lived AMOC variations as found in, for instance, ensemble members 2, 4 and 7, impact temperatures throughout the Northern Hemisphere. An in-depth discussion on the underlying mechanisms is not within the scope of this paper, but various AMOC modes have been described previously for the iLOVECLIM model (e.g. Friedrich et al., 2010; Goosse and Renssen, 2004; Kessler et al., 2020; Kim et al., 2021).
Because of the differences in the temperature fingerprint of the AMOC variations between the ensemble members, we also find differences in the way inter-continental temperature correlations are affected. For a total of 7 out of all 28 possible temperature correlations between our continental regions, we find a significant (p<0.05) relationship with the amount of AMOC variability (Fig. 4), encompassing combinations of all continental-scale regions except Antarctica and South America. We note that there can be two different reasons for a non-significant relationship between AMOC variability and a given inter-continental temperature correlation, namely because both continents are not sufficiently affected by AMOC variability or because both continents are always strongly correlated to AMOC variability, regardless of whether this AMOC variability is strong or weak. We further note that all significant relationships are positive relationships, meaning that an increase in AMOC variability leads to a higher degree of spatial coherency between continental-scale regions. Given that the impact of AMOC variability is mostly limited to the Northern Hemisphere (Fig. 3), one could expect inter-continental temperature correlations between continents on both hemispheres to decrease with stronger AMOC variability (a negative slope in Fig. 4); however, we do not find any such relationships (neither significant nor non-significant).
Combining all inter-continental relationships creates an overview of the degree to which the temperature evolutions for the different continental-scale regions are related to one another (Fig. 5, constructed following the approach of PAGES 2k-PMIP3 group, 2015). Overall we find that the characteristics of AMOC-induced temperature variability impacts the inter-continental temperature covariance structure. We use two members of the full iLOVECLIM perturbed-parameter ensemble to illustrate the range of possible solutions, while the results for all nine members of the iLOVECLIM ensemble can be found in Fig. A2. Examples of clear changes in intercontinental correlations are between the Arctic and Africa, Africa and Europe, and Asia and North America. For some other regions, the correlations remain mostly low (Antarctic, South America and Australasia), while between other regions the correlations are always relatively high (North America with Europe; North America with the Arctic; and between Europe, Africa, and Asia). Whether or not we optimize the correlations by considering possible lead–lag relationships does not lead to large changes (compare Figs. A2 and A3). The four CMIP5 last millennium simulations that are used for comparison in our analysis highlight that for different climate models the strength of the inter-continental temperature correlations also ranges from low overall (MRI-CGCM3) to high overall (MIROC-ESM). Taking the CMIP5 simulations into consideration it appears that the inter-continental temperature correlations that are always low or relatively high over the iLOVECLIM ensemble are not a robust feature of climate models in general.
The inter-continental temperature correlations based on the temperature reconstructions yields widely varying results for the different CFR methods (Fig. 6), a range that is not unlike the results obtained for the climate models. The CFR methods that use climate model input to generate the field reconstructions (see method section) generally show high inter-continental temperature correlations (AM and DA), while the CFR methods that use observational constraints to generate field reconstructions show relatively low inter-continental temperature correlations (CCA, PCR and GraphEM). The CFR method that is used to extend the point data to a full global coverage thus has a large impact on the resulting spatio-temporal temperature covariance structure. Not applying a CFR method but using the original PAGES2013 temperature time series for the different continental-scale regions (Fig. 6) results in lower correlations than those found in the results based on any model or CFR.
The CFRs include an estimate of the uncertainty by means of an 100-member ensemble (Neukom et al., 2019). We find that the inter-continental correlations are impacted by how we take this uncertainty into account. We show this by comparing two different ways to compute the multi-method-mean (Fig. 6). One can either calculate the inter-continental correlation for every individual ensemble member before calculating the ensemble mean inter-continental correlations (Fig. 6) or calculate the ensemble mean temperature time series per grid cell and based on that calculate the inter-continental correlations (Fig. A4). In the latter approach one averages out some variability before calculating the inter-continental correlations, leading to overall higher multi-method mean results.
The low inter-continental correlations between the original PAGES2013 temperature time series possibly result from the subsampling of a small number of sites per continental-scale region. We test this using the iLOVECLIM ensemble by randomly picking a small number of sites per region and calculate the correlations based on that. We find that depending on the sites that are randomly picked, the inter-continental correlations are at best similar to those based on the full-region data but can also be much lower (Fig. A5). The lower-end results for some perturbed-parameter ensemble members approach the original PAGES2013-based inter-continental correlations (Fig. 6).
Land–sea contrast in temperature variability
Another way to compare reconstructed and simulated spatio-temporal temperature correlations is using the differences in temperature variability between land and ocean at a given latitude. Before studying simulated and reconstructed long-term (>50 years) land–sea temperature variability ratios over the past 2 millennia, we first investigate how well climate models and the PAGES-based CFR compare with observational data sets for the period 1850–2000 (Fig. 7). Note that in contrast with all other analyses presented in this paper, for this comparison with more recent observations the time series are too short to use 50-year smoothed data, and instead we use annual mean temperature time series. However, the anthropogenic global warming signal is removed by detrending the time series using a second-order polynomial fit. The iLOVECLIM ensemble shows land–sea temperature variability ratios close to 1 for nearly all latitudes. The exceptions are the high latitudes in both hemispheres at which ocean temperature variability dominates and the NH mid-latitudes where continental temperature variability is larger. The spread over the iLOVECLIM perturbed-parameter ensemble is relatively small. For the mid-to-high latitudes of both hemispheres the CMIP5 simulations and the iLOVECLIM are in reasonable agreement; however, for the latitudes roughly between 40 and 10∘ in both hemispheres, the CMIP5 simulations suggest much more temperature variability over land than over the oceans, with values up to a ratio of 2 to 3. The two observational data sets that we show here for validation, ERA5 and HadCrut4_GraphEM, generally show land–sea temperature variability ratios close to unity. This is not unlike the iLOVECLIM ensemble, but quite different from the CMIP5 results for the latitudes between 40 and 10∘. MIROC-ESM differs from the other models and the observational data sets, with land–sea temperature variability ratio values of around 2 in the low latitudes. It is notable that both observational data sets are also rather different in many places. One possible cause of these differences could be the fact that both observational products cover a different period in time (1850–2000 versus 1979–2019). However, we find that this has only a minor impact (Fig. A6). The cause for the differences should thus be sought in underlying methodological differences of both observational products.
The PAGES-2k CFR methods also show many latitudes with land–sea temperature variability ratios close to unity (Fig. 7), in line with the observations and the iLOVECLIM ensemble. However, there is a substantial spread amongst the different CFR methods and there is a large bias in the latitude band from 30 to 70∘ N in which the CFR methods show substantially more temperature variability over the continents than over the oceans. Even though both models and most CFR methods are constructed using observational information, this validation shows that this does not guarantee a good agreement for higher-order metrics like land–sea temperature variability ratios.
Now we turn again to variability on longer, multi-decadal to multi-centennial, timescales (Fig. 8). The iLOVECLIM ensemble shows results for the past 2000 years that are largely comparable with the observational period, except for much smaller land–sea temperature variability ratios for the mid-to-high latitudes of the NH. In that region, the model simulates a large impact of the amount of AMOC variability, resulting in ratios that range between 50 % more ocean variability than land variability and up to 250 % more ocean variability. The different CMIP5 last millennium simulations are overall in good agreement with each other, and they show results that are in line with CMIP5 results for the observational period. The main difference being, in line with the iLOVECLIM ensemble, smaller ratios for the high latitudes of both hemispheres, indicating increased ocean temperature variability relative to land variability on these timescales.
The PAGES CFR-based land–sea temperature variability ratios for the past 2 millennia are again largely comparable with the CFR-based results for the observational period. The main difference is higher ratios in the DA method for the mid-latitudes of the SH and higher ratios in both the DA-method and the GraphEM method for the mid-latitudes of the NH, meaning that in both cases land temperature variability has increased relative to ocean variability. Comparing Figs. A7 and A9, it appears that the PAGES CFR-based land–sea temperature variability ratios for the past 2 millennia are biased high for the mid-latitudes of the NH because they underestimate temperature variability over the mid-latitude oceans.
Because of the similarities for all data sets between the results for the observational period and the past 2 millennia, we still face a large discrepancy between the different model results, between models and the reconstructions, and between the different reconstruction-based CFR methods (Fig. 8). The main differences are ratios larger than unity for the CMIP5 models at all latitudes equatorward of 40∘, where the iLOVECLIM ensemble and the PAGES-2k results suggest values close to unity, except for values smaller than one in the reconstruction close to the Equator. For the mid-to-high latitudes of the SH the models agree quite well with each other, with more variability in the ocean than over land, while the reconstructed ratios are close to unity. The main discrepancy is found in the mid-latitudes of the NH. There the iLOVECLIM ensemble shows much more variability in the ocean (which increases with stronger AMOC variability), the CMIP5 results suggest land–sea temperature variability ratios close to or just below unity, and the CFR-based results show much stronger variability over the continents than over the oceans.
It is important to note that these land–sea temperature variability ratios only give information on relative differences between temperature variability over land and oceans. If we look at the individual terms, we see, for instance, that the iLOVECLIM ensemble simulates more variability over both the continents and the ocean for the mid-to-high latitudes of the NH compared to the CMIP5 simulations (Fig. A7). On the other hand, the iLOVECLIM ensemble simulates too little variability over both the tropical oceans and continents (Fig. A7), leading to land–sea temperature variability ratios in the tropics that are very comparable to those simulated by the CMIP5 models (close to unity) but for the wrong reasons. The lack of tropical climate variability in iLOVECLIM is a known bias in the model (Goosse et al., 2010).
We have presented a perturbed-parameter ensemble of the iLOVECLIM Earth system model that is designed in order to have a large spread in simulated AMOC behaviour in terms of magnitude and frequency of centennial AMOC fluctuations. Combined with the PAGES-2k temperature reconstructions (Neukom et al., 2019) and a selected number of CMIP5 last millennium simulations, this allows us to discuss the potential importance of AMOC variability in driving centennial-scale temporal and spatio-temporal temperature variability over the past 2 millennia.
In the iLOVECLIM ensemble, the AMOC plays an important role in driving centennial temporal temperature variability; however, the spatial extent of this impact differs strongly, from a regional northern North Atlantic impact to a hemisphere-wide impact. Previous work has also shown climate models in which the AMOC is an important driver of centennial climate variability (e.g. Knight et al., 2005).
Previous studies looking at temperature variability in the time domain have suggested that climate models simulate too little variability on multi-decadal and longer timescales compared to proxy-based reconstructions (Laepple and Huybers, 2014; PAGES 2k-PMIP3 group, 2015). Comparing the iLOVECLIM ensemble and CMIP5 simulations for the past 2 millennia with the PAGES-2k continental-scale temperature reconstructions, we do not find such a model–data mismatch on the multi-decadal to multi-centennial timescales. Given the spread in both reconstructed and simulated continental-scale temperature variability, we find that model and data results either overlap or that the models suggest slightly more variability. From our results, and given the large uncertainty in reconstructed continental-scale temperature variability, it is not clear if increased AMOC variability would lead to a better model–data comparison in terms of continental-scale temporal temperature variability.
Increasing the strength of internal modes of climate variability like those related to the AMOC, not only increases temperature variability at a given site but can also change the temperature correlations between different continental-scale regions. We find that for 7 out of the total of 28 possible inter-continental temperature correlations there is a positive correlation with the magnitude of AMOC variability. None of the inter-continental temperature correlations show a significantly negative correlation with the magnitude of AMOC variability. This happens regardless of whether we correct for possible lead–lag relationships within the system. This implies that, in line with previous suggestions (PAGES 2k-PMIP3 group, 2015), enhanced internal climate variability, in our case driven by the AMOC, leads to an enhancement in the spatio-temporal temperature covariance by increasing the strength of climatic teleconnections between regions. Previous studies have suggested that models simulate too high inter-continental temperature correlations (PAGES 2k-PMIP3 group, 2015), and our results suggest that enhanced AMOC-related climate variability will not resolve such a model–data discrepancy. Mechanisms of centennial climate variability that have a more local impact could possibly lead to a decrease in the simulated spatio-temporal temperature covariance structure or a mixture of various large-scale modes of variability. However, comparing the inter-continental temperature correlations based on the iLOVECLIM ensemble, the CMIP5 models, the different CFRs and the original PAGES2013 reconstructions, we conclude that the spread in the results based on both models and reconstructions is so large that we cannot confirm the previously suggested model–data mismatch in terms of inter-continental temperature correlations.
Our comparison of reconstructed and simulated land–sea ratios in terms of temperature variability revealed large differences: between the iLOVECLIM results and the CMIP5 results, between the various CMIP5 simulations, and between the CFRs. As a result, we conclude that available temperature reconstructions of the past 2 millennia are very uncertain and do currently not provide constraints on model results. Part of the reason why the reconstructed land–sea ratios are so uncertain is possibly because they are based on continental temperature proxies and not directly on sea surface temperature (SST) proxies. As a result, the CFR methods play a large role extrapolating continental atmospheric temperature onto neighbouring ocean regions. Acknowledging that the temperature reconstructions reflect atmospheric temperatures over the ocean rather than SSTs did improve the model–data comparison in our analysis, but large biases remain (Figs. A7 and A8). One can also compare the simulated SSTs and the CFR-based “ocean temperatures” with a data set of actual SST reconstructions over the past 2 millennia (McGregor et al., 2015). However, we find that the amount of reconstructed local SST variability (McGregor et al., 2015) is roughly an order of magnitude larger than the variability in iLOVECLIM, CMIP5 or the CFR-based temperature estimates (Figs. A10 and A11). Note that the SST reconstructions are a collection of individual records (not a CFR), so this comparison is done on a site-by-site basis. In fact, compared to the large discrepancy with the SST reconstructions, the iLOVECLIM and the CFR-based temperature estimates are in much better agreement with each other (Fig. A12). The mismatch we find with the SST reconstructions of McGregor et al. (2015) seems relevant because some previous indications of model–data mismatches in terms of long-term temperature variability were based on similar SST reconstructions (Laepple and Huybers, 2014). More in-depth studies are need to understand and resolve, on the one hand, the differences between reconstructed point-based temperature variability and, on the other hand, temperature variability in coarse-resolution products (2–5∘ in this study), like model results and CFR-based reconstructions. Our findings suggest that increasing AMOC-related climate variability does not significantly improve the model–data comparison of multi-decadal to multi-centennial local ocean temperature variability.
CFR-based reconstructions are in reasonable agreement with each other for first-order variables like continental-scale temperature time series and variability. However, for higher-order metrics like inter-continental temperature correlations or land–sea contrast, the differences between the various CFR methods is substantially increased. The uncertainty in these CFR-based higher-order metrics is even larger when taking into account the uncertainty within the individual CFR methods given by the 100 ensemble members (compare, for instance, the inter-continental temperature correlations in Figs. A3 and 6). Neukom et al. (2019) suggest using only the multi-method mean over the six CFR methods, but by doing so it would remain unclear how large the uncertainty of the resulting spatio-temporal temperature reconstructions is, hampering the model–data comparison.
Despite the fact that over 500 reconstructed temperature time series cover the past 2 millennia with relatively small age uncertainties (Ahmed et al., 2013; PAGES 2k-PMIP3 group, 2015), uncertainties in the resulting CFRs remain relatively large. This, in combination with the relatively small magnitude multi-decadal to multi-centennial temperature variations on the continental scale (for most regions the standard deviation is below 0.2 K), leads to unfavourable signal-to-noise ratios and continuing difficulty to constrain climate model simulations using temperature reconstructions of the past 2 millennia.
AMOC variability is often thought to be a prominent player in driving multi-decadal to multi-centennial climate change. Indeed, our iLOVECLIM perturbed-parameter ensemble shows a large impact of AMOC variability on both continental-scale temperature variability and the spatio-temporal temperature correlations between the various continents. However, comparing the iLOVECLIM results with the PAGES-2k continental-scale temperature reconstructions and a selection of CMIP5 last millennium simulations, reveals that uncertainties in both model results and temperature reconstructions hamper our ability to determine the importance of AMOC variability for the climatic evolution over the past 2 millennia from such large-scale diagnostics as the one applied here. It thus remains unclear which magnitude of AMOC variability would lead to a better agreement between simulated and reconstructed temperatures for the past 2 millennia.
The iLOVECLIM source code is based on the LOVECLIM model version 1.2, whose code is accessible at http://www.elic.ucl.ac.be/modx/elic/index.php?id=289 (last access: 22 November 2022, UCL, 2022). The developments on the iLOVECLIM source code are hosted at https://forge.ipsl.jussieu.fr/ludus (last access: 22 November 2022, IPSL, 2022) but are not publicly available due to copyright restrictions. Access can be granted on demand by request to Didier M. Roche (firstname.lastname@example.org) to those who conduct research in collaboration with the iLOVECLIM user group. The iLOVECLIM perturbed physics ensemble climate model output is available through the ZENODO repository under the following DOI: https://doi.org/10.5281/zenodo.6675429 (Bakker, 2022).
PB designed the study and performed the climate model experiments. PB, HG and DMR analysed the results and wrote the manuscript.
The contact author has declared that none of the authors has any competing interests.
Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
We thank the two anonymous reviewers for their insightful comments. We acknowledge the Institut Pierre Simon Laplace for hosting the iLOVECLIM model code under the LUDUS framework project (https://forge.ipsl.jussieu.fr/ludus).
This paper was edited by Jürg Luterbacher and reviewed by two anonymous referees.
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