Global mean temperature change simulated by climate models deviates from the observed temperature increase during decadal-scale periods in the past. In particular, warming during the ‘global warming hiatus’ in the early twenty-first century appears overestimated in CMIP5 and CMIP6 multi-model means. We examine the role of equatorial Pacific variability in these divergences since 1950 by comparing 18 studies that quantify the Pacific contribution to the ‘hiatus’ and earlier periods and by investigating the reasons for differing results. During the ‘global warming hiatus’ from 1992 to 2012, the estimated contributions differ by a factor of five, with multiple linear regression approaches generally indicating a smaller contribution of Pacific variability to global temperature than climate model experiments where the simulated tropical Pacific sea surface temperature (SST) or wind stress anomalies are nudged towards observations. These so-called pacemaker experiments suggest that the ‘hiatus’ is fully explained and possibly over-explained by Pacific variability. Most of the spread across the studies can be attributed to two factors: neglecting the forced signal in tropical Pacific SST, which is often the case in multiple regression studies but not in pacemaker experiments, underestimates the Pacific contribution to global temperature change by a factor of two during the ‘hiatus’; the sensitivity with which the global temperature responds to Pacific variability varies by a factor of two between models on a decadal time scale, questioning the robustness of single model pacemaker experiments. Once we have accounted for these factors, the CMIP5 mean warming adjusted for Pacific variability reproduces the observed annual global mean temperature closely, with a correlation coefficient of 0.985 from 1950 to 2018. The CMIP6 ensemble performs less favourably but improves if the models with the highest transient climate response are omitted from the ensemble mean.
The overall modelled global temperature increase of the past seven decades agrees well with what has been observed (Fig. 1a), but differences occurred on decadal to multidecadal time scales (Dai et al. 2015; Meehl et al. 2016). While the climate models participating in the Coupled Model Intercomparison Project phase 5 (CMIP5; Taylor et al. 2012) and phase 6 (CMIP6; Eyring et al. 2016) capture the observed global mean surface temperature (GMST) trend from the 1940s/early 1950s to the mid-1970s reasonably well (Folland et al. 2018; Papalexiou et al. 2020), they tend to overestimate the warming from the mid-1970s to present-day (Tokarska et al. 2020). On shorter time scales, further differences become apparent (Fig. 1b). Whereas Earth appeared to warm faster than simulated by models from the 1970s to the 1990s, models overestimate the GMST increase during the so-called ‘global warming hiatus’ from the 1990s to the early twenty-first century (Medhaug et al. 2017). On decadal to multidecadal time scales, episodes of differences in the rate of modelled and observed global temperature change are related mostly to internal climate variability (Dai et al. 2015; Kosaka and Xie 2016), uncertainty in radiative forcing (Haustein et al. 2019; Marotzke and Forster 2015), and observational uncertainty (Karl et al. 2015).
The ‘global warming hiatus’, the most recent period of divergence between observed and modelled global warming, has been examined extensively and is explained by a combination of factors: under-representation of the fastest warming regions in the observational record (Cowtan and Way 2014); a biased comparison between observations and models, where sea surface temperature (SST) was assumed to warm at the same rate as marine air temperature (Cowtan et al. 2015); uncorrected biases in SST datasets related to changes in measurement instruments over time (Hausfather et al. 2017; Karl et al. 2015); mismatches in the radiative forcing, caused mainly by solar variability and omitted small volcanic eruptions (e.g., Folland et al. 2018; Huber and Knutti 2014; Ridley et al. 2014; Schmidt et al. 2018; Schmidt et al. 2014); and internal variability in the climate system (e.g., England et al. 2014; Kosaka and Xie 2013) causing the excess heat to be transported more efficiently away from the atmosphere to the deeper ocean (e.g., Meehl et al. 2011; Watanabe et al. 2013). Modelled warming during recent decades might also be too large if models overestimate the transient climate response (TCR) (Jiménez-de-la-Cuesta and Mauritsen 2019), but Huber and Knutti (2014) and Santer et al. (2017) found little evidence for a biased response of the CMIP5 ensemble to external forcing. Climate sensitivity has, however, increased from CMIP5 to CMIP6 (Meehl et al. 2020; Zelinka et al. 2020) and the CMIP6 ensemble shows greater warming than CMIP5 since the 1970s, which increases the discrepancy with observed warming during the ‘global warming hiatus’ (Fig. 1).
Internal variability in the Pacific is believed to have played a key role in decadal-scale differences between observed and modelled warming, and numerous studies quantified its contribution to the ‘global warming hiatus’ and earlier episodes. During the ‘hiatus’ period, Pacific trade winds strengthened, thereby intensified the Pacific shallow ocean overturning cells and increased upwelling of cooler waters in the central and eastern Pacific (England et al. 2014; Maher et al. 2018). This lowered the SSTs in the eastern Pacific and led to increased heat uptake into the subsurface western Pacific Ocean (England et al. 2014). Part of the heat has been transported by an enhanced Indonesian throughflow from the Pacific into the subsurface Indian Ocean, leading to a warming of the Indian Ocean (Lee et al. 2015). These processes reduced the pace of global warming during the ‘hiatus’ period relative to the ensemble mean of climate model simulations where internal variability is averaged out (Kosaka and Xie 2013).
Here, we aim to reconcile differing conclusions on the importance of Pacific variability during periods of accelerated and reduced rates of warming. While a consensus emerged that Pacific variability has contributed to the ‘global warming hiatus’ (Medhaug et al. 2017), estimates of how much differ greatly, and range from fully explaining it (e.g., Kosaka and Xie 2016; Peyser et al. 2016), to most of it (Swingedouw et al. 2017), around half (Huber and Knutti 2014), around a fourth (Meehl et al. 2016), to even less than that (Chylek et al. 2016; Tung and Chen 2018).
After having introduced the data and methods in Sect. 2, we review different approaches of quantifying the influence of Pacific variability on the global mean temperature in Sect. 3. In Sect. 4 we quantitatively compare the estimated Pacific contribution to global mean temperature during the past seven decades, but with a focus on the ‘global warming hiatus’, from 18 studies and examine which factors led to differing conclusions on the importance of Pacific variability. We demonstrate that the difference between observed and modelled warming is dominated by Pacific variability. Adjusting the multi-model ensemble means for the effect of Pacific variability therefore allows us to uncover biases in the simulated global mean forced response unrelated to Pacific variability. Whereas the variability-adjusted CMIP5 multi-model mean closely resembles observed warming, the CMIP6 ensemble mean appears to overestimate warming during recent decades.
Data and methods
We focus on global mean surface temperature (GMST hereafter) as one of the key metrics of global climate change, but note that it is an incomplete measure of the warming of the globe since most of the heat is stored in the oceans. The underlying assumptions throughout the paper are that the forced signal and internal variability are independent and approximately add up linearly. Under strong forcing, these assumptions may break down (Brown et al. 2017; Olonscheck and Notz 2017).
We restrict our analysis to the period from 1950 to 2018 as the tropical Pacific SSTs were only poorly sampled prior to that (Deser et al. 2010) and to avoid large SST biases during the World War II period and prior (Chan et al. 2019; Cowtan et al. 2018; Thompson et al. 2008). Nonetheless, the examined period covers most of the human-made climate change, as around three-quarters of the overall anthropogenic global warming took place after 1950 (Haustein et al. 2017).
Further, we limit the analysis to annual mean (January–December) and global mean values. Explaining differences between observed and simulated annual mean GMST does not guarantee that the individual seasons are explained as well (Deser et al. 2017; Douville et al. 2015) nor that the simulated temperature pattern agrees fully with the observed pattern (Deser et al. 2017; Xu et al. 2020).
To quantify GMST changes, we use two spatially interpolated datasets, CW19 and GISTEMPv14. CW19 is an updated version of the Cowtan and Way (2014) dataset, which combines CRUTEM4.6 (Jones et al. 2012) over land with HadSST4 (Kennedy et al. 2019) over the ocean and infills regions of missing observations by kriging. The initially published Cowtan and Way (2014) dataset used HadSST3, and to differentiate the two versions we refer to it as CW19 in the following. GISTEMPv4 (Hansen et al. 2010; Lenssen et al. 2019) represents SSTs by ERSSTv5 (Huang et al. 2017a) and land air temperatures are based on NOAA GHCNv4 (Menne et al. 2018). GISTEMPv4 extrapolates temperature anomalies between stations which are up to 1200 km apart and thereby achieves nearly complete spatial coverage after 1950. Because measurement coverage since 1950 is relatively high, statistical infilling is able to alleviate biases in global warming arising from poor coverage (Benestad et al. 2019), such as underestimated warming during the ‘global warming hiatus’ (Cowtan and Way 2014; Huang et al. 2017b). We compare GISTEMPv4 and CW19 with other spatially interpolated GMST datasets in the supporting information (Fig. S1). While there are some differences between the datasets, our results do not depend strongly on the choice of GMST dataset.
To characterize Pacific variability, we use indices based on tropical SST and wind stress. We calculate indices of oceanic variability from two SST datasets, COBE-SST2 (Hirahara et al. 2014) and ERSSTv5. Both datasets are spatially interpolated. Among other SST datasets, ERSSTv5 and COBE-SST2 are most consistent with independent ocean profile data used for evaluating the datasets after 1950 (Huang et al. 2018), and are not affected by a cooling bias in recent years seen in other SST datasets (Hausfather et al. 2017). We represent the El Niño-Southern Oscillation (ENSO) by the observed monthly-mean equatorial Pacific SSTs in the Nino3.4 region (5° S–5 °N, 170°–120° W; Trenberth 1997). The simulated ENSO variability might be spatially displaced compared to the observed variability, and therefore we also use a larger region in the tropical, central to eastern Pacific, typical of what has been used in tropical Pacific pacemaker experiments (15° N–15° S, 180°–90° W; hereafter the pacemaker region).
We quantify tropical Pacific zonal mean eastward wind stress variability using four modern reanalyses, ERA5 (Hersbach and Dee 2016; covering the period 1979–2018), JRA-55 (Kobayashi et al. 2015; 1958–2018), MERRA2 (Gelaro et al. 2017; 1980–2018), and the NOAA-CIRES 20th Century Reanalysis (20CR) v2c (Compo et al. 2011; 1851–2014). ERA5, JRA-55 and MERRA2 assimilate different observation types and variables whereas 20CR only assimilates surface pressure observations and may, therefore, be less susceptible to changes in the observational system, but is also less tightly constrained by observations. For calculating the zonal mean wind stress variability, we use 180°–150° W and 6° S–6° N, a region where England et al. (2014) found maximum regression between the observed Interdecadal Pacific Oscillation (IPO) and wind stress variability. Again, we also use a larger region, 150° E–150° W and 10° S–10° N, as in Saenko et al. (2016), to assess the robustness of our results. In the following, we refer to these as the England and Saenko regions. All regions are displayed in Fig. 2.
For the GMST and SST observations we use 1961–1990 as the reference period, whereas we compute anomalies with respect to 1982–2010 for the wind stress reanalyses fields.
To estimate unforced climate variability, we use pre-industrial control (piControl) simulations from 33 CMIP5 models and 35 CMIP6 models consisting of 18,797 and 21,740 simulated years, respectively. The models used are listed in Table S1 in the supporting information. We linearly detrend the control simulations to remove residual model drift.
We compare the observed warming against the means of CMIP5 and CMIP6 models. For the CMIP5 ensemble, 86 historical members from 38 models are available, and we extend these with the RCP8.5 scenario from 2006 onward (the choice of the scenario, however, does not make a large difference for 2006–2018; England et al. 2015). The CMIP6 ensemble consists of 47 models with 347 realizations. Besides their improved model physics, and a generally higher resolution, the CMIP6 models are forced with updated external forcings. From 2015 onward we use simulations under SSP5-8.5 forcing for which a subset of 34 models provides simulations. We compute the historical multi-model means by first averaging the members of each model to then average across the models (including only the first member of each model results in a very similar multi-model average). The uncertainty around the multi-model ensemble means is quantified by resampling the ensembles with replacement.
When comparing simulated to observed warming, we blend absolute SST over oceans with absolute near-surface air temperature over land and sea ice as in observations (procedure as introduced by Cowtan et al. 2015) for the CMIP5 models. Clarke and Richardson (2020) show that the blending bias expressed as the ratio of ΔGSAT, the global mean air temperature change, to ΔGMST, the blended temperature change, is similar for the CMIP5 and CMIP6 ensembles. Therefore, we approximate the CMIP6 ΔGMST as:
The last term on the right-hand side accounts for the difference in warming between the two ensembles. β is the ratio of (ΔGMST – ΔGSAT)/ΔGSAT, and we estimate it to be – 0.048 during 1900–2018 for the CMIP5 mean, consistent with other assessments (Richardson et al. 2018). For ERSSTv5, night-time marine air temperature observations are used to correct biases in SST measurements, but it is not obvious how this influences the differential warming between SSTs and marine air temperatures (Cowtan et al. 2015), and we therefore also compare GISTEMPv4 against blended model output.
For the historical simulations, we use the same reference periods as for the observations and assume that biases in the simulated climatological GMST project only weakly onto the simulated climate change (Hawkins and Sutton 2016; Stolpe et al. 2019).
We compare published studies that estimate the influence of tropical Pacific variability on global temperature using various methods (see Sect. 3). We restrict this comparison to studies that use a measure of Pacific variability, such as SST or surface wind variability, and relate this to GMST, and exclude studies that decompose GMST statistically into different components and then relate these to spatial patterns and modes of variability (e.g., Chen and Tung 2018; Dai and Wang 2018; Wei et al. 2019). Further we only consider studies that use a measure of tropical Pacific variability and omit studies that solely use other measures of Pacific internal variability [e.g., the IPO as in Meehl et al. (2016) or Power et al. (2017) or the Pacific Decadal Oscillation, PDO, as in Steinman et al. (2015)] to remove one source of potential spread between estimates. This leaves us with 18 studies that we use for the comparison—which we argue is a representative sample of the literature. All studies are summarized in Table S2.
Most of the data is provided by the corresponding authors (see acknowledgments) and for a few studies we extracted the data from figures in the individual papers. The data of Peyser et al. (2016) was not available to us, and we therefore computed it following their methodology (see supporting information). Within CMIP6, two projects include experiments dedicated to quantifying the role of time-evolving equatorial Pacific variability to regional and global temperature variability: The Decadal Climate Prediction Project (Boer et al. 2016; DCPP; “dcppC-pac-pacemaker” experiment) and the Global Monsoons Model Intercomparison Project (Zhou et al. 2016; GMMIP, “hist-resIPO” experiment). Data from one model, IPSL-CM6A-LR, following the dcppC-pac-pacemaker experiment was available and is also included in our analysis. At the time of writing, three models performed the hist-resIPO experiment, but each model only provided very small ensemble sizes (Table S2) and therefore the data is not included in our analysis.
To understand differences between the studies, and to test assumptions made when relating Pacific variability and GMST, we use variability analogues (Huber and Knutti 2014; Stolpe et al. 2017). Variability analogues are periods from piControl simulations for which the simulated, unforced variability matches the observed Pacific variability. The mean over the selected analogues in another variable, e.g., in GMST, then provides an estimate of the influence of Pacific variability on the examined quantity.
We measure tropical Pacific variability based both on SST and wind stress from the regions shown in Fig. 2 and standardize the observed and modelled time series of Pacific variability. This allows a better comparison between time series with different amounts of variability but has only a small impact on our results. Starting from January 1950 we select the 20 variability analogues from the more than 40,000 piControl years that have the smallest root-mean-square error (RMSE) with the observed time series of Pacific variability over a period of 40 months. We shift by 1 month and again select the best matching analogues starting from February 1950 and repeat this until we sampled the whole observational period. Then we average all the overlapping global near-surface air temperature fields of these variability analogues for every month and compute global mean time series. We assume that the relationship between Pacific variability and GMST is the same under present-day and pre-industrial conditions.
Comparison of methods to quantify the Pacific imprint on GMST
Methods to quantify the tropical Pacific influence on GMST can be broadly categorized into three groups. Regression-based approaches, pacemaker experiments, and freely evolving climate model simulations. In Table S2 we list key features of studies based on these methods.
In pacemaker experiments (Boer et al. 2016; Deser et al. 2017; Douville et al. 2015; Kosaka and Xie 2013, 2016; Swingedouw et al. 2017; Zhou et al. 2016), modelled SSTs in the central to eastern equatorial Pacific are nudged towards observed SST anomalies. The influence of Pacific variability is then estimated as the difference in GMST evolution between two ensembles: A freely evolving initial condition ensemble with historical changes in external radiative forcing, and an ensemble with nudged tropical SSTs, but the same historical forcing. Kosaka and Xie (2016) argue that the obtained estimate of GMST variability induced by the Pacific is independent of the climate model’s radiative forcing and climate sensitivity, and Douville et al. (2015) propose that it depends instead on the model-specific relationship between equatorial Pacific variability and GMST and in particular how strongly the equatorial variability projects onto high latitudes. Wang et al. (2017) similarly find that the tropical impact on high-latitude air temperature varies strongly between models on a decadal time scale and Deser et al. (2017) argue that atmospheric teleconnections forced by the tropical Pacific, which are not captured by all models, are of relevance for Eurasian and North American boreal winter temperature and thereby also GMST. The link between equatorial Pacific SST and global temperature has been shown to be overestimated in some models (e.g., in CanESM2, see Saenko et al. 2016). The SST-pacemaker approach creates an artificial heat sink in the Pacific which could bias, if large, the estimated Pacific contribution to global temperature variability (Tung and Chen 2018), but Kosaka and Xie (2016) argue this is not a major concern.
The key differences between the pacemaker studies are the climate models used, the number of ensemble members, which determines how much variability originating from outside the Pacific is still present, the SST dataset, and the restoring time scale. A larger restoring time scale allows the model to evolve more freely, and results in a more physical higher-frequency ocean-atmosphere interaction (Swingedouw et al. 2017). The larger restoring time scale has also been recommended for the CMIP6 DCPP pacemaker experiments (Boer et al. 2016).
To remedy the issue of artificial heat uptake, England et al. (2014), Delworth et al. (2015), Douville et al. (2015), Gastineau et al. (2019), Oka and Watanabe (2017), Svendsen et al. (2018), and Watanabe et al. (2014) prescribe wind stress trends instead of SST. This is done either over tropical oceans (Watanabe et al. 2014) or only over the tropical Pacific. The wind nudging experimental design comes with the disadvantage of larger uncertainties in wind stress from reanalyses compared to SST reconstructions. The agreement between reanalyses in decadal tropical Pacific wind stress trends is relatively poor in the early 20th century, but improves over time (Kajtar et al. 2018). Further, the SST evolution in the tropical Pacific is not constrained. While year-to-year variability in tropical Pacific SST is usually well-matched when wind fields are prescribed (Douville et al. 2015; Gastineau et al. 2019), decadal trends have been shown to be biased in some models (e.g., Gastineau et al. 2019), which then might lead to a biased GMST influence. Most wind-stress studies use ERA-interim, for which the robustness of tropical Pacific wind trends has been evaluated against several observational datasets (de Boisséson et al. 2014), but it is limited to the period after 1979. Watanabe et al. (2014), Oka and Watanabe (2017), and Svendsen et al. (2018) use JRA-55 and 20CR which cover a longer period.
In regression-based approaches (Folland et al. 2018; Foster and Rahmstorf 2011; Hu and Fedorov 2017; Johansson et al. 2015; Lean 2018; Rypdal 2018; Saenko et al. 2016; Schmidt et al. 2014) the observed GMST, or its rate of change, is modelled by a number of predictors that are linearly combined. These studies differ in which predictors they include, whether the predictors are filtered, for example with a long-memory response (Rypdal 2018), an e-folding response profile (Folland et al. 2018), or by using a mixed-layer model (e.g., Thompson et al. 2008), and the temporal resolution of the predictors, i.e., monthly or annual. The regression models typically consist of anthropogenic forcing, solar variability, stratospheric aerosol optical thickness as a measure of volcanic activity, and a term to describe tropical Pacific variability. Some studies include further modes of internal variability, such as the Atlantic Multidecadal Variability (AMV; e.g., Chylek et al. 2016; Folland et al. 2018; Rypdal 2018), or the Arctic Oscillation (AO; e.g., Folland et al. 2018), which can make a difference if predictors are correlated. Contrary to other regression analyses, Chylek et al. (2014) propose a minimal regression model with only greenhouse gas forcing and the AMV as predictors of annual GMST, but Rypdal (2018) argues that including the AMV at annual resolution misattributes GMST variability caused by ENSO variability and volcanic forcing to the AMV. This is because ENSO variability and volcanic forcing also influence North Atlantic SST, and accordingly the predictors are correlated. Regarding the Pacific variability term, regression-based studies often use the Nino3.4 index or the Multivariate ENSO index (MEI; Wolter and Timlin 2011). The latter is a more comprehensive way of characterizing ENSO variability than a purely oceanic, SST based index as it combines environmental variables from both the atmosphere and the ocean. Exceptions are Saenko et al. (2016) who instead use western tropical Pacific zonal wind stress as a predictor and Peyser et al. (2016) who relate the east-minus-west difference in tropical Pacific sea surface height to GMST variability.
A general concern of regression models is that the effect of predictors on GMST is not physically constrained and hence much of the variance is explained by construction, although a connection might not exist in reality. The more predictors are included, the larger the risks of overfitting. Kosaka and Xie (2016), Peyser et al. (2016), and Wang et al. (2017) argue that models simulate a GMST response to tropical Pacific variability that is around 20–45% larger on a decadal time scale than on an interannual time scale. Regression models are constructed on observations that are dominated by the latter and therefore might underestimate the amplitude of Pacific variability on GMST on a decadal time scale (Wang et al. 2017). Whereas Kajtar et al. (2019) demonstrate that the sensitivity of decadal GMST variability on the IPO is similar in the CMIP5 multi-model mean and observations, Haustein et al. (2019) reconcile observed and modelled warming during the twentieth century without a time scale dependent GMST response on tropical Pacific variability.
The third class of methods uses readily available climate model simulations to establish the effect of Pacific variability on GMST. This can be done either by searching for variability analogues from piControl simulations (Huber and Knutti 2014), regressing GMST on indices of Pacific variability in control (Peyser et al. 2016; Wang et al. 2017) or historical simulations (Kajtar et al. 2019), or by only including historical model simulations that are in the right ENSO phase to the ensemble mean (Risbey et al. 2014). The latter approach gives an ensemble mean that is closer to the observed warming (Risbey et al. 2014). The adjusted ensemble mean is, however, based on fewer models and may be less robust. A strength of the variability analogues method is that it retains the physical connection across variables, and does not induce an artificial heat sink. A limitation, however, is the sparsity of piControl simulations. With increasing length of the analogues, i.e., analogues that track the observed variability over a longer period, it becomes harder to find suitable analogues, and accordingly the Pacific SST trend is underestimated (Fig. S2 in the supporting information). Therefore, we here search for relatively short analogues of 40 months length to ensure that the selected analogues follow the observed variability closely. Also, the number of analogues selected at each time step is somewhat arbitrary, but the results are only weakly dependent on this threshold (Fig. S3). Further, the simulated relationship between Pacific and GMST variability could be biased and is not constrained by observations. This bias is, however, as we show later, likely substantially lower in multi-model analyses than in pacemaker experiments, which usually rely on a single climate model.
Simulated and observed global mean temperature change
We start by examining the long-term GMST increase simulated by the CMIP5 and CMIP6 ensemble means and whether there is evidence for a mismatch with the observed warming. Such a discrepancy might indicate that internal variability alone is insufficient in reconciling observed and modelled warming, but that there is a bias in radiative forcing or in how sensitive the climate responds to the imposed forcing.
The 1950–2018 long-term warming of both the CMIP5 and CMIP6 ensemble agrees well with what has been observed, but the CMIP6 ensemble mean shows greater warming than CMIP5 from around 1970 onward for trends ending in 2018. CMIP6 ensemble mean trends starting from 1975 and later even fall outside the observational 2σ envelope, although some bootstrapped samples of the ensemble mean remain within the observational uncertainty (Fig. 3a). This enhanced warming of the CMIP6 ensemble during the last decades is likely caused by its 11% higher ensemble mean TCR (2.03 °C compared to 1.83 °C for CMIP5; Table S1. Note that TCR estimates are not available for all models) (Flynn and Mauritsen 2020; Nijsse et al. 2020; Tokarska et al. 2020).
Several recent studies observationally constrained TCR to central values from 1.3 to 2.05 °C, with upper 95th percentiles of the constrained distributions in the range 1.9–2.4 °C (Fig. 3b). 20% of the CMIP6 models (9 out of 45 models with available TCR estimate; Table S1), but only one CMIP5 model, simulate a TCR that exceeds 2.4 °C, which is more than we would expect if the models were random samples of the observationally constrained TCR distributions, suggesting that some CMIP6 models overestimate the response to external forcing. We therefore also consider a constrained CMIP6 ensemble, CMIP6_con, for which we conservatively only include models with a TCR of less than 2.4 °C. CMIP6_con consists of 27 models (Table S1) with a mean TCR of 1.83 °C, virtually identical to that of the CMIP5 ensemble, and expectedly it simulates temperature trends from 1965 and onward which are closer to the observed trends (Fig. 3a).
Despite the overall agreement in long-term warming, and the potentially overestimated warming from CMIP6 to which we come back in Sect. 6, differences remain on decadal time scales (Fig. 1b) and we therefore examine the contribution of the tropical Pacific to these. We start with a general overview of the Pacific contribution to GMST since 1950 and then examine the ‘global warming hiatus’ in detail. We first present results of the published literature to then examine why studies come to differing conclusions on the GMST imprint of Pacific variability.
Study intercomparison: Pacific influence on global mean temperature
Overview: Pacific contribution 1950 to present-day
Across the assessed studies, there is broad agreement that tropical Pacific variability has contributed to the difference between observed and modelled warming since 1950. For the period from 1960 to 2012, the estimated tropical Pacific influence on GMST (in °C) from the examined studies is positively correlated with the difference between observed and modelled annual mean GMST (mean r = 0.69, with a range of 0.52–0.85; see Fig. S4 for details). After smoothing the time series with a running 5-year mean to emphasize lower frequency variability, the average correlation with the residual remains similar, r = 0.72, but the spread among the studies increases (r = 0.35–0.93) (Fig. S4).
Pacific variability may therefore explain a significant part of the difference between observed and modelled GMST increase on different time scales, but there is a large spread between the studies. Whereas the multiple linear regression studies indicate a consistent Pacific imprint on running 15-year long GMST trends (Fig. 4a), the variability across the SST and wind stress nudging experiments is considerably larger (Fig. 4b). The regression-based Pacific variability estimates reconcile observed and modelled warming during most of the examined period, except for temperature trends starting in the 1950s and during the ‘global warming hiatus’ although there is similarity in the temporal evolution during these periods. The pacemaker experiments display a larger spread and greater amplitude of GMST trends related to Pacific variability than the multiple regression estimates. Compared to the difference between observed and modelled GMST changes, several pacemaker experiments appear to overestimate the Pacific influence on GMST, but also suggest that potentially the complete discrepancy between observed and modelled running 15-year trends can be attributed to Pacific variability. These findings are similar when we instead examine running 10-, and 20-year long trends (Fig. S6).
Pacific contribution to the ‘global warming hiatus’
Next, we exemplarily examine the Pacific contribution to the ‘global warming hiatus’. This period is not only covered by all the studies, shows particularly large trends in the Pacific, but also the spread between the different studies is large. We use two different periods to define the ‘hiatus’, 1997–2012 and 1992–2012. The latter period is motivated by the onset of the acceleration in Pacific trade winds (England et al. 2014). The ‘hiatus’ ended with the years 2014–2016, when a strong El Niño released large amounts of heat from the north-western tropical Pacific (Yin et al. 2018), but we use 2012 as the end-year because most studies in our intercomparison only include data until then (cf. Table S2).
During 1997–2012, the observed warming was between − 0.21 and − 0.11 °C smaller than the modelled temperature increase of the multi-model ensemble means when calculated as the linear trend multiplied by its length (Fig. 5a). For the years from 1992 to 2012, this difference ranges from − 0.28 to − 0.19 °C (Fig. 5b). For both periods GISTEMPv4 shows slightly greater warming than CW19, but the uncertainty in modelled warming is larger than observational uncertainty. CMIP6 shows greater warming than CMIP5 and CMIP6_con and accordingly the largest divergence from observed GMST.
All inspected studies agree that the tropical Pacific acted to lower GMST trends during the early twenty-first century. The spread among the studies is, however, substantial and reaches a factor of more than five for 1992–2012 (Fig. 5b).
Most of the SST-based pacemaker studies indicate that the model—observation difference during both periods can be fully attributed to Pacific variability even under the high CMIP6 warming. The spread among the pacemaker studies is large, and several experiments find a contribution that is significantly larger than the actual model—observation difference. The experiments of Douville et al. (2015) show a cooling that is more than twice as large as that of the pacemaker experiment of Deser et al. (2017), although they mention that their model simulates a “weak but realistic ENSO-GMST relationship” on an annual time scale. On average the SST-pacemaker experiments simulate a cooling of 0.36 °C during 1992–2012, which is larger than the actual difference of 0.19–0.28 °C between observed and simulated warming.
Experiments where wind stress is overridden by reanalysis values span an even wider range. While Douville et al. (2015) find a contribution of − 0.12 °C for 1992–2012, the experiments of Watanabe et al. (2014) and Gastineau et al. (2019) show about four times larger influences on GMST. Douville et al. (2015) argue that MIROC5, the model used by Watanabe et al. (2014), has an unrealistically strong correlation between Pacific SST and GMST. In the wind stress experiment of Gastineau et al. (2019) the simulated cooling in the Nino3.4 region is more than twice as large as observed. This may be one reason why they find a larger Pacific contribution to the ‘hiatus’ than Swingedouw et al. (2017) who nudge eastern tropical SSTs in the same model. For the examined wind stress experiments, the global temperature decrease related to Pacific variability is on average 0.25 °C, which is sufficient to fully explain the observation—model discrepancy from 1992 to 2012. Among the wind stress pacemaker studies, the experiment of Svendsen et al. (2018) shows the smallest Pacific contribution during both periods. The use of 20CR, which shows a somewhat smaller intensification in Pacific trade winds than the other reanalyses during the ‘global warming hiatus’, or the relatively small ensemble size (Table S2) resulting in some internal variability from outside the Pacific still being present, might contribute to this.
The regression-based studies and variability analogues of Huber and Knutti (2014) show a smaller Pacific influence during the ‘global warming hiatus’, and these studies typically find additional contributions to the ‘hiatus’ from solar variability (e.g., Folland et al. 2018; Huber and Knutti 2014; Lean 2018) and stratospheric aerosols (Huber and Knutti 2014). Apart from the study of Saenko et al. (2016), which uses wind stress as a predictor and finds a considerably larger Pacific contribution than the other multiple regression studies, the Pacific induced cooling is smaller than in any SST-based pacemaker experiment. The GMST cooling estimated by multiple linear regression is on average 0.12 °C, or only about half of the difference between observed and modelled warming during 1992–2012 (estimates of Saenko et al. (2016) and Johansson et al. (2015) not included here). Adjusting the regression-based estimate upwards by about 40%, which is how much stronger GMST responds to tropical Pacific variability on average on a decadal than an interannual time scale according to CMIP5 models (Wang et al. 2017), still results in an estimate less than half of that of the SST-pacemaker experiments. This suggests that there are further fundamental differences between the methods. The regression of modelled GMST onto the east to west tropical Pacific sea surface height gradient (Peyser et al. 2016), results in a significantly larger suppression of the global mean temperature increase from 1997 to 2012, roughly in line with SST-based pacemaker experiment. Due to the short observational record it is difficult to assess how realistically models simulate this relationship. The regression coefficient is, however, similar across CMIP5 and CMIP6 models (supporting information).
In the following, we examine the differences between multiple linear regression and SST-based pacemaker experiments by inspecting the roles of anthropogenic forcings on tropical Pacific SST (Sect. 4.3) and of model uncertainty (Sect. 4.4). Then, we assess whether tropical Pacific wind variability leads to consistent results, and whether or not the differences between wind pacemaker experiments can be explained by observational uncertainty (Sect. 4.5).
Influence of forced trend in Pacific SST
Several studies assume there is no or a negligible forced signal in the tropical Pacific SSTs and directly use the area-mean SST as a predictor for GMST (cf. Table S2). Sometimes a long-term linear trend is removed (e.g., Hu and Fedorov 2017), and while this removes some external forcing, it probably does not remove all (e.g., Mann et al. 2014). If anthropogenic forcing is not fully accounted for, the tropical Pacific cooling due to internal variability during the ‘global warming hiatus’ period is underestimated by attributing it to external forcing. The MEI also shows a long-term positive trend, and might therefore contain a forced signal (Lewis and Curry 2018). Since the MEI is a combination of several variables, some of which might be less influenced by external forcing, it is not obvious where this signal originates. In pacemaker experiments the forced signal is implicitly removed as it is present in both the nudged and the freely evolving experiment. These experiments, however, rely on the faithful representation of the forced signal by a single climate model.
We estimate the forced signal in the tropical Pacific with the method of Turkington et al. (2019) and by using multi-model means. Turkington et al. (2019) quantify the forced signal as the linear trend in tropical SSTs from 30° S to 30° N over 1962–2011, a period chosen such that there is little trend in the IPO. The rate of global warming, however, increased significantly in the early 1970s (Rahmstorf et al. 2017) related to changes in anthropogenic forcing. This might bias the linear trend low. The approach further assumes that the tropical-wide forced trend is similar to the forced signal in the eastern tropical Pacific. Different to Turkington et al. (2019), we only estimate one trend over the whole period instead of separately for every month.
Alternatively, we directly take the multi-model means over the respective regions as estimates of the forced signal. Some higher frequency variability is still present, and we therefore smooth the multi-model means with a loess smoother, although that also partly removes the volcanic signal (Fig. 6a). The multi-model means show similar forced responses, and relative to that the Turkington method underestimates the forced signal in the past two decades, yet the multi-model means could be biased. It has therefore been suggested to scale either the regional multi-model mean SST (e.g., Frankcombe et al. 2015) or the simulated GMST (e.g., Kajtar et al. 2019) against the observed SST evolution in the region of interest by means of linear regression. In the case of the eastern equatorial Pacific SST the scaling factor is, however, not stable, but decreases when the most recent decades are included. This is not surprising given the occurrence of the ‘global warming hiatus’. Nonetheless, the scaling approach indicates a forced signal that is in between the Turkington et al. approach and the unscaled regional ensemble means (Fig. S8). Since we sample a reasonable range of the forced response uncertainty, we do not include the scaling approach in the following analysis.
We subtract the estimates of the forced signal from the observed SSTs to obtain the actual internal variability. After the correction, SSTs become colder during the late period of the observational record (Fig. 6b). The approach of Turkington et al. (2019) spuriously warms the mid-twentieth century, which is a limitation of the linear extrapolation. Using these forcing corrected SST time series, we estimate the Pacific contribution to GMST with the variability analogues method.
Overall, the running 15-year long trends associated with Pacific variability exhibit agreement with the difference between observed and modelled warming, irrespective of the method used to estimate the forced response, but differences become evident during recent decades (Fig. 7a). During the ‘global warming hiatus’ the uncorrected, raw SST index underestimates the Pacific contribution as is expected from the presence of a forced signal (Fig. 6b).
From 1992 to 2012 (Fig. 7b), Pacific variability reduces the GMST increase by 0.09–0.10 °C when the forced warming of the Pacific is not accounted for. This is similar to the results of Rypdal (2018) and Huber and Knutti (2014), who directly use the uncorrected Nino3.4 index. With the Turkington et al. (2019) method, the Pacific contribution increases to 0.14–0.17 °C, and with the multi-model means removed, to 0.18–0.22 °C (with CMIP5 mean subtracted), 0.17–0.23 °C (with CMIP6), and 0.16–0.21 °C (with CMIP6_con). The results from the different climate model ensembles are similar, because their forced responses are similar (Fig. 6a). This demonstrates the importance of removing the forced signal: It approximately doubles the influence of the Pacific during the ‘hiatus’.
Kosaka and Xie (2013) additionally performed a SST-based pacemaker experiment with fixed radiative forcings, which conceptually corresponds to using observed, uncorrected SST within a regression model or within variability analogues. The difference between the two types of experiments reveals a similar effect as discussed, and instead of cooling by more than 0.4 °C during 1992–2012 (Fig. 5b), global temperatures are reduced by only 0.13 °C when forcings are kept constant.
Removing the forced response from observed SST naturally makes a smaller difference for earlier periods, because the radiative forcing was weaker. Nonetheless, the effect cannot be neglected. Depending on whether variability cools or warms the planet during a certain period, accounting for positive radiative forcing will either increase or decrease the Pacific influence. For the period 1974–1995, as an example, the observed warming was greater than modelled, and the Pacific variability shows a positive trend. Part of the Pacific warming is externally driven and removing it lowers the internal variability contribution to the warming during this period. We suspect this is one reason why the SST-based pacemaker and regression-based estimates overlap during this period (Fig. S7), but not during the ‘global warming hiatus’ (Fig. 5b).
Contribution of model uncertainty
While the method of estimating and removing the forced response from Pacific SST is important, in particular during the recent ‘hiatus’ period, it does not explain why some SST-pacemaker studies find a Pacific contribution that is even larger. To examine this, we rank the climate models according to their sensitivities with which the simulated GMST responds to variability in the tropical Pacific on a decadal time scale. We estimate the sensitivities by regressing GMST trends on pacemaker SST trends in each model’s control simulation for 16-year long trends (corresponding to the period 1997–2012), 21-year long (1992–2012) and 22-year long trends (1974–1995). Then, we multiply these sensitivities with the observed SST change during each period. AMV may also affect GMST on these time scales, and including the modelled AMV as an additional predictor decreases the spread in regression coefficients relating the Pacific variability influence to GMST somewhat, but does not fundamentally change the conclusions.
This analysis demonstrates, in agreement with Wang et al. (2017), that there are considerable differences in how strongly tropical Pacific SST variability projects onto global mean temperatures between models. On the examined time scales, there is at least a factor of two difference between low- and high-sensitivity models (Fig. 8). The combination of model uncertainty and forced signal explains most of the spread across the studies examined: if the forced signal is not accounted for, even high-sensitivity models would not be able to fully explain the ‘global warming hiatus’ (which is also the case for the control experiment of Kosaka and Xie (2013) as discussed in the previous section). In absolute terms, the spread between low- and high-sensitivity models is relatively small if the forced signal is not removed. However, if it is accounted for, the sensitivity of a single model becomes more important, and the ‘hiatus’ contribution ranges from less than 0.15 °C to around 0.40 °C cooling (Fig. 8; middle), as we indeed observe (Fig. 5b). From 1974 to 1995, when Pacific variability acted to increase GMST, removing the forced response reduces Pacific warming and accordingly the model spread shrinks.
To verify whether modelled sensitivities are supported by observations, we subtract estimates of the forced signal, based on the multi-model ensemble means, from the SST and GMST time series from 1900 to 2018 and then follow the procedure as described. As shown in Fig. 8, observationally based estimates are comparable to that of the multi-model median, consistent with a similar analysis of Kajtar et al. (2019) for the IPO. Model-based estimates of the Pacific contribution to GMST variability should therefore be based on a sufficiently large number of climate models, either by repeating pacemaker experiments with different models, or by using variability analogues from a large set of control simulations.
Variability analogues on wind trends
Motivated by the large spread across wind-stress based pacemaker experiments (Figs. 5, S7), we next address the question, whether these experiments are expected to result in a similar Pacific contribution as SST-based setups, and what role observational uncertainty plays. Therefore, we first examine the wind response in analogues selected from tropical Pacific SST.
In these analogues, the standardized variability in zonal wind stress in the western tropical Pacific agrees well with observed variability (Fig. 9a), but 15-year long trends in absolute wind stress are generally underestimated (Fig. 9b). Swingedouw et al. (2017) observe a similar underestimation in wind stress trends when they nudge towards observed SSTs in their pacemaker experiment. This might indicate too weak SST-wind coupling in the climate model ensemble, other sources of internal variability (Swingedouw et al. 2017), or that the wind stress trends are partly driven by processes outside the Pacific, such as tropical Atlantic Ocean SST variations (e.g., Chikamoto et al. 2016; McGregor et al. 2014).
There is only a negligible forced Pacific wind stress trend in the historical simulations (Fig. 9b), consistent with the findings of Watanabe et al. (2014), which circumvents the need for estimating and removing the forced signal when searching for wind-based variability analogues. Unlike the SST time series, we do not standardize the wind stress prior to selecting analogues, as the standardized wind stress variability is already well captured when searching for SST-based analogues, but the absolute trend is underestimated.
The eastern equatorial Pacific SST response is overestimated in some wind-stress experiments (England et al. 2014; Gastineau et al. 2019), and we examine whether this is also the case with the variability analogues. As depicted in Fig. 10a, 15-year long trends in tropical Pacific SST are generally well-matched in the analogues based on wind variability. While SST trends starting in the 1960s tend to be underestimated in the analogues, trends starting from the early 1990s are overestimated. It is striking that the overestimation in the latter period is less severe than the underestimation of wind stress trends in SST-based analogues during the same period (cf. Figure 9b). We do not investigate this further, but it could be related to the set of models selected to provide analogues, and to a general tendency of the analogues to underestimate large changes in the target quantity.
Given that the wind stress analogues realistically reproduce eastern Pacific SST, we still consider them a useful setup for quantifying the Pacific influence on GMST. Except for trends starting in the 1950s, the effect of Pacific variability estimated from wind analogues reconciles observed and modelled GMST changes (Fig. 10b), and is similar to estimates based on SST-analogues after accounting for the forced response (Fig. 7a). Observational uncertainty is probably not the main reason for the differences among the wind-stress pacemaker experiments, because the different reanalyses show similar trends (Fig. 9b) and accordingly similar imprints on GMST during the studied period (Fig. 10b). However, we only examine the wind variability over a relatively small region, whereas the pacemaker experiments prescribe winds over a much larger region (Table S2), and significant differences might exist elsewhere.
To examine the spread among wind-based pacemaker experiments further, we regress modelled GMST trends against wind stress trends (i.e., as in Sect. 4.4 for tropical Pacific SST). This reveals that the spread in regression slopes between models is even larger than with tropical Pacific SST (Fig. S10), which might not be surprising given that the wind variability is less directly connected to GMST variability (Saenko et al. 2016). This reaffirms the need for repeating pacemaker experiments with multiple different climate models.
While we demonstrate that models that track the observed tropical Pacific variability (either by nudging or by searching for sufficiently short analogues) closely resemble the observed GMST changes, we have not yet examined whether models are actually capable of doing so on their own. Figure 11 compares both the observed SST trends in the tropical Pacific (Fig. 11b), from which we remove different estimates of the forced signal, and wind stress trends from reanalyses (Fig. 11a) with modelled variability from piControl simulations during the ‘global warming hiatus’. Consistent with the results of England et al. (2014), CMIP5 models are unable to simulate the intensification of trade winds during the ‘global warming hiatus’ (Fig. 11a). Observed wind stress trends starting in the early 1990s are not seen in any CMIP5 model irrespective of the reanalysis. Although the CMIP6 ensemble displays a broader range of 21-year long Pacific trade wind trends, only one model, MIROC6, simulates trends within the observed range.
Climate models generally appear to underestimate Pacific trade wind variability on a decadal time scale (Kajtar et al. 2018; Kociuba and Power 2015), possibly related to model biases in Atlantic mean SST, which mute the contribution of Atlantic SST variations to Pacific trade wind trends (Kajtar et al. 2018; McGregor et al. 2018), or there is an external, forced contribution to wind stress that models miss (cf. Figure 9b). In particular, the origin of the tropical Atlantic warming during the ‘global warming hiatus’, whether internal variability or anthropogenically forced, matters for the interpretation of the Pacific trade wind acceleration (McGregor et al. 2018). It has further been suggested that anthropogenic aerosols play a role during the ‘global warming hiatus’ by altering the trade winds and the state of the PDO (Smith et al. 2016; Takahashi and Watanabe 2016), but the robustness of these results has been questioned (Kuntz and Schrag 2016; Oudar et al. 2018). Further, observational uncertainties exist, and these are particularly large in the pre-satellite era (Bordbar et al. 2017; Kajtar et al. 2018). Reanalyses have been argued to overestimate the intensification of the Pacific Walker circulation during the past decades when compared to satellite-derived estimates (Chung et al. 2019), but de Boisséson et al. (2014) found the tropical Pacific trade wind trends, which are the surface expression of the Walker circulation cell, to be robust in different observations including reanalyses.
Regarding the eastern tropical Pacific SST trends, Fyfe and Gillett (2014) found that none of 117 historical CMIP5 simulations reproduces the observed regional cooling from 1993 to 2012, and Kajtar et al. (2019) argue that the CMIP5 ensemble underestimates IPO variability on time scales greater than 10 years. When searching for 21-year long trends in the piControl simulations, both the CMIP5 and CMIP6 ensembles show trends as observed during the ‘global warming hiatus’ from 1992 to 2012 (Fig. 11b), but with a higher frequency in the CMIP6 ensemble. Whereas 9–23 out of 33 CMIP5 models (depending on the dataset, and the method of removing the forced response from the observations) are capable of simulating cooling equal to or exceeding the observed eastern tropical Pacific cooling, 13–28 out of 35 CMIP6 models do so.
There is some evidence that the response of the tropical Pacific SST to anthropogenic forcing is biased in CMIP5 models (Coats and Karnauskas 2017), with too much warming in the eastern tropical Pacific, possibly related to a climatological cold bias of models’ equatorial cold tongues (Seager et al. 2019). If that is the case, the Pacific cooling during the ‘global warming hiatus’ from internal variability is smaller, as discussed in Sect. 4.3. This, in turn, would imply that less of the discrepancy between observed and modelled warming during the ‘global warming hiatus’ can be attributed to Pacific internal variability (cf. Figure 7b). A more detailed analysis of the CMIP6 ensemble will be required to assess whether the cold tongue bias has improved from CMIP5 and how to best quantify the forced signal in the tropical Pacific. This issue is common to all methods of quantifying the Pacific influence on GMST based on observed SST. Better constraining the forced signal in the tropical Pacific will help to reduce the uncertainty of the influence of internal Pacific variability on GMST during the ‘hiatus’ and in the future.
Conclusion: reconciling observed and modelled global mean temperature
While the three multi-model means track the overall observed GMST change from 1950 to 2018 well, with Pearson correlation coefficients of 0.96, 0.94, and 0.95, for CMIP5, CMIP6 and CMIP6_con, respectively, they do not match the year-to-year variability (Fig. 1a), and differences exist on decadal time scales (Fig. 1b). After adding in the influence of the tropical Pacific, keeping the potential limitations discussed in the previous section in mind, most of the discrepancies between observed and modelled GMST are resolved, and the correlation coefficients increase to 0.99 (with CMIP5), 0.97 (CMIP6), and 0.98 (CMIP6_con) (Fig. 12a). In agreement with Lehner et al. (2016), the apparent mismatch between simulated and observed volcanic cooling is also resolved after adjusting the multi-model means for the effect of Pacific variability.
Whereas the GMST trends of the CMIP5 and CMIP6_con ensemble means are similar to the observed trends after accounting for Pacific variability, the CMIP6 warming remains larger than observed during the past four decades (Fig. 12b). This is consistent with growing evidence that some CMIP6 models with a high TCR, present in CMIP6 but not in CMIP6_con, overestimate past and future warming (Brunner et al. 2020; Dittus et al. 2020; Liang et al. 2020; Nijsse et al. 2020; Tokarska et al. 2020; Winton et al. 2020), and supports a TCR of around or slightly below 1.8 °C. However, we stress that uncertainties in the tropical forced signal (Fig. 6) and the sensitivity with which GMST responds to Pacific variability (Fig. 8) remain.
The good agreement between observed and modelled warming since 1950 does not necessarily imply that they agree for the right reasons. First, there is significant uncertainty in the forced signal, as is evident from the ensemble spread, but this is not represented when analysing multi-model ensemble means, and similar forced signals can be achieved with various combinations of aerosol forcing and climate sensitivity (Kiehl 2007; Knutti 2008). Second, observational uncertainty remains (e.g., Davis et al. 2019), which might influence both the difference between modelled and observed warming, and the indices of internal variability used in this study. Third, further modes of internal variability might affect the observed global mean temperature evolution. In particular, the Atlantic Multidecadal Variability (AMV) has been argued to contribute significantly to GMST variations (e.g., Chen and Tung 2018; Chylek et al. 2016; Wu et al. 2019), although this view has been challenged repeatedly (e.g., Booth et al. 2012; Haustein et al. 2019). In the supporting information we estimate the AMV contribution to GMST and show that it does not reduce the difference between models and observations, but on the contrary, increases it. Further research is required to better understand this, but we note that the AMV contribution to GMST is relatively small after 1980 irrespectively.
We have shown that differences in the estimated Pacific contribution to GMST arise primarily from the method of how (and if) the forced signal in the tropical Pacific is accounted for and from the sensitivity of GMST on tropical Pacific SST and wind variability on a decadal time scale which varies substantially across models, in agreement with Wang et al. (2017) and Bordbar et al. (2019). When we account for this, we can reproduce most of the spread across the 18 studies examined. Further factors, such as a time-scale dependence of the Pacific influence on GMST (Peyser et al. 2016; Wang et al. 2017) likely further contribute to the differences between the studies.
Our results demonstrate that pacemaker experiments using a single model should be interpreted with caution. Based on observations, we have demonstrated that high sensitivities between tropical Pacific SST and GMST as simulated by some models are unlikely, but observations support a sensitivity similar to the multi-model median, consistent with Kajtar et al. (2019). To obtain robust estimates, pacemaker experiments should therefore be repeated with several models, as is currently done within CMIP6. For IPSL-CM5A-LR, the wind-stress simulation indicates a greater Pacific contribution to the ‘hiatus’ than the SST-nudging experiment (Gastineau et al. 2019; Swingedouw et al. 2017), whereas it is the opposite for CNRM-CM5 (Douville et al. 2015). Artificial heat uptake in SST-based pacemaker experiments is therefore presumably not a major concern compared to other uncertainties when quantifying the Pacific effect on GMST.
For multiple-regression approaches we recommend careful evaluation of whether the predictors contain a forced signal, how it influences the results, and how to best remove it prior to the analysis. There might be cases where it is justifiable not removing the forced signal, e.g., if a minimum Pacific contribution to the ‘global warming hiatus’ is estimated, but the assumptions should be clearly stated.
GISTEMPv4 is available from https://data.giss.nasa.gov/gistemp/. CW19 is available from http://www-users.york.ac.uk/~kdc3/papers/coverage2013/series.html (‘HadCRUT4 + HadSST4 infilled by kriging’). There we also accessed the Cowtan and Way (2014) datasets with HadSST3 and COBE-SST2 (used for Fig. S1). Berkeley Earth Surface Temperature was downloaded from http://berkeleyearth.org/data/ (also used for Fig. S1). COBE-SST2 (https://www.esrl.noaa.gov/psd/data/gridded/data.cobe2.html), and ERSSTv5 (https://www.esrl.noaa.gov/psd/data/gridded/data.noaa.ersst.v5.html) were obtained from NOAA/OAR/ESRL PSD, Boulder, Colorado, USA. ERA5 wind stress data was downloaded from https://cds.climate.copernicus.eu/, JRA-55 data from https://jra.kishou.go.jp/JRA-55/index_en.html, and MERRA2 data was downloaded from http://gmao.gsfc.nasa.gov/reanalysis/MERRA-2. NOAA-CIRES 20CR v2c was obtained from https://www.esrl.noaa.gov/psd/data/gridded/data.20thC_ReanV2c.html. CMIP5 and CMIP6 data is available from http://pcmdi9.llnl.gov/. The CESM1 large ensemble output was obtained from http://www.cesm.ucar.edu/projects/community-projects/LENS/. We downloaded data of the CESM1 Pacific pacemaker experiment from https://www.earthsystemgrid.org/dataset/ucar.cgd.ccsm4.pac-pacemaker.html. We digitized figures from the studies of Huber and Knutti (2014), Johansson et al. (2015) and Schmidt et al. (2014) to obtain their estimates of Pacific influence on GMST. Data from the other studies was provided by the corresponding authors of the respective studies and is available upon request.
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We are grateful to Hervé Douville, Chris Folland, Grant Foster, John Fyfe, Guillaume Gastineau, Shineng Hu, Yu Kosaka, Judith Lean, Kristoffer Rypdal, Lea Svendsen, Didier Swingedouw and Masahiro Watanabe for providing data. Urs Beyerle helped to download the CESM1 pacemaker experiments and the MERRA2 data. We thank David Clarke for helpful advice on the blending bias within the CMIP6 ensemble. We thank the two anonymous reviewers for the helpful comments and suggestions. We thank the National Center for Atmospheric Research for making their climate model output publicly available. We acknowledge the World Climate Research Programme’s Working Group on Coupled Modelling, which is responsible for CMIP, and we thank the climate modelling groups (listed in Table S1 of this paper) for producing and making available their model output. For CMIP the U.S. 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.
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Stolpe, M.B., Cowtan, K., Medhaug, I. et al. Pacific variability reconciles observed and modelled global mean temperature increase since 1950. Clim Dyn (2020). https://doi.org/10.1007/s00382-020-05493-y
- Internal variability
- Decadal variability
- Global mean temperature