Skip to main content

Lessons on Climate Sensitivity From Past Climate Changes


Over the last decade, our understanding of climate sensitivity has improved considerably. The climate system shows variability on many timescales, is subject to non-stationary forcing and it is most likely out of equilibrium with the changes in the radiative forcing. Slow and fast feedbacks complicate the interpretation of geological records as feedback strengths vary over time. In the geological past, the forcing timescales were different than at present, suggesting that the response may have behaved differently. Do these insights constrain the climate sensitivity relevant for the present day? In this paper, we review the progress made in theoretical understanding of climate sensitivity and on the estimation of climate sensitivity from proxy records. Particular focus lies on the background state dependence of feedback processes and on the impact of tipping points on the climate system. We suggest how to further use palaeo data to advance our understanding of the currently ongoing climate change.


The concept of climate sensitivity has been introduced with the aim of providing a measure of the response of the climate system to ‘external’ perturbations to Earth’s radiative balance. It is a useful quantity for projecting climate changes over the coming century as a response to increasing concentrations of atmospheric greenhouse gases.

The simplest framework of climate sensitivity is to think of the difference in global annual mean surface temperature ΔT between two statistical steady states, which have a different pCO2 level. A general equilibrium climate sensitivity parameter, indicated here by S, is given by

$$ S = \frac{\Delta T}{\Delta R} $$

where ΔR is the difference in radiative forcing between the climate states. More specifically, if ΔR is the radiative forcing associated with a doubling of atmospheric CO2, then the equilibrium climate sensitivity (ECS) is defined as ECS = \(S\cdot {\Delta } R_{2xCO_{2}}\). Due to the presence of feedbacks, the radiative perturbation can be amplified to lead to a larger ΔT than would be expected based on the direct effect of the increase in pCO2 on the radiative balance [1, 2].

Observational studies using the instrumental period together with model simulations give a range of ECS values between 1.5 and 4.5 C per CO2 doubling [3]. There remain, however, considerable uncertainties regarding the range of ECS, in particular concerning its upper limits, although understanding of the spread in model-based results is emerging, suggesting short-wave cloud feedbacks as the dominant source of intermodel differences [46]. Furthermore, analysis of ECS from the response to individual forcings [7], observational constraints from mixed-phase clouds [8], and estimates of transient climate sensitivity from observations of the last half century [9] all suggest that in particular, the higher values cannot be rejected.

Past climate changes can help to estimate the response of the climate system to variations in external forcing or greenhouse gas concentrations [10, 11]. One approach consists in considering ensembles of experiments with climate models, either perturbed parameter ensembles [1214] or multi-model ensembles [15, 16], which may also be calibrated to past climate observations [17]. Climate sensitivity estimates with this method may be delivered as probability distributions following the paradigm of Bayesian inference, but with the usual caveats of the many assumptions on the model, the observations used, and judgements on uncertainties of models and data [18]. The posterior distribution obtained with a given climate model may differ from another one. It is also expected to depend on the choice of observations used for calibrations, as well as on judgements about model uncertainties. Finally, experts advocate the importance of careful considerations about model structural errors, often termed discrepancy in this context [19]. Another approach for estimating climate sensitivity is to use time series of past climate changes and estimate climate sensitivity relevant to the present-day problem based on differences between different times sampled within the time series [20]. As more palaeoclimate data become available, with better estimates of pCO2 and ΔT, there appears to be a strong potential for the latter approach to be successful and thereby provide an independent estimate of the present ECS.

However, the response of the climate system to a radiative forcing perturbation occurs on many different timescales, due to the presence of different feedbacks [21]. This multi-scale response becomes particularly important if long timescales associated with the geological record are considered. On a timescale of a hundred years, the effect of fast feedbacks, such as the water-vapour feedback, has equilibrated. However, slower feedbacks, such as those associated with ocean heat uptake, or even slower land-ice changes will continue to cause adjustment of the climate system.

For the present climate, the equilibrium climate sensitivity parameter S has been introduced with a century timescale in mind [22], indicating that only a limited number of (relatively fast acting, <100 years) feedback processes are taken into account. The radiative perturbation ΔR is considered as the effective radiative forcing after very fast processes have equilibrated [3]. As climate model simulations generally do not reach full equilibrium, in particular with respect to ocean heat uptake, S is determined from the transient towards that equilibrium using the residual net top-of-the-atmosphere radiative imbalance [23].

When slow feedbacks also affect a proxy time series, one cannot determine S directly from these data. To this end, the concept of Earth system sensitivity (ESS) has been introduced [24], with ESS = \(S^{p}\cdot {\Delta } R_{2xCO_{2}}\) and S p (where ‘p’ stands for palaeo) quantifying the long-term (>1000 years) equilibrium response in global mean surface temperature after an increase in atmospheric pCO2 including the multi-scale Earth system feedbacks (except carbon cycle feedbacks). Because many more positive (slow) feedbacks are involved, S p is generally larger than S [24, 25].

In [21], the relation between S p and S was clarified and it was also described how to meaningfully compare values among different studies from different times in the past. When extracting S from past climate reconstructions, it is necessary to correct S p for slow feedback processes. If this is carefully done [21], then the range of climate sensitivity values found from palaeoclimate studies of the last 65 million years (Myr) broadly confirms the range covered by mostly climate model and observation-derived values given by the IPCC [3]; at the 68 % probability level, the IPCC range is S = 0.4−1.2 K (W m −2) −1, while the PALAEOSENS approach has led to S = 0.6−1.3 K (W m −2) −1. On the one hand, this result is promising if we view the fact that independent estimates of climate sensitivity do, in principle, improve our confidence in the mean value of climate sensitivity. On the other hand, it is disappointing that the extreme values of the currently accepted range of possible climate sensitivity could not be more confidently rejected from inspection of the palaeoclimate records. This state of affairs has been explained by the uncertainty in palaeoclimate reconstructions (temperature changes, forcing, and feedback strengths), and the fact that S focuses only on global mean quantities, which are inherently difficult to determine from local proxy observations [11]. However, it may also be that the concept of climate sensitivity should be extended or generalised in order to better account for the spatial distribution of temperature and radiative forcings, and for the different factors that affect the definition of the climate sensitivity parameter given in Eq. 1 as has been already suggested by Skinner [26].

For example, the astronomical forcing does not fit the climate sensitivity definition (Eq. 1) because this forcing mainly influences climate through changes in the seasonal and latitudinal distributions of the insolation, with little direct effects on the global average [27]. Effects associated with the slow tectonic forcing and erosion may also alter both the mean state of climate and the climate sensitivity since feedbacks are generally expected to vary with the background climate [1, 15, 20, 23, 2832]. More generally, the ratio (Eq. 1) between temperature and forcing may depend on the nature and spatial distribution of the forcing itself [26], as we clarify below. Finally, climate changes in the past as well as the present are a non-stationary response of the climate system to forcing and the question is, which, if any, of the responses can be considered to be in equilibrium. In past climate changes, a multitude of timescales (in forcing and response) play a role, and we cannot a priori assume a (constant) separation of fast and slow timescales. Even if there was timescale separation, non-linear processes in the climate system will introduce variability on any (new) timescale, which further complicates the analysis of the response to forcing in such a system. Estimating climate sensitivity from past climate changes (in models or observations) therefore requires a careful definition of the response timescale, the corresponding averaging procedure, and a careful analysis of the feedbacks involved. The presence of multiple scales in the response of the climate system to perturbations is apparent when one approaches the problem from the point of view of dynamical system theory and non-equilibrium statistical mechanics [33, 34].

The aim of this paper is to further clarify how the geological record can contribute to estimates of equilibrium climate sensitivity and its uncertainty. The focus is on the background state dependence of feedback processes and on the impact of tipping points on the climate system. Alternative concepts of climate sensitivity characterising the response to the present-day forcing in the complex climate system are also reviewed.


When determining S, it is mostly assumed that temperature differences are relatively small in comparison with the background temperature such that ΔR can be well approximated by

$$ {\Delta} R \simeq \left( \frac{\partial R}{\partial T}+ \frac{\partial R}{\partial \alpha}\frac{\partial \alpha}{\partial T}\right){\Delta} T. $$

Here, the terms in brackets represent the Planck response (\(\frac {\partial R}{\partial T}\)) and the combined effect of all (net positive) feedback processes α(T) (\(\frac {\partial R}{\partial \alpha }\frac {\partial \alpha }{\partial T}\)) [35]. While the higher order terms in ΔT are usually small, they can become important and may lead to runaway climates, i.e. rapid climate change when the system crosses a tipping point, reinforced by positive feedbacks until a new steady state is reached [36, 37].

In [21], feedback processes α were divided into two categories: fast process α f with timescales smaller than τ and the slow process α s with timescales larger than τ. The radiative heat flux changes due to the slow processes α s have no effect on ΔT on the timescale τ, and hence, only the fast processes contribute to the radiative heat flux changes responsible for ΔT. In view of the present-day climate change, we select τ = 100 years (as suggested in [21]) and define

$$ S = \frac{\Delta T}{\Delta R_{[CO_{2}]}}, $$

where the total response ΔT (due to all fast processes with respect to the timescale τ) is measured with respect to the radiative heat flux change due to the change in atmospheric CO2. By including an arbitrary number N of fast processes in addition to the Planck response, S is given by

$$ S = \frac{-1}{\lambda_{P} + {\sum}^{N}_{i=1} {\lambda^{f}_{i}}}, $$

with the Planck response parameter λ P < 0 and \({\lambda ^{f}_{i}} = {\Delta } R_{[{\alpha ^{f}_{i}}]}/{\Delta } T\) the feedback parameters of the fast process \({\alpha ^{f}_{i}}\). Using the surface energy balance, it was shown that S can be obtained from S p, according to

$$ S = S^{p} (1 + \frac{{\sum}^{M}_{j=1} {\lambda^{s}_{j}}}{\lambda_{P} + {\sum}^{N}_{i=1} {\lambda^{f}_{i}}}), $$

where each \({\lambda ^{s}_{j}} = {\Delta } R_{[{\alpha ^{s}_{j}}]}/{\Delta } T\) represents the feedback parameter of the slow process \({\alpha ^{s}_{j}}\) [21].

For practical estimates of S, all slow processes (with respect to the 100-year timescale) are considered forcings. Next, the specific climate sensitivity parameter

$$ S_{[CO_{2}, {\alpha^{s}_{1}}, \cdots, {\alpha^{s}_{m}}]} = \frac{\Delta T}{ {\Delta} R_{[CO_{2}]} + {\sum}^{m}_{j=1} {\Delta} R_{[{\alpha^{s}_{j}}]}}, $$

is computed leading to (if in reality there are M slow processes)

$$ S = \lim_{m \rightarrow M} S_{[CO_{2}, {\alpha^{s}_{1}}, \cdots, {\alpha^{s}_{m}}]}. $$

This approach is fully compatible with linear response theory [38, 39] where a linear relation is obtained between forcing and response although the equilibrium states are fully determined by non-linear processes. However, by linearly regressing the decay of the radiative imbalance on ΔT [23], feedback processes are assumed to stay constant, while deviations from the linear relationship have been suggested more recently on century timescales [40, 41], implying that the non-linear version of the response theory should be taken into account [34]. Moreover, interannual to decadal climate variability is generally averaged out by determining S intrinsically assuming that the processes generating the variability do not significantly interact with the background climate [33]. The definition of S in Eq. 3 allows for a consideration of the climate response (on the 100-year time scale) in any climate state of the Earth’s history including the present climate. Because the feedback processes need not be equally strong during all times, we specify a point in time to S, i.e. S(t), where S(t = 0) represents the present equilibrium climate sensitivity parametre (termed S a or ‘actuo’ climate sensitivity in [21]). The variation of S(t), S [X](t), and S p(t) over time is directly associated with the background state (or temperature) dependence of the feedback parametres λ P , λ f, and λ s, which we discuss in the next section.

State Dependence of Climate Sensitivity

In this section, we review progress in understanding the state dependence of the climate sensitivity parameter S(t) from both palaeo data and modelling studies.

Using palaeo data to reconstruct climate sensitivity has the advantage of portraying real-world responses that integrate all (known and unknown) processes. A key drawback, however, is that the reconstructions rely on indirect (proxy) measurements of the relevant quantities. Many proxies rely on calibrations in the modern environment. Hence, their use into deep geological time may be complicated by subtle changes through time in overall ocean chemistry, uncertain extrapolation into environmental conditions outside the calibration window (non-analogue conditions), and chronological uncertainties between the various records that are being compared. Modelling studies can help tackle some of such potential complications, but in turn may be compromised by explicit and implicit assumptions, and by a potential lack of (or incomplete representation) of processes, whether known or unknown. Palaeoclimate sensitivity studies need to account for both observations and modelling results, including transparent consideration of uncertainties wherever possible. This is particularly important when addressing the subtle problem of potential state dependence, which we focus on here.

State Dependence From Palaeo Data

Some new (re-)interpretation of existing palaeo data has emerged since the review of the PALAEOSENS project in 2012. Previous observation-based studies [21, 47] had indicated that climate sensitivity might be state dependent, but we’re not yet able to quantify this dependence. Progress was made when it was inferred from data through the entire interval covered by ice cores (last 800 kyr) that S may have been 30–40 % lower during full glacial conditions than during intermediate glaciations [20] (see yellow dots in Fig. 1). This was found to apply to both the simplest version of the specific climate sensitivity parameter, S [C O2,L I], in which CO2 radiative forcing was corrected only for the land-ice (LI) albedo feedback, and for the most complex version that also accounted for radiative forcing by all main greenhouse gases (GHGs), including CH4 and N2O, and including corrections for the slow feedbacks of albedo variation caused by vegetation (VE) and aerosols (AEs) (i.e. S [G H G,L I,V E,A E]). The general shape of this dependence was recently supported by a combined model-data approach [48]. Further support for a lower S [C O2,L I] during colder periods was found [32, 45] (green/brown dots in Fig. 1), showing that an extension of this state-dependence analysis is possible over the last 2.1 Myr based on existing boron-based CO2 proxy data. Furthermore, ice sheet volume and area are explicitly calculated using an ice sheet model implying a non-linear relation between volume and extent essentially caused by the rheological characteristics of ice. These results suggest that the latitudinal variation and strength of the land-ice albedo feedback is important for detecting state dependence in S; hence, other approaches did not detect the state dependence, given that they approximated land-ice albedo feedback by more simplified means (e.g. based on sea-level changes [49]). In particular, Rohling et al. [27] estimated zonally averaged changes in the land-ice albedo feedback from a combination of sea-level change, annual mean incoming solar radiation, and area-weighted scaling factors accounting for the latitudinal distribution of ice sheets but nevertheless detected no significant state dependence.

Fig. 1
figure 1

Published paleo-based values of \(S_{\mathrm [CO_{2},LI]}\) (specific equilibrium climate sensitivity parameter caused by CO2 radiative forcing and corrected by variations in land-ice (LI) feedbacks) indicating its state dependence. Only studies published after the PALAEOSENS review paper [21] are considered. For comparison, the state-independent values from PALAEOSENS, and from the IPCC report [3], and the CMIP5 multi-model mean for present day [41] are also shown. All values of \(S_{\mathrm {[CO_{2},LI]}}\) were given as mean (or most likely) ±1σ, apart from IPCC, which is the 90 % confidence (CF) range. Climate background states are given by ΔT from pre-industrial and are marked as estimated ranges (or ±2σ). In [42], further corrections for other slow feedbacks have been calculated, which has been ignored here, leading to different values of ΔT than published. To increase the clarity of the figure, the data-based results are visualised by colour-coded circles (mean values), while their uncertainties are combined in a cumulative probability density distribution (grey shading) assuming normal distributed values. Results based on climate models are shown by colour-coded squares (mean) including their uncertainties (bars). G glacial, IG interglacial, LE late Eocene, EE early Eocene, LP pre-PETM/late Paleocene, PETM Paleocene-Eocene thermal maximum. Reference numbers of the given citations: IPCC 2013 [3], PALAEOSENS 2012 [21], Andrews 2012 [41], Caballero 2013 [43] vdHeydt 2014 [20], Martinez-Boti 2015 [44] Köhler 2015 [32], Anagnoustou 2016 [42], Köhler 2016 [45], and Shaffer 2016 [46]

A new dataset of proxy-based CO2 from the Pliocene [44] has been used to state that S [C O2,L I] was similar in the late Pleistocene and the Pliocene implying no state dependence for S within the uncertainties (cyan points in Fig. 1). However, this study did not search for the state dependence of S within the Pleistocene itself and also used a sea level-based land-ice albedo feedback calculation, which would limit the potential to detect state dependence. The polar amplification factor is another uncertain parameter in these studies that could mask state dependence; climate models suggest a non-constant polar amplification and potentially less strong in the Pliocene than in the Pliocene [24, 32, 50, 51].

State Dependence on Climate Models

There is a growing modelling literature on how climate sensitivity may change with the climate state. Early work with a simplified coupled climate model [52] indicated higher sensitivity in climates colder than modern, which they argued was due to an increased role for cryospheric surface albedo feedback. The same conclusion was drawn from a range of modern climate models [53]. A study using the GISS Model E confirmed higher sensitivity in colder climates but also found higher sensitivity at high forcing, with a minimum in sensitivity near the modern climate [54]. Recent work using a modified version of the same model supported this non-monotonic U-shaped behaviour of climate sensitivity [55]. None of these studies quantitatively analysed the underlying feedback mechanisms driving the changes in sensitivity. The first study to do so across a broad range of climates was using the Australian Bureau of Meteorology model spanning a range of 1/16 to 32 times modern CO2 [56]; they found monotonically decreasing sensitivity as CO2 and temperature increased via a combination of decreasing surface albedo and cloud short-wave (SW) feedback strengths. On the other hand, Caballero and Huber [43] conducted Eocene simulations using NCAR CCSM3 spanning 1 to 32 times CO2 and found a transition to much higher sensitivity when global mean temperature increased above 23 C, driven by a sharp increase in positive SW cloud feedback and a more modest increase in water vapour feedback (see blue squares in Fig. 1). Within the same model [57] and the MPI-ECHAM6 over a smaller range of forcing [58], increasing sensitivity at higher CO2 was found due to mostly increased water-vapour feedback. As commonly found in model intercomparisons, the intermodel differences in sensitivity are driven mostly by cloud feedbacks. However, enhanced sensitivity in cold climates due to stronger surface albedo feedback and in warm climates due to stronger water vapour feedback emerge as robust features across models, suggesting that the non-monotonic U-shaped structure of climate sensitivity may have some qualitative validity (see Fig. 1).

Another line of work has focused on comparing the sensitivity to negative radiative forcing under last glacial maximum (LGM) conditions (due to combined decrease in CO2 and increased surface albedo) to positive forcing under doubled CO2 [15, 31, 59, 60]. These studies generally find a more muted response to negative than to positive forcing. This implies a weaker sensitivity for climates on the cold side of modern than on the warm side as the observation-based studies also suggest (which in turn implies that if the overall non-monotonic structure discussed above is true, then the minimum sensitivity is attained in climates colder than the LGM). However, these conclusions rely on an implicit assumption that a unit of radiative forcing by ice-sheet albedo is interchangeable with a unit of radiative forcing by CO2 [61]. This caveat also applies to the observation-based studies discussed above, and it is a key issue that remains to be tested [32].

Climate Sensitivity in the Presence of Tipping Points

It has been well-recognised that the concept of equilibrium climate sensitivity is quite limited when making adequate projections of global mean surface temperature for the end of this century [33]. The climate system has a strong internal variability on many timescales, is subject to a non-stationary forcing, and certainly is out of equilibrium with the changes in the radiative forcing up to the year 2100. Moreover, in the past, abrupt shifts have occurred, and also for the present climate, a number of potential tipping elements have been identified [66, 67].

Consider, for example, a typical zero-dimensional energy balance model as shown in [68], which has for a range of atmospheric CO2 concentrations two stable climate states coexisting, an ice-free state and an ice-covered one (see Fig. 2). These two climate states are often interpreted as the snowball Earth and a much warmer greenhouse climate, which both may have existed in the far distant past [69, 70]. There can be, however, more branches in such a system [71], including partially glaciated climate states. The transition from the greenhouse climate during the early part of the Cenozoic to the climate states with major polar ice sheets (on one or both hemispheres) that existed since the Oligocene [72] can, therefore, conceptually be considered as a transition between different branches like those in Fig. 2.

Fig. 2
figure 2

Schematic of the phase diagram of a climate model with two stable coexisting climate states. The shape of the S curve follows closely that discussed in [6264]; see also [65]. The climate sensitivity parameter S is defined on each of the stable branches as the local slope of the global mean surface temperature T versus the (logarithm of) atmospheric pCO2 (cf. Eq. 8). Type I state dependence: When starting at point A (e.g. the pre-industrial climate), the temperature increase after a doubling of pCO2 (point B) is smaller than when starting from a colder climate (point C) on the same branch. Type II state dependence: When the initial pCO2 is the same as in point A, but the climate is initially on the cold branch (point D), a doubling of pCO2 results in a smaller temperature increase (point E) than if starting from point A and ending in point B. S becomes undefined at the transition points (open squares) between the two branches. The conditional climate sensitivity is equal to S for small perturbations (going from points D to E), but largely increases if the perturbation in CO2 is large enough to move the system from point D beyond the bifurcation point (blue open square) and jumps to the warm branch. Note that S is generally defined as a local gradient, while the 2xCO2 definition in the ECS may involve a perturbation too large for the linear assumption along the branch to be applicable

The equilibrium climate sensitivity S is well defined along most of the two branches, but infinite at the bifurcation (tipping) points themselves. Moreover, the local slope along each branch depends on how feedback processes depend on the background temperature, i.e. it does not need to be constant. As long as there is a steady-state branch, the climate sensitivity parameter S (Eq. 1) is given by

$$ {S} = \frac{\partial E(\textbf{x}(\mu))}{\partial R_{[\mu]}}, $$

where E(x) is a metric for the state of x (i.e. the global mean temperature T) and the parameter μ indicates the (logarithm of the) CO2 concentration (see Fig. 2).

These considerations lead us to define two types of state dependence of climate sensitivity. Type I refers to the fact that the strength of fast feedbacks depends on the control parameter, so that S on one branch varies with T. To define the type II state dependence, let us first observe that at the (saddle node) bifurcation points (open squares in Fig. 2), the derivative becomes infinitely large, indicating a structural change in the model climate system. This structural change is reflected in the two branches of the system, which exhibit different behaviours as to climate sensitivity: at one particular pCO2 in the multiple equilibria range, two (different) values for S can be determined. If the slopes on the two branches are different, then the climate sensitivity depends which branch the system is on. In other words, the climate sensitivity depends on the active feedbacks determining the background climate. The type II state dependence then refers to the fact that the strength and number of active feedbacks may depend on the equilibrium point being visited, even if the control parametre is the same. As the saddle-node bifurcation is approached, non-linear effects may become increasingly important, such that the first-order Taylor expansion of the radiative forcing (see Eq. 2) may not be sufficient any more. The closer to the bifurcation point the background climate is, equilibrium non-linearity leads to run-away climate, or at least jumps to some other stable climate branches [37].

In [68], the concept of conditional climate sensitivity parametre S(δ,t e ) of a background climate state (indicated by \(\bar {T}\)) was defined as

$$ S(\delta, t_{e}) = \frac{\Delta T(\delta, t_{e})}{\Delta R(\delta, t_{e})} $$

where \({\Delta } T(\delta , t_{e}) = | T(t_{e}) - \bar {T} |\) is the maximum temperature difference that can occur under the constraint \(| T(0) - \bar {T} | < \delta \) over a time t e , and ΔR(δ,t e ) is the change in radiative forcing over the same time interval. Note that scalar norms are used here, but the model to determine it can be very high dimensional. In a climate system in which there is a single equilibrium for each value of pCO2, S(δ,t e ) is independent of δ (i.e. there is no region of conditional stability) and will approach the equilibrium climate sensitivity S parameter in the limit t e . In this limit, ΔT will be precisely the difference between the temperature of the equilibrated states and ΔR the difference in radiative forcing between both states (Eq. 8).

The conditional climate sensitivity is also suited for situations in which bifurcations occur (and type II state dependence). For example, suppose we are on the lower branch (point D in Fig. 2), when increasing CO2 (or μ) up to point E, the equilibrium climate sensitivity is relatively small. Such values are found in [68], for t e =100 years when δ is relatively small. When the initial perturbations are large (i.e. increasing CO2 beyond the blue open square in Fig. 2), however, the system may jump to another state (upper branch in Fig. 2), increasing the sensitivity greatly.

In addition to steady-state dynamics, more complicated dynamics may occur on each of the branches such as periodic orbits. Self-sustained oscillations mimicking the late Pleistocene ice-age cycles have been found in models by [7379], and also in a slightly more complex model by [80] as relaxation oscillations. The issues of internal climate variability on palaeoclimatic timescales are discussed in more detail in [77, 81, 82]. In these cases, while S still is defined by Eq. 8, ΔT may not be a smooth function any more, critically depending on the timescale of interest. For example, when considering the Pleistocene ice ages as (long-term) oscillations, the sensitivity derived from comparing glacial with interglacial periods will differ from the sensitivity to CO2 doubling in a climate model, because the two extremes of the oscillation cannot be reached within a century timescale [83]. Shorter timescale variability may be represented by stochastic noise in the forcing, which then requires adaptation of climate sensitivity in probabilistic terms [84].

Challenges Ahead

One of the main insights about climate sensitivity that has been gained from palaeoclimate studies is its potential state dependence. Consequently, findings about the value of S from past climate states that are colder (most of the Pleistocene) or significantly warmer (e.g. Eocene) may not be directly applicable to projections of global warming in the present climate due to anthropogenic CO2 emissions. Nevertheless, for future climate projections, it is crucial to know whether there is state dependence or not and which processes are responsible. This is particularly important for improving the confidence in climate models used for future projections, if processes such as cloud feedbacks are involved that are not adequately captured in those models [85]. The challenge now is to further quantify state dependence from past climate changes and to understand the responsible processes from both models and data.

On the data side, adequate statistical methods should be used to detect whether scatter plots of temperature change over radiative forcing (ΔT over ΔR) follow (locally) linear or non-linear behaviour indicating constant or state-dependent characteristics of S [X]. More precise and higher resolved CO2 data (for the pre-ice core interval > 800 kyr) and more robust time series of global temperature change as well as (model-interpreted) land-ice and vegetation reconstructions will be necessary to quantify the state dependence of S.

The difficulty lies, however, not only in the uncertainties intrinsic to proxy reconstructions: even if we were able to reconstruct, say, past CO2 levels and ice sheet extents with great accuracy, there would remain considerable uncertainty in the radiative forcing actually supplied. Recent work [41] quantifying the forcing due to quadrupled CO2 across the CMIP5 model ensemble, for example, shows that the canonical value of 3.7 Wm −2 for CO2 doubling is precise only to about 1 Wm −2. Much of this uncertainty comes from the role of tropospheric adjustment—the direct tropospheric response to CO2 before surface temperature has changed—whose importance has only recently come to the fore [61]. The uncertainty in radiative forcing due to ice sheets is even less well known, having been quantified in only a handful of models (e.g. [60, 86, 87]). The treatment of CO2 as forcing in the climate sensitivity framework needs further clarification; in past climate changes, co-variation is a dynamic process [83, 88] while in models used for future projection the response to fixed CO2 is considered. Finally, potentially differing efficacies of forcings remain largely unexplored. Orbital forcing [89] is generally believed to play a key role in the waxing and waning of glacial cycles [90, 91], although the precise mechanisms remain debated [9294]. Feedback processes in particular those related to snow, sea-, and and land-ice albedo [47, 95] are central to understanding ice age cycles. Most likely, the annual mean radiative imbalance caused by these feedback processes is much stronger than the initial orbital radiative forcing [27, 32, 49]. In climate sensitivity studies, orbital forcing has been largely ignored because the direct effect of forcing is predominantly seasonal (at least the precessional component), while the climate response is measured on century timescales focusing on the global annual mean value of the radiative forcing [21]. However, when determining climate sensitivity in periods with glacial cycles, differing orbital configurations need to be taken into account. For example, climate sensitivity measured from the Eemian period, where summer insolation was high in the Northern Hemisphere, is difficult to compare with the recent anthropogenic warming caused by enhanced levels of greenhouse gases. This difference is only partly reflected in the state dependence, as seen in the different values of S during glacial and interglacial periods [20, 32, 96]. Disentangling the contributions to S of orbital forcing and feedback state dependence requires running climate models under different orbital configurations, which at the same time effectively performs out-of-sample tests of the models [97]. Even outside the glacial-interglacial cycles, it is important to quantify how orbital variations affect local proxy data [98].

Another problem still lies in the quantification of S from time series of palaeo data. Recent work [45] suggests that the methods for calculating S can not simply be transferred from the state-independent to the state-dependent case, because the state dependence may appear as a non-smooth (not even locally) relationship between S and T. A further complication arises when tipping points have been crossed in the time series [20], where the classical definition of S breaks down. Therefore, robust methods to detect and interpret those tipping points in palaeo data need to be further developed [99101], but also the recently suggested generalisations of S such as the conditional climate sensitivity [68] or the quantification of non-linear contributions in the Taylor expansion of the radiative balance [37] need to be further explored.

When it comes to alternative metrics for characterising the response of the climate system to changes in the forcing, clearly, more than one single climate sensitivity parametre is required. The difficulty of accounting for the effect of orbital forcing highlights two major shortcomings in the concept of climate sensitivity, namely the lack of both spatial and temporal structures in the climate response.

Not only the radiative forcing varies in latitude but also the temperature response may exhibit spatial structure, e.g. [27]. One important and still a large-scale quantity is the equator-to-pole temperature gradient, which is generally believed to be smaller in the ice-free and high greenhouse gas climates of the early Cenozoic with different feedbacks at work [102105]. In colder climate states with ice, the temperature response is clearly latitude dependent as reflected in polar amplification factors between polar and global mean temperature change. Polar amplification varies over time, but how remains largely unknown [32, 59, 60, 106, 107]. Another form of spatial and temporal patterns in the response to forcing can appear in terms of the major modes of climate variability such as the El Ni˜no Southern Oscillation (ENSO) or the monsoons, which may change their pattern, amplitude, or frequency through (non-linear) interactions with the background climate [108111].

An extension of the concept of S as given by Eq. 8 to the non-stationary nature of the climate response could be to also consider the change in higher order moments (e.g. variance, skewness) and the long tails of distributions of temperature instead of only using the (temporal) mean as metric E(x). The information contained in all moments together can be captured in one single metric (Wasserstein distance) as suggested recently in a non-autonomous stochastic dynamical system approach to climate sensitivity [33, 112]. Response theory provides an additional way for incorporating rather general measures of climate sensitivity; it allows prediction of both globally averaged quantities and spatial patterns of change [39]. In all of these approaches, the challenge is to keep concepts simple enough to be applied to palaeo data without oversimplification.

In conclusion, while a major challenge remains to improve accuracy in past climate reconstructions, one of the important issues we can learn from past climates about climate sensitivity is to better understand its potential state dependence in order to eventually reduce the uncertainty in ECS. At the same time, from a theoretical point of view, it is necessary to further develop and apply alternative concepts for quantifying the response to forcing in the highly complex climate system as have been outlined in this review, with special emphasis to those, which can also (practically) be determined from the geological record.


  1. Knutti R, Rugenstein MAA. Phil Trans R Soc A 2015;373:20150146. doi:10.1098/rsta.2015.0146.

  2. Schwartz SE. Surv Geophys 2012;33(3):745. doi:10.1007/s10712-012-9180-4.

  3. IPCC. Climate change 2013: the physical science basis. Contribution of Working Group I to the Fifth Assessment Report of the Intergovernmental Panel on Climate Change (Cambridge University Press, Cambridge, United Kingdom and New York, NY, USA).

  4. Vial J, Dufresne JL, Bony S. Clim Dyn 2013;41(11-12):3339. doi:10.1007/s00382-013-1725-9.

  5. Caldwell PM, Zelinka MD, Taylor KE, Marvel K. J Clim 2016; 29(2):513. doi:10.1175/JCLI-D-15-0352.1.

  6. Zhao M, Golaz JC, Held IM, Ramaswamy V, Lin SJ, Ming Y, Ginoux P, Wyman B, Donner LJ, Paynter D, Guo H. J Clim 2016;29(2):543. doi:10.1175/JCLI-D-15-0191.1.

  7. Marvel K, Schmidt GA, Miller RL, Nazarenko LS. Nature Clim Change 2016;6(4):386. doi:10.1038/nclimate2888.

  8. Tan I, Storelvmo T, Zelinka MD. Science 2016;352(6282):224.

    CAS  Article  Google Scholar 

  9. Storelvmo T, Leirvik T, Lohmann U, Phillips PCB, Wild M. Nature Geosci 2016;9(4):286. doi:10.1038/ngeo2670.

  10. Edwards TL, Crucifix M, Harrison SP. Prog Phys Geogr 2007;31(5):481.

    Article  Google Scholar 

  11. McCarroll D. Int J Qual Sci 2015;30(2):154. doi:10.1002/jqs.2775.

  12. Schneider von Deimling T, Held H, Ganopolski A, Rahmstorf S. Clim Dyn 2006;27:149. doi:10.1007/s00382-006-0126-8.

  13. Annan J, Hargreaves JC. Geophys Res Lett 2006;33:L06704. doi:10.1029/2005GL025259.

  14. Schmittner A, Urban NM, Shakun JD, Mahowald NM, Clark PU, Bartlein PJ, Mix AC, Rosell-Melé A. Science 2011;334(6061):1385. doi:10.1126/science.1203513.

  15. Crucifix M. Geophys Res Lett 2006;33(18):L18701. doi:10.1029/2006GL027137.

  16. Schmidt GA, Annan JD, Bartlein PJ, Cook BI, Guilyardi E, Hargreaves JC, Harrison SP, Kageyama M, LeGrande AN, Konecky B, Lovejoy S, Mann ME, Masson-Delmotte V, Risi C, Thompson D, Timmermann A, Tremblay LB, Yiou P. Clim Past 2014;10(1):221. doi:10.5194/cp-10-221-2014.

  17. Hargreaves JC, Annan JD, Yoshimori M, Abe-Ouchi A. Geophysical Research Letters 2012;39(24):L24702. doi:10.1029/2012GL053872.

  18. Owhadi H, Scovel C, Sullivan T. SIAM Rev 2015;57(4):566. doi:10.1137/130938633.

    Article  Google Scholar 

  19. Brynjarsdóttir J, O’Hagan A. Inverse Problems 2014;30(11):114007. doi:10.1088/0266-5611/30/11/114007.

    Article  Google Scholar 

  20. von der Heydt AS, Köhler P, van de Wal RSW, Dijkstra HA. Geophys Res Lett 2014;41(18):6484. doi:10.1002/2014GL061121.

    Article  Google Scholar 

  21. PALAEOSENS Project members. Nature 2012;491(7426):683. doi:10.1038/nature11574.

    Article  Google Scholar 

  22. Charney JG. 1979. Carbon dioxide and climate: a scientific assessment (National Academy of Science, Washington, D.C., U.S.A).

  23. Gregory JM, Ingram WJ, Palmer MA, Jones GS, Stott PA, Thorpe RB, Lowe JA, Johns TC, Williams KD. Geophys Res Lett 2004;31(3):L03205. doi:10.1029/2003GL018747.

  24. Lunt DJ, Haywood AM, Schmidt GA, Salzmann U, Valdes PJ, Dowsett HJ. Nat Geosci 2010;3(1):60. doi:10.1038/ngeo706.

  25. Pagani M, Liu Z, LaRiviere J, Ravelo AC. Nat Geosci 2010;3(1):27. doi:10.1038/ngeo724.

  26. Skinner L. Science 2012;337(6097):917. doi:10.1126/science.1224011.

  27. Rohling EJ, Medina-Elizalde M, Shepherd JG, Siddall M, Stanford JD. J Clim 2012;25:1635. doi:10.1175/2011JCLI4078.1.

  28. Senior CA, Mitchell JFB. Geophys Res Lett 2000;27(17):2685. doi:10.1029/2000GL011373.

  29. Andrews T, Forster PM. Geophys Res Lett 2008;35:L04802. doi:10.1029/2007GL032273.

  30. Andrews T, Gregory JM, Webb MJ. J Clim 2015;28:1630. doi:10.1175/JCLI-D-14-00545.1.

  31. Yoshimori M, Hargreaves JC, Annan JD, Yokohata T, Abe-Ouchi A. J Clim 2011;24:6440. doi:10.1175/2011JCLI3954.1.

  32. Köhler P, de Boer B, von der Heydt AS, Stap LB, van de Wal RSW. Clim Past 2015;11:1801. doi:10.5194/cp-11-1801-2015.

  33. Ghil M. Climate change: multidecadal and beyond (World Scientific Publ. Co., 2015, pp. 31–51), chap. 2, A mathematical theory of climate sensitivity or, How to deal with both anthropogenic forcing and natural variability.

  34. Lucarini V, Blender R, Herbert C, Ragone F, Pascale S, Wouters J. Rev Geophys 2014;52(4):809. doi:10.1002/2013RG000446.

  35. Roe G. Annu Rev Earth Planet Sci 2009;37:93. doi:10.1146/

  36. Zaliapin I, Ghil M. Nonlinear Process Geophys 2010;17(2):113. doi:10.5194/npg-17-113-2010.

  37. Bloch-Johnson J, Pierrehumbert RT, Abbot DS. Geophys Res Lett 2015;42(12):4973. doi:10.1002/2015GL064240.

  38. Ragone F, Lucarini V, Lunkeit F. Clim Dyn 2016;46(5-6):1459. doi:10.1007/s00382-015-2657-3.

  39. Lucarini V, Ragone F, Lunkeit F. J Stat Phys 2016:1–29. doi:10.1007/s10955-016-1506-z.

  40. Li C, von Storch JS, Marotzke J. Clim Dyn 2013;40(5):1071. doi:10.1007/s00382-012-1350-z.

  41. Andrews T, Gregory JM, Webb MJ, Taylor KE. Geophys Res Lett 2012;39(9):L09712. doi:10.1029/2012GL051607.

  42. Anagnostou E, John EH, Edgar KM, Foster GL, Ridgwell A, Inglis GN, Pancost RD, Lunt DJ, Pearson PN. Nature 2016;380(7603). doi:10.1038/nature17423.

  43. Caballero R, Huber M. Proc Natl Acad Sci 2013;110:14162. doi:10.1073/pnas.1303365110.

  44. Martinez-Boti MA, Foster GL, Chalk TB, Rohling EJ, Sexton PF, Lunt DJ, Pancost RD, Badger MPS, Schmidt DN. Nature 2015;518(7537):49. doi:10.1038/nature14145.

  45. Köhler P, Stap LB, von der Heydt AS, de Boer B, van de Wal RSW. Clim Past Discuss 2016;2016:1. doi:10.5194/cp-2016-23.

  46. Shaffer G, Huber M, Rondanelli R, Pedersen JOP. Geophys Res Lett 2016;43(12):6538. doi:10.1002/2016GL069243.

  47. Köhler P, Bintanja R, Fischer H, Joos F, Knutti R, Lohmann G, Masson-Delmotte V. Quat Sci Rev 2010;29(1-2):129. doi:10.1016/j.quascirev.2009.09.026.

  48. Friedrich T, Timmermann A, Tigchelaar M, Timm OE, Ganopolski A. Science Advances in press 2016.

  49. Hansen J, Sato M, Kharecha P, Beerling D, Berner R, Masson-Delmotte V, Pagani M, Raymo M, Royer DL, Zachos JC. Open Atmos Sci J 2008;2(217). doi:10.2174/1874282300802010217.

  50. Haywood AM, Hill DJ, Dolan AM, Otto-Bliesner BL, Bragg F, Chan WL, Chandler MA, Contoux C, Dowsett HJ, Jost A, Kamae Y, Lohmann G, Lunt DJ, Abe-Ouchi A, Pickering SJ, Ramstein G, Rosenbloom NA, Salzmann U, Sohl L, Stepanek C, Ueda H, Yan Q, Zhang Z. Clim Past 2013;9(1):191. doi:10.5194/cp-9-191-2013.

  51. Stap LB, de Boer B, Ziegler M, Bintanja R, Lourens LJ, van de Wal RSW. Earth and Planet Sci Lett 2016;439(1). doi:10.1016/j.epsl.2016.01.022.

  52. Manabe S, Bryan K, Geophys J. Res Oceans 1985;90:11689.

  53. Kutzbach JE, He F, Vavrus SJ, Ruddiman WF. Geophys Res Lett 2013;40:3721. doi:10.1002/grl.50724.

  54. Hansen J, Sato M, Ruedy R, Nazarenko L, Lacis A, Schmidt G, Russell G, Aleinov I, Bauer M, Bauer S, Bell N, Cairns B, Canuto V, Chandler M, Cheng Y, Del Genio A, Faluvegi G, Fleming E, Friend A, Hall T, Jackman C, Kelley M, Kiang N, Koch D, Lean J, Lerner J, Lo K, Menon S, Miller R, Minnis P, Novakov T, Oinas V, Perlwitz J, Perlwitz J, Rind D, Romanou A, Shindell D, Stone P, Sun S, Tausnev N, Thresher D, Wielicki B, Wong T, Yao M, Zhang S. J Geophys Res 2005;110(D18):D18104. doi:10.1029/2005JD005776.

  55. Russell GL, Lacis AA, Rind DH, Colose C, Opstbaum RF. Geophys Res Lett 2013;40:5787. doi:10.1002/2013GL056755.

  56. Colman R, McAvaney B. Geophys Res Lett 2009;36:L01702. doi:10.1029/2008GL036268.

  57. Jonko AK, Shell KM, Sanderson BM, Danabasoglu G. J Clim 2013;26:2784. doi:10.1175/JCLI-D-12-00479.1.

  58. Meraner K, Mauritsen T, Voigt A. Geophys Res Lett 2013; 40 (22): 5944. doi:10.1002/2013GL058118.

  59. Hargreaves JC, Abe-Ouchi A, Annan JD. Clim Past 2007;3:77. doi:10.5194/cp-3-77-2007.

  60. Yoshimori M, Yokohata T, Abe-Ouchi A. J Climate 2009;22:3374. doi:10.1175/2009JCLI2801.1.

  61. Sherwood SC, Bony S, Boucher O, Bretherton C, Forster PM, Gregory JM, Stevens B. Bull Am Meteorol Soc 2015;96:217. doi:10.1175/BAMS-D-13-00167.1.

  62. Ghil M. J Atmos Sci 1976;33:3.

  63. Ghil M, Childress S. Topics in geophysical fluid dynamics: atmospheric dynamics, dynamo theory, and climate dynamics. Berlin/Heidelberg/New York: Springer-Verlag; 1987.

  64. Ghil M. Nonlinear Process Geophys 2001;8(4/5):211. doi:10.5194/npg-8-211-2001.

  65. Bódai T, Lucarini V, Lunkeit F, Boschi R. Clim Dyn 2015;44:3361.

  66. Lenton TM, Held H, Kriegler E, Hall JW, Lucht W, Rahmstorf S, Schellnhuber HJ. Proc Nat Acad Sci 2008;105(6):1786. doi:10.1073/pnas.0705414105.

  67. Drijfhout S, Bathiany S, Beaulieu C, Brovkin V, Claussen M, Huntingford C, Scheffer M, Sgubin G, Swingedouw D. Proc Natl Acad Sci 2015;112(43):E5777.

  68. Dijkstra HA, Viebahn JP. Commun Nonlinear Sci Numer Simul 2015;13(1–3). doi:10.1016/j.cnsns.2014.09.015.

  69. Pierrehumbert RT, Abbot D, Voigt A, Koll D. Annu Rev Earth Planet Sci 2011;39:417.

  70. Rose BEJ, Ferreira D, Marshall J. J Clim 2013;26(9):2862. doi:10.1175/JCLI-D-12-00175.1.

  71. Bhattacharya K, Ghil M, Vulis IL. J Atmos Sci 1982;39:1747.

  72. Zachos JC, Dickens GR, Zeebe RE. Nature 2008;451(7176):279. doi:10.1038/nature06588.

  73. Kallen E, Crafoord C, Ghil M. J Atmos Sci 1979;36(12):2292. doi:10.1175/1520-0469(1979)036%3C2292:FOIACM%3E2.0.CO;2.

  74. Ghil M, Le Treut H. J Geoph Res 1981;86(C6):5262.

    Article  Google Scholar 

  75. Maasch KA, Saltzman B. J Geophys Res Atmos 1990;95(D2):1955. doi:10.1029/JD095iD02p01955.

  76. Saltzman B, Maasch KA. Earth and Environmental Science Transactions of the Royal Society of Edinburgh 1990;81(04):315. doi:10.1017/S0263593300020824.

  77. Ghil M. Physica D 1994;77:130.

  78. Paillard D, Parrenin F. Earth Planet Sc Lett 2004;227:263. doi:10.1016/j.epsl.2004.08.023.

  79. Ashwin P, Ditlevsen P. Clim Dyn 2015;45:2683–2695. doi:10.1007/s00382-015-2501-9.

  80. Gildor H, Tziperman E. J Geophys Res 2001;106(C5):9117. doi:10.1029/1999JC000120.

  81. Saltzman B. 2001. Dynamical Palaeoclimatology, (Academic Press, New York, U.S.A.)

  82. Crucifix M. Philos Trans R Soc A Math Phys Eng Sci 2012;370(1962):1140. doi:10.1098/rsta.2011.0315.

  83. von der Heydt AS, Ashwin P. 2016. 1604.03311. In review.

  84. Thuburn J. Quat J Roy Met Soc 2005;131(605):73. doi:10.1256/qj.04.46.

  85. Huber M. Nature Geosci 2013;6:15.

  86. Hewitt C, Mitchell J. Clim Dyn 1997;13:821.

    Article  Google Scholar 

  87. Goldner A, Huber M, Caballero R. Clim Past 2013;9:173. doi:10.5194/cp-9-173-2013.

  88. Scheffer M, Brovkin V, Cox PM. Geophys Res Lett 2006; 33 (10): L10702. doi:10.1029/2005GL025044.

  89. Milankovitch M. 1941. Kanon der Erdbestrahlung und seine Anwendung auf das Eiszeiten-problem (Roy. Serbian Acad.)

  90. Hays JD, Imbrie J, Shackleton NJ. Science 1976;194:1121. doi:10.1126/science.194.4270.1121.

  91. Imbrie J, Boyle EA, Clemens SC, Duffy A, Howard WR, Kukla G, Kutzbach J, Martinson DG, McIntyre A, Mix AC, Molfino B, Morley JJ, Peterson LC, Pisias NG, Prell WL, Raymo ME, Shackleton NJ, Toggweiler JR. Paleoceanogr 1992;7(6):701. doi:10.1029/92PA02253.

  92. Huybers P, Tziperman E. Paleoceanography 2008;23(1). doi:10.1029/2007PA001463.

  93. Kawamura K, Parrenin F, Lisiecki L, Uemura R, Vimeux F, Severinghaus JP, Hutterli MA, Nakazawa T, Aoki S, Jouzel J, Raymo ME, Matsumoto K, Nakata H, Motoyama H, Fujita S, Goto-Azuma K, Fujii Y, Watanabe O. Nature 2007;448(7156):912. doi:10.1038/nature06015.

  94. Paillard D. Quat Sci Rev 2015;107:11. doi:10.1016/j.quascirev.2014.10.002.

  95. Hansen J, Lacis A, Rind D, Russell G, Stone P, Fung I, Ruedy R, Lerner J. Geophys Monogr 1984;29. doi:10.1029/GM029p0130. (Amer. Geophys. Union.)

  96. de Boer B, Stocchi P, van de Wal RSW. Geosci Model Dev 2014;7(5):2141. doi:10.5194/gmd-7-2141-2014.

  97. Schmidt GA. J Quat Sci 2010;25(1):79. doi:10.1002/jqs.1314.

  98. Haywood AM, Dowsett HJ, Dolan AM. Nature Commun 2016;7:10646. doi:10.1038/ncomms10646.

  99. Lenton TM, Livina VN, Dakos V, van Nes EH, Scheffer M. Philos Trans R Soc A Math Phys Eng Sci 2012;370(1962):1185. doi:10.1098/rsta.2011.0304.

  100. Mudelsee M, Bickert T, Lear CH, Lohmann G. Rev Geophys 2014;52(3):333. doi:10.1002/2013RG000440.

  101. van der Mheen M, Dijkstra HA, Gozolchiani A, den Toom M, Feng Q, Kurths J, Hernandez-Garcia E. Geophys Res Lett 2013;40(11):2714. doi:10.1002/grl.50515.

  102. Huber M, Caballero R. Clim Past 2011;7(2):603. doi:10.5194/cp-7-603-2011.

  103. Jaramillo C, Ochoa D, Contreras L, Pagani M, Carvajal-Ortiz H, Pratt LM, Krishnan S, Cardona A, Romero M, Quiroz L, Rodriguez G, Rueda MJ, de la Parra F, Moron S, Green W, Bayona G, Montes C, Quintero O, Ramirez R, Mora G, Schouten S, Bermudez H, Navarrete R, Parra F, Alvaran M, Osorno J, Crowley JL, Valencia V, Vervoort J. Science 2010;330(6006):957. doi:10.1126/science.1193833.

  104. Zhou J, Poulsen CJ, Rosenbloom N, Shields C, Briegleb B. Clim Past 2012;8(2):565. doi:10.5194/cp-8-565-2012.

  105. Abbot DS, Huber M, Bousquet G, Walker CC. Geophys Res Lett 2009;36:L05702. doi:10.1029/2008GL036703.

  106. Masson-Delmotte V, Kageyama M, Braconnot P, Charbit S, Krinner G, Ritz C, Guilyardi E, Jouzel J, Abe-Ouchi A, Crucifix M, Gladstone RM, Hewitt CD, Kitoh A, LeGrande AN, Marti O, Merkel U, Ohgaito TMR, Otto-Bliesner B, Peltier WR, Ross I, Valdes PJ, Vettoretti G, Weber SL, Wolk F, YU Y. Clim Dyn 2006;26(5):513. doi:10.1007/s00382-005-0081-9.

  107. Singarayer JS, Valdes PJ. Quat Sci Rev 2010;29(1-2):43. doi:10.1016/j.quascirev.2009.10.011.

  108. Tziperman E, Stone L, Cane M, Jarosh H. Science 1994;264:72.

    CAS  Article  Google Scholar 

  109. Jin FF, Neelin J, Ghil M. Physica D: Nonlinear Phenomena 1996;98(442):2–4. doi:10.1016/0167-2789(96)00111-X.

  110. Fedorov AV, Philander SG. Science 2000;288(5473):1997. doi:10.1126/science.288.5473.1997.

  111. Collins M. Clim Dyn 2005;24:89. doi:10.1007/s00382-004-0478-x.

  112. Chekroun MD, Simonnet E, Ghil M. Physica D: Nonlinear Phenomena 2011;240(21):1685. doi:

Download references


This work arose from a workshop on Mathematical approaches to palaeo-climate sensitivity held in Utrecht in November 2015. We thank the Netherlands Earth System Science Centre (NESSC), financially supported by the Ministry of Education, Culture and Science (OCW), grant no. 024.002.001, for financial support to the workshop. MG’s work is partially supported by grant N00014-16-1-2073 from the Multidisciplinary University Research Initiative (MURI) of the Office of Naval Research and by the US National Science Foundation grant OCE 1243175. A.M.H. acknowledges that this review was completed in receipt of funding from the European Research Council under the European Union’s Seventh Framework Programme (FP7/2007-2013)/ERC grant agreement no. 278636. GL received funding by Helmholtz through PACES and REKLIM. A. M. acknowledges funding by the National Science Foundation (NSF) award #1536454. HP acknowledges ERC funding under contract no. 617462. DS acknowledges funding from the People Programme (Marie Curie Actions) of the European Unions Seventh Framework Programme FP7/2007-2013/ under REA Grant Agreement No. 290201 MEDGATE.

Author information

Authors and Affiliations


Corresponding author

Correspondence to Anna S. von der Heydt.

Ethics declarations

Conflict of Interest

On behalf of all authors, the corresponding author states that there is no conflict of interest.

Additional information

Human and Animal Rights and Informed Consent

This article does not contain any studies with human or animal subjects performed by any of the authors.

This article is part of the Topical Collection on Constraints on Climate Sensitivity

This work arose from a workshop on Mathematical approaches to palaeo-climate sensitivity in November 2015. A.v.d.H., H.D., and R.v.d.W. initiated the workshop and led the drafting of this study together with R.C., M.C., M.H., P. K., G.F., E.R., and P.V. The other authors contributed specialist insights, discussions and feedback.

Rights and permissions

Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (, which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.

Reprints and Permissions

About this article

Verify currency and authenticity via CrossMark

Cite this article

von der Heydt, A.S., Dijkstra, H.A., van de Wal, R.S.W. et al. Lessons on Climate Sensitivity From Past Climate Changes. Curr Clim Change Rep 2, 148–158 (2016).

Download citation

  • Published:

  • Issue Date:

  • DOI:


  • Climate sensitivity
  • Palaeoclimate
  • Climate tipping points