Abstract

We directly exploit the stochasticity of the internal variability, and the linearity of the forced response to make global temperature projections based on historical data and a Green’s function, or Climate Response Function (CRF). To make the problem tractable, we take advantage of the temporal scaling symmetry to define a scaling CRF characterized by the scaling exponent H, which controls the long-range memory of the climate, i.e. how fast the system tends toward a steady-state, and an inner scale tau approx 2 years below which the higher-frequency response is smoothed out. An aerosol scaling factor and a non-linear volcanic damping exponent were introduced to account for the large uncertainty in these forcings. We estimate the model and forcing parameters by Bayesian inference which allows us to analytically calculate the transient climate response and the equilibrium climate sensitivity as: 1.7^{+0.3} _{-0.2} K and 2.4^{+1.3} _{-0.6} K respectively (likely range). Projections to 2100 according to the RCP 2.6, 4.5 and 8.5 scenarios yield warmings with respect to 1880–1910 of: 1.5^{+0.4}_{-0.2}K, 2.3^{+0.7}_{-0.5} K and 4.2^{+1.3}_{-0.9} K. These projection estimates are lower than the ones based on a Coupled Model Intercomparison Project phase 5 multi-model ensemble; more importantly, their uncertainties are smaller and only depend on historical temperature and forcing series. The key uncertainty is due to aerosol forcings; we find a modern (2005) forcing value of [-1.0, -0.3], ,,mathrm{Wm} ^{-2} (90 % confidence interval) with median at -0.7 ,,mathrm{Wm} ^{-2}. Projecting to 2100, we find that to keep the warming below 1.5 K, future emissions must undergo cuts similar to RCP 2.6 for which the probability to remain under 1.5 K is 48 %. RCP 4.5 and RCP 8.5-like futures overshoot with very high probability.

Highlights

  • The atmosphere is a complex system involving turbulent processes operating over a wide range of scales starting from millimeters at the Kolmogorov dissipation scale up to the size of the Earth, spanning over 10 orders of magnitudes in space

  • An approach related to the scaling Climate Response Function (CRF) we develop below is that of Procyk et al (2020) which is based on the Earth energy balance

  • Using Bayes’ theorem as described above, we derived a PDF for the parameters of the scaling CRF (SCRF) from the mean likelihood of the five observational datasets available: HadCRUTv4, Cowtan & Way (C&W), GISS Surface Temperature Analysis (GISTEMP), NOAAGlobalTemp and Berkeley Earth Surface Temperature (BEST)

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Summary

Introduction

The atmosphere is a complex system involving turbulent processes operating over a wide range of scales starting from millimeters at the Kolmogorov dissipation scale up to the size of the Earth, spanning over 10 orders of magnitudes in space. For planetary scale structures in the atmosphere, the overall deterministic prediction limit of about 10 days corresponds to the scaling transition timescale w from the weather regime to the macroweather regime (Lovejoy and Schertzer 2013a). The atmospheric components of GCMs exhibit the same weather-macroweather scaling transition as the atmosphere and similar predictability limits. Beyond this horizon, the internal variability has to be interpreted stochastically so that a single GCM run is only one realization of the random. The mean of the MME is taken to obtain the deterministic forced component of temperature variability and average out the internal variability (Collins et al 2013)

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