Abstract

Abstract. We consider the statistical properties of solutions of the stochastic fractional relaxation equation and its fractionally integrated extensions that are models for the Earth's energy balance. In these equations, the highest-order derivative term is fractional, and it models the energy storage processes that are scaling over a wide range. When driven stochastically, the system is a fractional Langevin equation (FLE) that has been considered in the context of random walks where it yields highly nonstationary behaviour. An important difference with the usual applications is that we instead consider the stationary solutions of the Weyl fractional relaxation equations whose domain is −∞ to t rather than 0 to t. An additional key difference is that, unlike the (usual) FLEs – where the highest-order term is of integer order and the fractional term represents a scaling damping – in the fractional relaxation equation, the fractional term is of the highest order. When its order is less than 1/2 (this is the main empirically relevant range), the solutions are noises (generalized functions) whose high-frequency limits are fractional Gaussian noises (fGn). In order to yield physical processes, they must be smoothed, and this is conveniently done by considering their integrals. Whereas the basic processes are (stationary) fractional relaxation noises (fRn), their integrals are (nonstationary) fractional relaxation motions (fRm) that generalize both fractional Brownian motion (fBm) as well as Ornstein–Uhlenbeck processes. Since these processes are Gaussian, their properties are determined by their second-order statistics; using Fourier and Laplace techniques, we analytically develop corresponding power series expansions for fRn and fRm and their fractionally integrated extensions needed to model energy storage processes. We show extensive analytic and numerical results on the autocorrelation functions, Haar fluctuations and spectra. We display sample realizations. Finally, we discuss the predictability of these processes which – due to long memories – is a past value problem, not an initial value problem (that is used for example in highly skillful monthly and seasonal temperature forecasts). We develop an analytic formula for the fRn forecast skills and compare it to fGn skill. The large-scale white noise and fGn limits are attained in a slow power law manner so that when the temporal resolution of the series is small compared to the relaxation time (of the order of a few years on the Earth), fRn and its extensions can mimic a long memory process with a range of exponents wider than possible with fGn or fBm. We discuss the implications for monthly, seasonal, and annual forecasts of the Earth's temperature as well as for projecting the temperature to 2050 and 2100.

Highlights

  • Over the last decades, stochastic approaches have rapidly developed and have spread throughout the geosciences

  • Whereas the basic processes are fractional relaxation noises, their integrals are fractional relaxation motions that generalize both fractional Brownian motion as well as Ornstein–Uhlenbeck processes. Since these processes are Gaussian, their properties are determined by their second-order statistics; using Fourier and Laplace techniques, we analytically develop corresponding power series expansions for fRn and fRm and their fractionally integrated extensions needed to model energy storage processes

  • We develop an analytic formula for the fRn forecast skills and compare it to fractional Gaussian noise (fGn) skill

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Summary

Introduction

Stochastic approaches have rapidly developed and have spread throughout the geosciences. The FEBE determines the Earth’s global temperature when the energy storage processes are scaling and modelled by a fractional time-derivative term. Whereas the EBE is integerordered and describes the deterministic, exponential relaxation of the Earth’s temperature to equilibrium, the FEBE is of fractional order, and because it is both deterministic and stochastic, it unites all the forcings and responses into a single model. We have mentioned that the FEBE can be derived phenomenologically where the fractional derivative of order h term represents the energy storage processes (Lovejoy et al, 2021) In this approach order h is an empirically determined parameter with h = 1 corresponding to the classical (exponential) exception. We could note that the paper is somewhat complex due to the necessity of developing several approaches: Fourier for the main integral representations (Sect. 2), Laplace for the asymptotic expansions (Sect. 3), and real space for the predictability results (Sect. 4)

The fractional relaxation equation
Green’s functions
The α-order fractionally integrated fRn and fRm processes
Statistics
Finite-resolution processes
Asymptotic expansions
Haar fluctuations
Sample processes
Prediction
Conclusions
Power series expansions about the origin
Findings
A convenient approximation
Full Text
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