Abstract

Complex systems often involve random fluctuations for which self-similar properties in space and time play an important role. Fractional Brownian motions, characterized by a single scaling exponent, the Hurst exponent H, provide a convenient tool to construct synthetic signals that capture the statistical properties of many processes in the physical sciences and beyond. However, in certain strongly interacting systems, e.g., turbulent flows, stock market indices, or cardiac interbeats, multiscale interactions lead to significant deviations from self-similarity and may therefore require a more elaborate description. In the context of turbulence, the Kolmogorov–Oboukhov model (K62) describes anomalous scaling, albeit explicit constructions of a turbulent signal by this model are not available yet. Here, we derive an explicit formula for the joint multipoint probability density function of a multifractal field. To this end, we consider a scale mixture of fractional Ornstein–Uhlenbeck processes and introduce a fluctuating length scale in the corresponding covariance function. In deriving the complete statistical properties of the field, we are able to systematically model synthetic multifractal phenomena. We conclude by giving a brief outlook on potential applications which range from specific tailoring or stochastic interpolation of wind fields to the modeling of financial data or non-Gaussian features in geophysical or geospatial settings.

Highlights

  • The theory of fractals has provided a unifying view on processes that occur in complex systems [1]

  • It is convenient to describe fluctuating time series or spatial fields as fractional Brownian motion where the roughness of the signal is determined by a single scaling exponent, the Hurst exponent H [10,11,12]

  • We introduce here an explicit construction of the joint multipoint probability density function (PDF) (1) with multifractal scaling that belongs to the class of the Kolmogorov-Oboukhov (K62) model of turbulence [44, 45]

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Summary

INTRODUCTION

The theory of fractals has provided a unifying view on processes that occur in complex systems [1]. The method is based on an ensemble of fractional Ornstein-Uhlenbeck processes which have been modified by the introduction of fluctuating length scales It can be considered as a multipoint generalization of the two-point statistics proposed by Kolmogorov and Oboukhov [44, 45]. II discusses the ensemble of fractional Ornstein-Uhlenbeck processes and derives their respective correlation functions It is shown through the example of a turbulent velocity field that a lognormal distribution of the fluctuating scale parameters reproduces the KomogorovOboukhov scaling of turbulence. By virtue of these three step process, we introduce strong correlations which culminate in the non-Gaussian statistics of field increments (17) This will be further elaborated upon, where we derive the main result of this paper, i.e., the multipoint statistics of the Kolmogorov-Oboukhov-type velocity field

MULTIPOINT STATISTICS OF THE GAUSSIAN SCALE MIXTURE
Single-point statistical quantities
Two-point statistical quantities
Three-point statistical quantities
OUTLOOK
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