Abstract

A novel method for measuring distances between statistical states as represented by probability distribution functions (PDF) has been proposed, namely the information length. The information length enables the computation of the total number of statistically different states that a system evolves through in time. Anomalous transport can presumably be modeled fractional velocity derivatives and Langevin dynamics in a Fractional Fokker–Planck (FFP) approach. The numerical solutions or PDFs are found for varying degree of fractionality ( α ) of the stable Lévy distribution as solutions to the FFP equation. Specifically, the information length of time-dependent PDFs for a given fractional index α is computed.

Highlights

  • Anomalous transport processes is ubiquitus in many different fields where a diffusive description is improper

  • The fluctuations under such plasma conditions are often distributed according to Lévy statistics in contrast to the Gaussian charactistics as was displayed in [17]. the turbulence induced fluxes at the edge of the W7-AS stellarator where shown to have probability density functions (PDFs) with power law characteristics most often it is expected that Gaussian statistics dominate, which induces exponentially decaying tails of the distributions

  • The objective of the present paper is to explore the information length concept pertaining to time-dependent solutions of the fractional Fokker–Planck (FFP) equation resulting from a Langevin description driven by Lévy stochastic force. the present work is based on previous efforts reported in Anderson et al [35,36,37] and may provide new insights on the recent developments in the understanding of the anomalous transport and turbulent processes

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Summary

Introduction

Anomalous transport processes is ubiquitus in many different fields where a diffusive description is improper. In the gradient region or in the scrape-off layer (SOL), the thermal and particle fluxes can be dominated by coherent structures such as (blobs) [1,2,3,4,5,6,7,8] which inherently possess a non-local character [9,10,11,12,13,14,15,16] The fluctuations under such plasma conditions are often distributed according to Lévy statistics in contrast to the Gaussian charactistics as was displayed in [17].

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