Abstract

Time-dependent processes are often analysed using the power spectral density (PSD), calculated by taking an appropriate Fourier transform of individual trajectories and finding the associated ensemble-average. Frequently, the available experimental data sets are too small for such ensemble averages, and hence it is of a great conceptual and practical importance to understand to which extent relevant information can be gained from $S(f,T)$, the PSD of a single trajectory. Here we focus on the behavior of this random, realization-dependent variable, parametrized by frequency $f$ and observation-time $T$, for a broad family of anomalous diffusions---fractional Brownian motion (fBm) with Hurst-index $H$---and derive exactly its probability density function. We show that $S(f,T)$ is proportional---up to a random numerical factor whose universal distribution we determine---to the ensemble-averaged PSD. For subdiffusion ($H<1/2$) we find that $S(f,T)\sim A/f^{2H+1}$ with random-amplitude $A$. In sharp contrast, for superdiffusion $(H>1/2)$ $S(f,T)\sim BT^{2H-1}/f^2$ with random amplitude $B$. Remarkably, for $H>1/2$ the PSD exhibits the same frequency-dependence as Brownian motion, a deceptive property that may lead to false conclusions when interpreting experimental data. Notably, for $H>1/2$ the PSD is ageing and is dependent on $T$. Our predictions for both sub- and superdiffusion are confirmed by experiments in live cells and in agarose hydrogels, and by extensive simulations.

Highlights

  • The power spectral density of any time-dependent process Xt is a fundamental feature of its spectral content, dynamical behavior, and temporal correlations [1]

  • We focus on the behavior of this random, realization-dependent variable parametrized by frequency f and observation time T, for a broad family of anomalous diffusions—fractional Brownian motion with Hurst index H—and derive exactly its probability density function

  • One expects that for an arbitrary realization of the process, a single-trajectory power spectral density (PSD) should exhibit the same large-f dependence as a traditional ensembleaveraged PSD. (ii) Our experiments and numerical simulations impressively evidence that this 1=fβ dependence is observed for both super- and subdiffusive fractional Brownian motion (FBM)-type processes

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Summary

INTRODUCTION

The power spectral density of any time-dependent process Xt is a fundamental feature of its spectral content, dynamical behavior, and temporal correlations [1]. In a recent work [23] (see the perspective [24]), it was proven that for standard Brownian motion, the single-trajectory PSD Sðf; TÞ in the large-f limit and at finite T exhibits the same f dependence as its traditional ensemble-average counterpart. This mathematical prediction was fully corroborated by numerical simulations and experiments with polystyrene beads in aqueous solution [23]. VI, we present a brief summary of our results and a perspective

FRACTIONAL BROWNIAN MOTION AND ITS POWER SPECTRAL DENSITIES
Agarose hydrogel
Telomeres
Amoeba and intracellular vacuoles
Mean-squared displacement
PSD analysis
Numerical algorithms
ANALYTICAL PREDICTIONS
COMPARISON WITH EXPERIMENTAL AND NUMERICAL DATA
DISCUSSION
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