Nonergodicity of $d$-dimensional generalized L\'evy walks and their relation to other space-time coupled models
Tony Albers, G\"unter Radons

TL;DR
This paper analyzes the nonergodic behavior of generalized Lévy walks, revealing divergence in mean-squared displacements, contrasting ensemble and individual trajectory diffusion, and introducing a broader model to connect various space-time coupled processes.
Contribution
The study provides detailed analytical insights into the nonergodicity of generalized Lévy walks and introduces a variable speed model linking multiple space-time coupled anomalous diffusion models.
Findings
Mean-squared displacements can diverge for certain parameters.
Individual trajectories can show superdiffusion while ensemble spreads subdiffusively.
Time-averaged squared displacement fluctuations can diverge, indicating infinitely strong ergodicity breaking.
Abstract
We investigate the nonergodicity of the generalized L\'evy walk introduced by Shlesinger et al. [Phys. Rev. Lett. 58, 1100 (1987)] with respect to the squared displacements. We present detailed analytical derivations of our previous findings outlined in a recent Letter [Phys. Rev. Lett. 120, 104501 (2018)], give profound interpretations, and especially emphasize three surprising results: First, we find that the mean-squared displacements can diverge for a certain range of parameter values. Second, we show that an ensemble of trajectories can spread subdiffusively, whereas individual time-averaged squared displacements show superdiffusion. Third, we recognize that the fluctuations of the time-averaged squared displacements can become so large that the ergodicity breaking parameter diverges, what we call infinitely strong ergodicity breaking. The latter phenomenon can also occur for…
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