2018
DOI: 10.1103/physrevlett.120.104501
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Exact Results for the Nonergodicity of d -Dimensional Generalized Lévy Walks

Abstract: We provide analytical results for the ensemble-averaged and time-averaged squared displacement, and the randomness of the latter, in the full two-dimensional parameter space of the d-dimensional generalized Lévy walk introduced by Shlesinger et al. [Phys. Rev. Lett. 58, 1100 (1987)PRLTAO0031-900710.1103/PhysRevLett.58.1100]. In certain regions of the parameter plane, we obtain surprising results such as the divergence of the mean-squared displacements, the divergence of the ergodicity breaking parameter despit… Show more

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Cited by 42 publications
(55 citation statements)
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“…There the mean squared displacement is equal to the second derivative of the spatial distribution of the process. Results are known for processes of with PDFs of the form of equation (10) for Levy flights [25] and Levy walks [26]. The results in both cases are the same and therefore independent of the exact path the system takes during each waiting time.…”
Section: Model and Its Diffusive Behaviormentioning
confidence: 99%
“…There the mean squared displacement is equal to the second derivative of the spatial distribution of the process. Results are known for processes of with PDFs of the form of equation (10) for Levy flights [25] and Levy walks [26]. The results in both cases are the same and therefore independent of the exact path the system takes during each waiting time.…”
Section: Model and Its Diffusive Behaviormentioning
confidence: 99%
“…For long times, in the former case, the particles spread like Richardson-Obukhov diffusion in turbulence, where the velocity follows a simple Brownian motion [34,35]. The Richardson-Obukhov diffusion is also discussed in recent papers on the diffusion of cold atoms in optical lattices [19,20] and the d-dimensional generalized Lévy walk [36]. In the latter case, the particle motion is like Lévy walk [37][38][39][40] of the sub-ballistic superdiffusion regime.…”
Section: Introductionmentioning
confidence: 99%
“…Jump lengths and waiting times may be coupled linearly, such that the resulting LW moves in a given direction with a constant speed until velocity reversal after a given waiting time, the velocity model [43], or the space-time coupling may have a power-law type [40]. The velocity may also be considered to change from one step to another [44,45]. Interestingly, for certain parameters even Lévy walks have an infinite variance, namely, when there is a distribution of velocities associated with different path lengths [45].…”
Section: Introductionmentioning
confidence: 99%
“…The velocity may also be considered to change from one step to another [44,45]. Interestingly, for certain parameters even Lévy walks have an infinite variance, namely, when there is a distribution of velocities associated with different path lengths [45]. LFs and LWs are non-ergodic in the sense that long time and ensemble averages of physical observables are different [19,20,[45][46][47][48][49].…”
Section: Introductionmentioning
confidence: 99%
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