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Random walks with feedback on fractal lattices
Beatrix M Schulz1, Michael Schulz, Steffen Trimper
1Abteilung Theoretische Physik, Universität Ulm, D-89069 Ulm, Germany. beatrix.schulz@physik.uni-ulm.de
Summary
This study explores random walks on fractal lattices with self-organized feedback. Repulsive feedback causes superdiffusion, while attractive feedback leads to localization, altering the dynamical exponent.
Area of Science:
- Complex Systems
- Statistical Physics
- Dynamical Processes
Background:
- Fractal lattices inherently promote subdiffusive random walk behavior.
- Self-organized feedback coupling introduces attractive (lambda>0) or repulsive (lambda<0) dynamics.
- The interplay between fractal geometry and feedback dictates particle transport.
Purpose of the Study:
- To numerically investigate random walk dynamics on fractal lattices with self-organized feedback.
- To analyze how feedback strength (lambda) influences subdiffusion, superdiffusion, and localization.
- To determine the effect of combined fractal and feedback processes on the dynamical exponent (z).
Main Methods:
- Numerical simulations of random walks on fractal lattices (Sierpinski gasket, Sierpinski carpet).
- Introduction of a self-organized feedback coupling with variable strength (lambda).
- Analysis of transport properties and calculation of the dynamical exponent (z) using scaling arguments.
Main Results:
- Repulsive feedback coupling on Sierpinski gaskets and carpets leads to superdiffusion (2/z=1.04 and 2/z=1.08, respectively).
- Attractive feedback coupling results in particle localization, similar to random walks on regular lattices.
- The dynamical exponent (z) is significantly modified by the competitive feedback and fractal structure.
Conclusions:
- The competition between fractal subdiffusion and feedback dynamics determines the overall transport behavior.
- Attractive feedback can induce localization, overriding the subdiffusive tendency of fractal lattices.
- Numerical findings are robustly supported by analytical scaling arguments.