35 research outputs found

    Finite-velocity diffusion on a comb

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    A Cattaneo equation for a comb structure is considered. We present a rigorous analysis of the obtained fractional diffusion equation, and corresponding solutions for the probability distribution function are obtained in the form of the Fox HH-function and its infinite series. The mean square displacement along the backbone is obtained as well in terms of the infinite series of the Fox HH-function. The obtained solutions describe the transition from normal diffusion to subdiffusion, which results from the comb geometry.Comment: 7 page

    Anomalous diffusion on a fractal mesh

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    An exact analytical analysis of anomalous diffusion on a fractal mesh is presented. The fractal mesh structure is a direct product of two fractal sets which belong to a main branch of backbones and side branch of fingers. The fractal sets of both backbones and fingers are constructed on the entire (infinite) yy and xx axises. To this end we suggested a special algorithm of this special construction. The transport properties of the fractal mesh is studied, in particular, subdiffusion along the backbones is obtained with the dispersion relation ⟨x2(t)⟩∼tβ\langle x^2(t)\rangle\sim t^{\beta}, where the transport exponent β<1\beta<1 is determined by the fractal dimensions of both backbone and fingers. Superdiffusion with β>1\beta>1 has been observed as well when the environment is controlled by means of a memory kernel

    Heterogeneous diffusion in comb and fractal grid structures

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    We give an exact analytical results for diffusion with a power-law position dependent diffusion coefficient along the main channel (backbone) on a comb and grid comb structures. For the mean square displacement along the backbone of the comb we obtain behavior ⟨x2(t)⟩∼t1/(2−α)\langle x^2(t)\rangle\sim t^{1/(2-\alpha)}, where α\alpha is the power-law exponent of the position dependent diffusion coefficient D(x)∼∣x∣αD(x)\sim |x|^{\alpha}. Depending on the value of α\alpha we observe different regimes, from anomalous subdiffusion, superdiffusion, and hyperdiffusion. For the case of the fractal grid we observe the mean square displacement, which depends on the fractal dimension of the structure of the backbones, i.e., ⟨x2(t)⟩∼t(1+ν)/(2−α)\langle x^2(t)\rangle\sim t^{(1+\nu)/(2-\alpha)}, where 0<ν<10<\nu<1 is the fractal dimension of the backbones structure. The reduced probability distribution functions for both cases are obtained by help of the Fox HH-functions

    First encounters on Bethe Lattices and Cayley Trees

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    In this work we consider the first encounter problems between a fixed and/or mobile target A and a moving trap B on Bethe Lattices and Cayley trees. The survival probability (SP) of the target A on the both kinds of structures are analyzed analytically and compared. On Bethe Lattices, the results show that the fixed target will still prolong its survival time, whereas, on Cayley trees, there are some initial positions where the target should move to prolong its survival time. The mean first encounter time (MFET) for mobile target A is evaluated numerically and compared with the mean first passage time (MFPT) for the fixed target A. Different initial settings are addressed and clear boundaries are obtained. These findings are helpful for optimizing the strategy to prolong the survival time of the target or to speed up the search process on Cayley trees, in relation to the target's movement and the initial position configuration of the two walkers. We also present a new method, which uses a small amount of memory, for simulating random walks on Cayley trees.Comment: 25 pages, 11 figure
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