On the relation between a fluctuating diffusion equation and long time tails in stationary random media

1986 ◽  
Vol 42 (5-6) ◽  
pp. 935-940 ◽  
Author(s):  
Alan K. Harrison ◽  
Robert Zwanzig
1984 ◽  
Vol 35 (3-4) ◽  
pp. 413-442 ◽  
Author(s):  
J. Machta ◽  
M. H. Ernst ◽  
H. van Beijeren ◽  
J. R. Dorfman

1984 ◽  
Vol 34 (3-4) ◽  
pp. 477-495 ◽  
Author(s):  
M. H. Ernst ◽  
J. Machta ◽  
J. R. Dorfman ◽  
H. van Beijeren

1976 ◽  
Vol 55 (7) ◽  
pp. 391-392 ◽  
Author(s):  
J.P. Boon ◽  
A. Bouiller

2013 ◽  
Vol 10 (02) ◽  
pp. 1341001 ◽  
Author(s):  
LEEVAN LING ◽  
MASAHIRO YAMAMOTO

We consider the solutions of a space–time fractional diffusion equation on the interval [-1, 1]. The equation is obtained from the standard diffusion equation by replacing the second-order space derivative by a Riemann–Liouville fractional derivative of order between one and two, and the first-order time derivative by a Caputo fractional derivative of order between zero and one. As the fundamental solution of this fractional equation is unknown (if exists), an eigenfunction approach is applied to obtain approximate fundamental solutions which are then used to solve the space–time fractional diffusion equation with initial and boundary values. Numerical results are presented to demonstrate the effectiveness of the proposed method in long time simulations.


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