Tempered stable Lévy motion and transient super-diffusion
The space-fractional diffusion equation models anomalous super-diffusion. Its solutions are transition densities of a stable Lévy motion, representing the accumulation of power-law jumps. The tempered stable Lévy motion uses exponential tempering to cool these jumps. A tempered fractional diffusion...
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          | Published in | Journal of computational and applied mathematics Vol. 233; no. 10; pp. 2438 - 2448 | 
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| Main Authors | , | 
| Format | Journal Article | 
| Language | English | 
| Published | 
        Kidlington
          Elsevier B.V
    
        15.03.2010
     Elsevier  | 
| Subjects | |
| Online Access | Get full text | 
| ISSN | 0377-0427 1879-1778  | 
| DOI | 10.1016/j.cam.2009.10.027 | 
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| Summary: | The space-fractional diffusion equation models anomalous super-diffusion. Its solutions are transition densities of a stable Lévy motion, representing the accumulation of power-law jumps. The tempered stable Lévy motion uses exponential tempering to cool these jumps. A tempered fractional diffusion equation governs the transition densities, which progress from super-diffusive early-time to diffusive late-time behavior. This article provides finite difference and particle tracking methods for solving the tempered fractional diffusion equation with drift. A temporal and spatial second-order Crank–Nicolson method is developed, based on a finite difference formula for tempered fractional derivatives. A new exponential rejection method for simulating tempered Lévy stables is presented to facilitate particle tracking codes. | 
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| ISSN: | 0377-0427 1879-1778  | 
| DOI: | 10.1016/j.cam.2009.10.027 |