Fokker-Planck and Kolmogorov backward equations for continuous time random walk scaling limits (Q2832839)
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scientific article; zbMATH DE number 6652875
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Fokker-Planck and Kolmogorov backward equations for continuous time random walk scaling limits |
scientific article; zbMATH DE number 6652875 |
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14 November 2016
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continuous-time random walk
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scaling limits
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Fokker-Planck equations
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Kolmogorov backward equations
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anomalous diffusion
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fractional kinetics
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fractional derivative
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subordination
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Skorokhod continuity
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Feller process
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transience
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coupled random walks
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0.8078704
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0.7985426
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0.7968248
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0.79005075
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Fokker-Planck and Kolmogorov backward equations for continuous time random walk scaling limits (English)
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The paper under review unifies the solutions of the Fokker-Planck equation and aims at understanding the distributions of scaling limits of continuous-time random walks (CTRWs) in terms of integro-differential equations.NEWLINENEWLINESection 2 uses results of [\textit{M. M. Meerschaert} and \textit{P. Straka}, Ann. Probab. 42, No. 4, 1699--1723 (2014; Zbl 1305.60089)] and exploits the Skorokhod continuity of the path mapping to obtain the CTRW scaling limit. With the transience in the time-component, the authors present Theorem 2.2 to characterise the distribution of \(X_t\) for Lebesgue almost every \(t\in \mathbb R\).NEWLINENEWLINESection 3 gives a projection of the semigroup in the proper Banach space framework. Section 4 gives an example of the Kolmogorov backward equation for CTRW limits.NEWLINENEWLINESection 5 shows that the probability law of the CTRW limit is a unique solution of the Fokker-Planck equation as long as the temporal Lévy measure is time-independent or the corresponding operator is invertible. Theorem 5.2 gives the Fokker-Planck equation for CTRW limits. Special cases of Fokker-Planck operators are also given.NEWLINENEWLINESection 6 is devoted to subdiffusions in a time-dependent potential and traps of spatially varying depth as well as space- and time-dependent Lévy walks, to further illustrate the results.
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