Abstract
We adopt a procedure of operational-umbral type to solve the (1 + 1)-dimensional fractional Fokker-Planck equation in which time fractional derivative of order α (0 < α < 1) is in the Riemann-Liouville sense. The technique we propose merges well documented operational methods to solve ordinary FP equation and a redefinition of the time by means of an umbral operator. We show that the proposed method allows significant progress including the handling of operator ordering.
Acknowledgments
The authors thanks Prof. Andrzej Horzela and Dr. Silvia Liccardi for helpful discussion and suggestions.
K.G and A.L. were supported by the NCN, OPUS-12, Program No. UMO-2016/23/B/ST3/01714. Moreover, K.G. thanks for support from MNiSW (Poland), Iuventus Plus 2015-2016, Program No. IP2014 013073.
References
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Appendix A. Proof of Eq. (5.10)
Let us recall
in which we take λ = τ and
The use of example (2) enable us to obtain Eq. (7.2) as the left hand site of Eq. (5.10) times eτ.
Observe that the solution (7.2) satisfies the partial differential equation in the form
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- Editorial Note
- FCAA related news, events and books (FCAA–volume 21–1–2018)
- Survey Paper
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- Survey Paper
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