SDEs Driven by a Time-Changed Lévy Process and Their Associated Time-Fractional Order Pseudo-Differential Equations
By Marjorie G. Hahn, Kei Kobayashi, Sabir Umarov. 2009
54 citations recorded by the source corpus.
It is known that the transition probabilities of a solution to a classical Itô stochastic differential equation (SDE) satisfy in the weak sense the associated Kolmogorov equation. The Kolmogorov equation is a partial differential equation with coefficients determined by the corresponding SDE. Time-fractional Kolmogorov-type equations are used to model complex processes in many fields. However, the class of SDEs that is associated with these equations is unknown except in a few special cases. The present paper shows that in the cases of either time-fractional order or more general time-distributed order differential equations, the associated class of SDEs can be described within the framework of SDEs driven by semimartingales. These semimartingales are time-changed Lévy processes where the independent time-change is given respectively by the inverse of a single or mixture of independent stable subordinators. Examples are provided, including a fractional analogue of the Feynman–Kac formula.
Subfields: Applied Mathematics, Finance, Modeling and Simulation
View Paper: https://www.semanticscholar.org/paper/e43d2fb9367855fad777097c5c1504f0bd7c3bc2
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In Applied Mathematics
- Palaniappan Vellaisamy
- Erkan Nane
- Mark M. Meerschaert
- Kei Kobayashi
- Anatoly N. Kochubei
- Suleyman Ulusoy
- Arun Kumar
- Mohamed M. Khader
In Finance
In Modeling and Simulation
- Palaniappan Vellaisamy
- Kei Kobayashi
- Erkan Nane
- Mark M. Meerschaert
- Anatoly N. Kochubei
- Charles Tadjeran
- Fawang Liu
- Ian L Turner
Citations in the corpus
- Distributed-order fractional diffusions on bounded domains (2009, background): “[15] studied the time-fractional equation ∂u/∂t = Lu in this case, as well as the distributed-order extension.”
- Stochastic Calculus for a Time-Changed Semimartingale and the Associated Stochastic Differential Equations (2009, background): “of order β with respect to the time variable t (see [4]), and δx is the Dirac delta function with mass at x. For the proof, see Hahn, Kobayashi and Umarov [ 5, Theorem 4.1 ].”