Fractional diffusion for Fokker-Planck equation with heavy tail equilibrium: an à la Koch spectral method in any dimension

Abstract

In this paper, we extend the spectral method developed [Dechicha and Puel, 2023] to any dimension $d⩾1$, in order to construct an eigen-solution for the Fokker-Planck operator with heavy tail equilibria, of the form $(1+|v{|}^2{)}^{-\frac{\beta }{2}}$, in the range $\beta \in ]d,d+4[$. The method developed in dimension 1 was inspired by the work of H. Koch on nonlinear KdV equation [Koch, Nonlinearity, 2015]. The strategy in this paper is the same as in dimension 1 but the tools are different, since dimension 1 was based on ODE methods. As a direct consequence of our construction, we obtain the fractional diffusion limit for the kinetic Fokker-Planck equation, for the correct density $\rho :={\int }_{{\mathbb{R}}^d}f\mathrm{d}v$, with a fractional Laplacian $\kappa (-{\Delta }_x{)}^{\frac{\beta -d+2}{6}}$ and a positive diffusion coefficient $\kappa$.

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References in corpus (2)

• Self-similar solutions to super-critical gKdV
• Fractional diffusion for Fokker-Planck equation with heavy tail equilibrium: an à la Koch spectral method in any dimension

Cited by in corpus (1)

• Fractional diffusion for Fokker-Planck equation with heavy tail equilibrium: an à la Koch spectral method in any dimension