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We study two schemes for a time-fractional Fokker--Planck equation with space- and time-dependent forcing in one space dimension. The first scheme is continuous in time and discretized in space using a piecewise-linear Galerkin finite element method. The second is continuous in space and employs a time-stepping procedure similar to the classical implicit Euler method. We show that the space discretization is second-order accurate in the spatial L₂-norm, uniformly in time, whereas the corresponding error for the time-stepping scheme is O(k^α) for a uniform time step k, where α∈(1/2,1) is the fractional diffusion parameter. In numerical experiments using a combined, fully discrete method, we observe convergence behavior consistent with these results.
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Le et al. (2016) studied this question.
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