Abstract

We use a piecewise-linear, discontinuous Galerkin method for the time discretization of a fractional diffusion equation involving a parameter in the range ??1?<???<?0. Our analysis shows that, for a time interval (0,T) and a spatial domain ?, the error in $L_\infty\bigr((0,T);L_2(\Omega)\bigr)$ is of order k 2?+?? , where k denotes the maximum time step. Since derivatives of the solution may be singular at t?=?0, our result requires the use of non-uniform time steps. In the limiting case ??=?0 we recover the known O(k 2) convergence for the classical diffusion (heat) equation. We also consider a fully-discrete scheme that employs standard (continuous) piecewise-linear finite elements in space, and show that the additional error is of order h 2log(1/k). Numerical experiments indicate that our O(k 2?+?? ) error bound is pessimistic. In practice, we observe O(k 2) convergence even for ? close to ??1.

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