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In this paper, we analyze an operator splitting scheme of the nonlinear heat equation in (): $\partial_t u = \Delta u + \lambda |u|^{p-1} u\Omega\times(0,\infty)u=0\partial\Omega\times(0,\infty)u ({\bf x},0) =\phi ({\bf x})\Omega$. where and $\phi \in W^{1,q}(\Omega)\cap L^{\infty} (\Omega)2\leq p < \inftyd(p-1)/2<q<\infty$. We establish the well-posedness of the approximation of in -space (), and furthermore, we derive its convergence rate of order for a time step . Finally, we give some numerical examples to confirm the reliability of the analyzed result.

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