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An exact local error representation of exponential operator splitting methods for evolutionary problems and applications to linear Schrödinger equations in the semi-classical regime.

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Academic year: 2021

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Fig. 5.1 Numerical solution |ψ(x, 0.64)| of the linear Schrödinger equation (5.13) for two different values of the critical parameter ε.
Table 5.1 Dependence on the critical parameter. Global error and ratio for the Lie-splitting method (top, p = 1), the Strang-splitting method (middle, p = 2), and the splitting method by Yoshida (bottom, p = 4).

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