2019
DOI: 10.1007/s00211-018-1015-x
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Non-satisfiability of a positivity condition for commutator-free exponential integrators of order higher than four

Abstract: We consider commutator-free exponential integrators as put forward in [Alverman, A., Fehske, H.: High-order commutator-free exponential time-propagation of driven quantum systems. J. Comput. Phys. 230, 5930-5956 (2011)]. For parabolic problems, it is important for the well-definedness that such an integrator satisfies a positivity condition such that essentially it only proceeds forward in time. We prove that this requirement implies maximal convergence order of four for real coefficients, which has been conje… Show more

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Cited by 4 publications
(10 citation statements)
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“…with coefficients a j,k given in Table 3. For these coefficients the positivity condition is not satisfied, in agreement with the fact that this cannot be the case for real coefficients, see [10]. For some applications, however, it is essential for stability reasons that this condition is satisfied.…”
Section: Th Order Commutator-free Magnus-type Integratorsmentioning
confidence: 73%
“…with coefficients a j,k given in Table 3. For these coefficients the positivity condition is not satisfied, in agreement with the fact that this cannot be the case for real coefficients, see [10]. For some applications, however, it is essential for stability reasons that this condition is satisfied.…”
Section: Th Order Commutator-free Magnus-type Integratorsmentioning
confidence: 73%
“…A proof of Theorem 2 was proposed in [7]. In Section 2 we will give a new independent proof by showing that Theorem 3 (and thus also Theorem 2) is an easy consequence of a recent result proved by the authors in [8].…”
Section: Theoremmentioning
confidence: 94%
“…2 Note that we have changed some denotations: H(t), H 0 , H 1 , s, a j , c j correspond respectively to the denotations A(t), A 0 , A 1 , J, b j , y j of [8].…”
Section: Proof Of Theoremmentioning
confidence: 99%
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