2014
DOI: 10.48550/arxiv.1410.2076
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Helmholtz theorem for Hamiltonian systems on time scales

Abstract: We derive the Helmholtz theorem for Hamiltonian systems defined on time scales in the context of nonshifted calculus of variations which encompass the discrete and continuous case. Precisely, we give a theorem characterizing first order equation on time scales, admitting a Hamiltonian formulation which is defined with non-shifted calculus of variation. Moreover, in the affirmative case, we give the associated Hamiltonian.

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Cited by 2 publications
(2 citation statements)
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“…Contrary to what happens in the Lagrangian case where technical difficulties related to the composition of operators seem to cancel such a generalization, the Hamiltonian case is possible due to its linear nature in the discrete differential operators. We refer to [13] for more details.…”
Section: Discussionmentioning
confidence: 99%
“…Contrary to what happens in the Lagrangian case where technical difficulties related to the composition of operators seem to cancel such a generalization, the Hamiltonian case is possible due to its linear nature in the discrete differential operators. We refer to [13] for more details.…”
Section: Discussionmentioning
confidence: 99%
“…For the Hamiltonian case it has been done for the discrete calculus of variations in [1] using the framework of [32] and in [20] using a discrete embedding procedure derived in [19]. In the case of time-scale calculus it has been done in [36]; for the Stratonovich stochastic calculus see [37].…”
Section: Introductionmentioning
confidence: 99%