2005
DOI: 10.1063/1.2116320
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Hamiltonian multivector fields and Poisson forms in multisymplectic field theory

Abstract: We present a general classification of Hamiltonian multivector fields and of Poisson forms on the extended multiphase space appearing in the geometric formulation of first order classical field theories. This is a prerequisite for computing explicit expressions for the Poisson bracket between two Poisson forms.

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Cited by 35 publications
(67 citation statements)
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“…41); alternatively, note that D M is of the form described in Theorem IV.4 and hence automatically determines a (multi-)Dirac structure. Now, let X : M → T Z be a partial vector field as in (18). In local coordinates, we have…”
Section: B Electromagnetismmentioning
confidence: 99%
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“…41); alternatively, note that D M is of the form described in Theorem IV.4 and hence automatically determines a (multi-)Dirac structure. Now, let X : M → T Z be a partial vector field as in (18). In local coordinates, we have…”
Section: B Electromagnetismmentioning
confidence: 99%
“…To see why the previous theorem implies energy conservation, decompose the multivector field X as in (18). Using Lemma A.2, the interior product can then be written as…”
Section: Theorem 46: For Any Lagrange-dirac System (X E D N+1 ) mentioning
confidence: 99%
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