2013
DOI: 10.1016/j.geomphys.2013.08.009
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Lifting geometric objects to the dual of the first jet bundle of a bundle fibred over R

Abstract: Abstract. We study natural lifting operations from a bundle τ : E → R to the bundle π : J 1 τ * → E which is the dual of the first-jet bundle J 1 τ . The main purpose is to define a complete lift of a type (1, 1) tensor field on E and to understand all features of its construction. Various other lifting operations of tensorial objects on E are needed for that purpose. We prove that the complete lift of a type (1, 1) tensor with vanishing Nijenhuis torsion gives rise to a Poisson-Nijenhuis structure on J 1 τ * … Show more

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Cited by 5 publications
(14 citation statements)
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“…One is the symmetry property referred to above (which equally holds for the projected Poisson structure on J 1 τ * ). A second one is the vanishing of the so-called Magri-Morosi concommitant; this was proved to be the case in detail on J 1 τ * in [25] and the proof for T * E can be found in [12]. The last condition is the vanishing of the Nijenhuis torsion, so that the statement then immediately follows from the preceding theorem.…”
Section: Introductionmentioning
confidence: 82%
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“…One is the symmetry property referred to above (which equally holds for the projected Poisson structure on J 1 τ * ). A second one is the vanishing of the so-called Magri-Morosi concommitant; this was proved to be the case in detail on J 1 τ * in [25] and the proof for T * E can be found in [12]. The last condition is the vanishing of the Nijenhuis torsion, so that the statement then immediately follows from the preceding theorem.…”
Section: Introductionmentioning
confidence: 82%
“…the induced transformation of a time-dependent point transformation on E, which as such will not destroy the coordinate form of the Poisson tensor. We have proved in detail in [25] that this can be done for the Poisson-Nijenhuis structure (P, R) on J 1 τ * , and it is an easy matter to verify that the same point transformation on E will also induce a canonical transformation on T * E that does the job. Note further that in the course of proving the existence of an appropriate transformation (t, q) → (t, Q(t, q)) on E, we found that each eigenvalue λ i will in the new coordinates at most depend on the corresponding coordinate Q i .…”
Section: Introductionmentioning
confidence: 91%
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“…1 Different authors use various appellations for Y, or for its associated bundle manifold: the covariant phase space bundle, the doubly extended phase space, the extended dual bundle [9], orthe extended multimomentum bundle [7] ...…”
Section: Hamiltonian Dynamicsmentioning
confidence: 99%