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An invariant variational principle for Hamiltonian mechanics

Alexey V Golovnev1 and Alexander S Ushakov2

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It is shown that the action for Hamiltonian equations of motion can be brought into invariant symplectic form. In other words, it can be formulated directly in terms of the symplectic structure ω without any need to choose some 1-form γ, such that ω = dγ, which is not unique and does not even generally exist in a global sense.


PACS

45.20.Jj Lagrangian and Hamiltonian mechanics

45.10.Db Variational and optimization methods

MSC

70H05 Hamilton's equations

70G75 Variational methods

Subjects

Mathematical physics

Computational physics

Dates

Issue 23 (13 June 2008)

Received 12 January 2008, in final form 24 April 2008

Published 21 May 2008



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