The Hamiltonian Tube Of A Cotangent-Lifted Action

Fuente: arXiv
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Main Authors: Rodriguez-Olmos, Miguel, Teixidó-Román, Miguel
Format: Preprint
Published: 2014
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author Rodriguez-Olmos, Miguel
Teixidó-Román, Miguel
author_facet Rodriguez-Olmos, Miguel
Teixidó-Román, Miguel
contents The Marle-Guillemin-Sternberg (MGS) form is local model for a neighborhood of an orbit of a Hamiltonian Lie group action on a symplectic manifold. One of the main features of the MGS form is that it puts simultaneously in normal form the existing symplectic structure and momentum map. The main drawback of the MGS form is that it does not have an explicit expression. We will obtain a MGS form for cotangent- lifted actions on cotangent bundles that, in addition to its defining features, respects the additional fibered structure present. This model generalizes previous results obtained by T. Schmah for orbits with fully-isotropic momentum. In addition, our construction is explicit up to the integration of a differential equation on $G$. This equation can be easily solved for the groups $SO(3)$ or $SL(2)$, thus giving explicit symplectic coordinates for arbitrary canonical actions of these groups on any cotangent bundle.
format Preprint
id arxiv_https___arxiv_org_abs_1410_3697
institution arXiv
publishDate 2014
record_format arxiv
spellingShingle The Hamiltonian Tube Of A Cotangent-Lifted Action
Rodriguez-Olmos, Miguel
Teixidó-Román, Miguel
Symplectic Geometry
53D20, 70H33, 37J15
The Marle-Guillemin-Sternberg (MGS) form is local model for a neighborhood of an orbit of a Hamiltonian Lie group action on a symplectic manifold. One of the main features of the MGS form is that it puts simultaneously in normal form the existing symplectic structure and momentum map. The main drawback of the MGS form is that it does not have an explicit expression. We will obtain a MGS form for cotangent- lifted actions on cotangent bundles that, in addition to its defining features, respects the additional fibered structure present. This model generalizes previous results obtained by T. Schmah for orbits with fully-isotropic momentum. In addition, our construction is explicit up to the integration of a differential equation on $G$. This equation can be easily solved for the groups $SO(3)$ or $SL(2)$, thus giving explicit symplectic coordinates for arbitrary canonical actions of these groups on any cotangent bundle.
title The Hamiltonian Tube Of A Cotangent-Lifted Action
topic Symplectic Geometry
53D20, 70H33, 37J15
url https://arxiv.org/abs/1410.3697