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Symplectic realizations and Lie groupoids in Poisson Electrodynamics

Fabio Di Cosmo, Alberto Ibort, Giuseppe Marmo, Patrizia Vitale

Abstract

We define the gauge potentials of Poisson electrodynamics as sections of a symplectic realization of the spacetime manifold and infinitesimal gauge transformations as a representation of the associated Lie algebroid acting on the symplectic realization. Finite gauge transformations are obtained by integrating the sections of the Lie algebroid to bisections of a symplectic groupoid, which form a one-parameter group of transformations, whose action on the fields of the theory is realized in terms of an action groupoid. A covariant electromagnetic two-form is obtained, together with a dual two-form, invariant under gauge transformations. The duality appearing in the picture originates from the existence of a pair of orthogonal foliations of the symplectic realization, which produce dual quotient manifolds, one related with space-time, the other with momenta.

Symplectic realizations and Lie groupoids in Poisson Electrodynamics

Abstract

We define the gauge potentials of Poisson electrodynamics as sections of a symplectic realization of the spacetime manifold and infinitesimal gauge transformations as a representation of the associated Lie algebroid acting on the symplectic realization. Finite gauge transformations are obtained by integrating the sections of the Lie algebroid to bisections of a symplectic groupoid, which form a one-parameter group of transformations, whose action on the fields of the theory is realized in terms of an action groupoid. A covariant electromagnetic two-form is obtained, together with a dual two-form, invariant under gauge transformations. The duality appearing in the picture originates from the existence of a pair of orthogonal foliations of the symplectic realization, which produce dual quotient manifolds, one related with space-time, the other with momenta.
Paper Structure (12 sections, 3 theorems, 28 equations)

This paper contains 12 sections, 3 theorems, 28 equations.

Key Result

Theorem 1

Given a Poisson manifold $(M,\Theta)$ and a Poisson spray $V_{\Theta}$, then there exists an open neighborhood $\mathcal{U}\subset T^*M$ of the zero section so that is a symplectic structure on $\mathcal{U}$ and the canonical projection $\pi\,\colon\,\mathcal{U}\,\rightarrow\,M$ is a symplectic realization.

Theorems & Definitions (3)

  • Theorem 1
  • Theorem 2
  • Theorem 3