Abstract:
We consider the geometric formulation of the Hamiltonian formalism for field theory in terms of {\em Hamiltonian connections} and {\em multisymplectic forms}. In this framework the covariant Hamilton equations for Mechanics and field theory are defined in terms of multisymplectic (n+2)(n+2)--forms, where nn is the dimension of the basis manifold, together with connections on the configuration bundle. We provide a new geometric Hamiltonian description of field theory, based on the introduction of a suitable {\em composite fibered bundle} which plays the role of an {\em extended configuration bundle}. Instead of fibrations over an nn--dimensional base manifold \bX, we consider {\em fibrations over a line bundle \Tht fibered over \bX}. The concepts of {\em extended Legendre bundle}, {\em Hamiltonian connection}, {\em Hamiltonian form} and {\em covariant Hamilton equations} are introduced and put in relation with the corresponding standard concepts in the polymomentum approach to field theory.
  • talk: Opava 2001/08/27
  • field theory: classical
  • Hamiltonian formalism
  • differential forms: symplectic
  • differential geometry
  • operator: differential
  • fibre bundle