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Skinner--Rusk formalism of action-dependent multicontact field theories

Xavier Rivas, Narciso Román-Roy, Annamaria Villanova

TL;DR

The paper addresses the need for a covariant framework to describe action-dependent (non-conservative) classical field theories. It develops multicontact geometry as a generalization of contact and multisymplectic formalisms and introduces a Skinner–Rusk–type unified approach that merges the Lagrangian and Hamiltonian descriptions within action-dependent dynamics, including a constraint algorithm for singular theories. The main contributions are the systematic development of multicontact Lagrangian and Hamiltonian formalisms, and the Skinner–Rusk unified framework implemented on extended jet–multimomentum bundles with a final constraint submanifold, illustrated by Maxwell theory with action-dependent terms describing electromagnetism in matter. This work provides a robust geometric toolkit for dissipative field theories and opens avenues for extensions to higher-order theories and gauge-field models, with potential applications in modified gravitation and electromagnetism in complex media.

Abstract

The newly developed multicontact structure, based on contact and multisymplectic geometries, provides a very general geometrical framework suitable for the treatment of action-dependent classical field theories. Having successfully applied it to formulate the Lagrangian and Hamiltonian descriptions of these theories, in the present work, the well-known Skinner--Rusk formalism is presented in this multicontact setting, which allows us to provide a combined version of both Lagrangian and Hamiltonian formalisms particularly suitable for the study and description of singular theories. As an application of this last situation, we study a modification of Maxwell's Lagrangian of classical electromagnetism, which incorporates action-dependent terms and allows us to describe electromagnetism in material media.

Skinner--Rusk formalism of action-dependent multicontact field theories

TL;DR

The paper addresses the need for a covariant framework to describe action-dependent (non-conservative) classical field theories. It develops multicontact geometry as a generalization of contact and multisymplectic formalisms and introduces a Skinner–Rusk–type unified approach that merges the Lagrangian and Hamiltonian descriptions within action-dependent dynamics, including a constraint algorithm for singular theories. The main contributions are the systematic development of multicontact Lagrangian and Hamiltonian formalisms, and the Skinner–Rusk unified framework implemented on extended jet–multimomentum bundles with a final constraint submanifold, illustrated by Maxwell theory with action-dependent terms describing electromagnetism in matter. This work provides a robust geometric toolkit for dissipative field theories and opens avenues for extensions to higher-order theories and gauge-field models, with potential applications in modified gravitation and electromagnetism in complex media.

Abstract

The newly developed multicontact structure, based on contact and multisymplectic geometries, provides a very general geometrical framework suitable for the treatment of action-dependent classical field theories. Having successfully applied it to formulate the Lagrangian and Hamiltonian descriptions of these theories, in the present work, the well-known Skinner--Rusk formalism is presented in this multicontact setting, which allows us to provide a combined version of both Lagrangian and Hamiltonian formalisms particularly suitable for the study and description of singular theories. As an application of this last situation, we study a modification of Maxwell's Lagrangian of classical electromagnetism, which incorporates action-dependent terms and allows us to describe electromagnetism in material media.

Paper Structure

This paper contains 12 sections, 7 theorems, 106 equations.

Key Result

Proposition 2.6

Let $(\mathcal{M},\Theta,\omega)$ be a special (pre)multicontact manifold, then there exists a unique $1$-form $\sigma_{\Theta}\in\Omega^1(\mathcal{M})$, called the dissipation form, satisfying

Theorems & Definitions (32)

  • Definition 2.1
  • Definition 2.2
  • Definition 2.3
  • Remark 2.4
  • Remark 2.5
  • Proposition 2.6
  • Definition 2.7
  • Definition 2.8
  • Definition 2.9
  • Proposition 2.10
  • ...and 22 more