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Related papers: On covariant Poisson brackets in field theory

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The concept of Lagrange structure allows one to systematically quantize the Lagrangian and non-Lagrangian dynamics within the path-integral approach. In this paper, I show that any Lagrange structure gives rise to a covariant Poisson…

High Energy Physics - Theory · Physics 2015-06-22 Alexey Sharapov

Peierls brackets are part of the space-time approach to quantum field theory, and provide a Poisson bracket which, being defined for pairs of observables which are group invariant, is group invariant by construction. It is therefore well…

High Energy Physics - Theory · Physics 2007-05-23 Giampiero Esposito , Giuseppe Marmo , Cosimo Stornaiolo

Peierls brackets are part of the space-time approach to quantum field theory, and provide a Poisson bracket which, being defined for pairs of observables which are group invariant, is group invariant by construction. It is therefore well…

High Energy Physics - Theory · Physics 2016-09-06 Giuseppe Bimonte , Giampiero Esposito , Giuseppe Marmo , Cosimo Stornaiolo

How to give a natural geometric definition of a covariant Poisson bracket in classical field theory has for a long time been an open problem - as testified by the extensive literature on "multisymplectic Poisson brackets", together with the…

Mathematical Physics · Physics 2015-01-16 Michael Forger , Mário O. Salles

It is well known that both the symplectic structure and the Poisson brackets of classical field theory can be constructed directly from the Lagrangian in a covariant way, without passing through the non-covariant canonical Hamiltonian…

Mathematical Physics · Physics 2014-02-21 Igor Khavkine

The covariant canonical formalism is a covariant extension of the traditional canonical formalism of fields. In contrast to the traditional canonical theory, it has a remarkable feature that canonical equations of gauge theories or gravity…

High Energy Physics - Theory · Physics 2017-03-21 Yasuhito Kaminaga

The idea of a companion Lagrangian associated with $p$-Branes is extended to include the presence of U(1) fields. The Brane Lagrangians are constructed with $F_{ij}$ represented in terms of Lagrange Brackets, which make manifest the…

High Energy Physics - Theory · Physics 2009-10-31 David B. Fairlie

A geometrical approach to the covariant formulation of the dynamics of relativistic systems is introduced. A realization of Peierls brackets by means of a bivector field over the space of solutions of the Euler-Lagrange equations of a…

Mathematical Physics · Physics 2017-06-06 Manuel Asorey , Florio M. Ciaglia , Fabio Di Cosmo , Alberto Ibort

We extend the Poisson bracket from a Lie bracket of phase space functions to a Lie bracket of functions on the space of canonical histories and investigate the resulting algebras. Typically, such extensions define corresponding Lie algebras…

High Energy Physics - Theory · Physics 2009-10-22 Donald Marolf

As it is well-known, Poisson brackets play a fundamental role both in mechanics and in classical field theories. In this paper we develop a theory of extensions of graded Poisson brackets in graded Dirac manifolds. We then show how these…

Mathematical Physics · Physics 2025-07-08 Manuel de León , Rubén Izquierdo-López

We establish a link between the multisymplectic and the covariant phase space approach to geometric field theory by showing how to derive the symplectic form on the latter, as introduced by Crnkovic-Witten and Zuckerman, from the…

Mathematical Physics · Physics 2012-02-24 Michael Forger , Sandro V. Romero

An explicit Lorentz covariant formulation of the canonical theory for classical fields is established on a space-like hypersurface. Hamilton's equations and a Poisson bracket are defined on the space-like hypersurface. The Poisson bracket…

High Energy Physics - Theory · Physics 2009-09-25 Hiroshi Ozaki

We construct a Leibniz bracket on the space $\Omega^\bullet (J^k (\pi))$ of all differential forms over the finite-dimensional jet bundle $J^k (\pi)$. As an example, we write Maxwell equations with sources in the covariant…

Mathematical Physics · Physics 2015-05-13 S. A. Pol'shin

In this note the long standing problem of the definition of a Poisson bracket in the framework of a multisymplectic formulation of classical field theory is solved. The new bracket operation can be applied to forms of arbitary degree.…

Mathematical Physics · Physics 2015-06-26 Michael Forger , Cornelius Paufler , Hartmann Römer

The dynamic of a classical system can be expressed by means of Poisson brackets. In this paper we generalize the relation between the usual non covariant Hamiltonian and the Poisson brackets to a covariant Hamiltonian and new brackets in…

Classical Physics · Physics 2007-05-23 A. Berard , H. Mohrbach , P. Gosselin

We present a general definition of the Poisson bracket between differential forms on the extended multiphase space appearing in the geometric formulation of first order classical field theories and, more generally, on exact multisymplectic…

Mathematical Physics · Physics 2009-11-07 Michael Forger , Cornelius Paufler , Hartmann Roemer

We introduce the concept of multisymplectic formalism, familiar in covariant field theory, for the study of integrable defects in 1+1 classical field theory. The main idea is the coexistence of two Poisson brackets, one for each spacetime…

Mathematical Physics · Physics 2015-06-23 V. Caudrelier , A. Kundu

We bring together aspects of covariant Hamiltonian field theory and of classical integrable field theories in $1+1$ dimensions. Specifically, our main result is to obtain for the first time the classical $r$-matrix structure within a…

Mathematical Physics · Physics 2019-12-02 Vincent Caudrelier , Matteo Stoppato

A consistent, local coordinate formulation of covariant Hamiltonian field theory is presented. Whereas the covariant canonical field equations are equivalent to the Euler-Lagrange field equations, the covariant canonical transformation…

Mathematical Physics · Physics 2020-12-16 Jürgen Struckmeier , Andreas Redelbach

We review the recent generalization of the basic structures of classical analytical mechanics to field theory within the framework of the De Donder-Weyl (DW) covariant canonical theory. We start from the Poincar\'e-Cartan form and construct…

High Energy Physics - Theory · Physics 2007-05-23 I. Kanatchikov
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