160 research outputs found
Geometric Hamilton-Jacobi Theory
The Hamilton-Jacobi problem is revisited bearing in mind the consequences
arising from a possible bi-Hamiltonian structure. The problem is formulated on
the tangent bundle for Lagrangian systems in order to avoid the bias of the
existence of a natural symplectic structure on the cotangent bundle. First it
is developed for systems described by regular Lagrangians and then extended to
systems described by singular Lagrangians with no secondary constraints. We
also consider the example of the free relativistic particle, the rigid body and
the electron-monopole system.Comment: 40 page
Structural aspects of Hamilton-Jacobi theory
In our previous papers [11,13] we showed that the Hamilton-Jacobi problem can
be regarded as a way to describe a given dynamics on a phase space manifold in
terms of a family of dynamics on a lower-dimensional manifold. We also showed
how constants of the motion help to solve the Hamilton-Jacobi equation. Here we
want to delve into this interpretation by considering the most general case: a
dynamical system on a manifold that is described in terms of a family of
dynamics (`slicing vector fields') on lower-dimensional manifolds. We identify
the relevant geometric structures that lead from this decomposition of the
dynamics to the classical Hamilton-Jacobi theory, by considering special cases
like fibred manifolds and Hamiltonian dynamics, in the symplectic framework and
the Poisson one. We also show how a set of functions on a tangent bundle can
determine a second-order dynamics for which they are constants of the motion.Comment: 26 pages. Minor changes (some minor mistakes are corrected
Pre-multisymplectic constraint algorithm for field theories
We present a geometric algorithm for obtaining consistent solutions to
systems of partial differential equations, mainly arising from singular
covariant first-order classical field theories. This algorithm gives an
intrinsic description of all the constraint submanifolds.
The field equations are stated geometrically, either representing their
solutions by integrable connections or, what is equivalent, by certain kinds of
integrable m-vector fields. First, we consider the problem of finding
connections or multivector fields solutions to the field equations in a general
framework: a pre-multisymplectic fibre bundle (which will be identified with
the first-order jet bundle and the multimomentum bundle when Lagrangian and
Hamiltonian field theories are considered). Then, the problem is stated and
solved in a linear context, and a pointwise application of the results leads to
the algorithm for the general case. In a second step, the integrability of the
solutions is also studied.
Finally, the method is applied to Lagrangian and Hamiltonian field theories
and, for the former, the problem of finding holonomic solutions is also
analized.Comment: 30 pp. Presented in the International Workshop on Geometric Methods
in Modern Physics (Firenze, April 2005
Hamilton-Jacobi theory and the evolution operator
We present a new setting of the geometric Hamilton-Jacobi theory by using the so-called time-evolution operator K. This new approach unifies both the Lagrangian and the Hamiltonian formulation of the problem developed in a previous paper [7], and can be applied to the case of singular Lagrangian dynamical systems
Constraint algorithm for k-presymplectic Hamiltonian systems. Application to singular field theories
The k-symplectic formulation of field theories is especially simple, since
only tangent and cotangent bundles are needed in its description. Its defining
elements show a close relationship with those in the symplectic formulation of
mechanics. It will be shown that this relationship also stands in the
presymplectic case. In a natural way, one can mimick the presymplectic
constraint algorithm to obtain a constraint algorithm that can be applied to
-presymplectic field theory, and more particularly to the Lagrangian and
Hamiltonian formulations of field theories defined by a singular Lagrangian, as
well as to the unified Lagrangian-Hamiltonian formalism (Skinner--Rusk
formalism) for k-presymplectic field theory. Two examples of application of the
algorithm are also analyzed.Comment: 22 p
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