14-11-2003
Xavier Gràcia.
Some fine points in affine geometry
20-05-2003
Olga Krupková.
Recent results in Hamiltonian field theory, II:
Regular variational problems and regularization of Lagrangians
20-05-2003
Demeter Krupka.
Variational principles for energy-momentum tensors
19-05-2003
Olga Krupková.
Recent results in Hamiltonian field theory, I:
Hamiltonian systems associated with Euler-Lagrange equations, Lepagean
and multisymplectic forms
07-05-2003
Rafael Ramírez.
Cartesian approach for nonholonomic systems
18-03-2003
Rubén Martín.
Time-dependent singular systems
17-01-2003
Jorge Cortés.
Characterization of gradient control systems
The purpose of this talk is to study some affine-geometric and algebraic aspects of the vector hull, and to show that an apparently quiet domain as affine geometry can hide pleasant surprises.
Abstracts:
Classical Hamilton-De Donder equations are related with the
Poincaré-Cartan form of a Lagrangian.
For Lagrangians satisfying a regularity condition they are
equivalent with the Euler-Lagrange equations,
and it is possible to find a coordinate transformation
(Legendre transformation)
bringing the Hamilton-De Donder equations to a canonical form.
It turns out, however, that almost all interesting Lagrangians
in field theory
(e.g. Dirac field, electromagnetic field, gravity, Yang-Mills
fields)
do not satisfy the regularity condition, hence there is not a clear
Hamiltonian counterpart to their Euler-Lagrange equations.
In the present two talks we shall discuss recent generalizations
of Hamilton theory for first and higher order variational
problems on fibered manifolds,
based on the concept of Lepagean (n+1)-form.
These forms are closed counterparts of Euler-Lagrange forms,
and provide Hamilton equations associated directly with
Euler-Lagrange equations
(i.e. the same for the class of equivalent Lagrangians).
Since, in this setting, Hamilton equations become equations for
integral sections of a differential system,
it is possible to understand the concepts of regularity and of
Legendre transformation geometrically as properties of the
Hamiltonian differential system.
As a result, one obtains not only a geometric meaning for these
concepts, but also generalized regularity conditions and Legendre
transformation formulas.
It is also significant that regularity conditions depend on
a concrete choice of a Lepage form associated with the given
variational problem
(in this context, the Poincaré-Cartan form represents one
possible choice) --
this leads to a regularization procedure for Lagrangians.
We shall show that all the above mentioned physical field
Lagrangians are regularizable, and have appropriate Hamilton
equations, Hamiltonian, and independent momenta.
Lepage (n+1)-forms and the arising Hamilton equations are
closely related with multisymplectic forms:
these relations will be also discussed.
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