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  • Articles: DFG German National Licenses  (2)
  • 1970-1974  (1)
  • 1965-1969  (1)
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  • Articles: DFG German National Licenses  (2)
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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Archive for rational mechanics and analysis 43 (1971), S. 101-124 
    ISSN: 1432-0673
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Abstract We prove that the set D of vector fields on the configuration space B of a field whose 1-parameter groups locally associated are groups of fibre-preserving transformations of B that leave invariant that field in the sense of variational theory, is a Lie algebra with respect to ordinary addition, multiplication by real numbers and Lie brackets. We see that this Lie algebra structure can be carried over to the corresponding set ℐ of Noether invariants, which then becomes a Lie algebra in a natural way. Further, we define the “n-form of Poincaré-Cartan” of a field, and we use it to generalize the Lie algebras D and ℐ in a reasonable way. The algebras D and ℐ are subalgebras of the new Lie algebras D and ℐ′ introduced. A main result in this connection is the following: the differential dΘ of the n-form of Poincaré-Cartan Θ is −θ∧(dΩ+fοω), where (θ, dΩ+fοω) are the field equations on the vertical bundle B. The “symplectic manifold of solutions” associated with a field is introduced in a formal way and the former Lie algebras D, ℐ, D′, ℐ′ are interpreted on this manifold. In imitation of the case of analytical dynamics, the main results in this direction are: a) Every vector field of the Lie algebra D′ defines, in a canonical way, a vector field on the manifold of solutions such that its polar 1-form with respect to the symplectic metric ω 2 is the differential of its corresponding Noether invariant, and b) the Lie bracket [ω, ω′] of two Noether invariants ω, ω′ ∈ ℐ′ is the Noether invariant given by ω 2(D, D′), where D, D′ are the vector fields on the manifold of solutions defined, in the sense a), by two infinitesimal generators of ω, ω′, respectively. This will allow us to regard the Lie algebra ℐ′ as the analogous object in field theory to the Poisson algebra of analytic dynamics. We apply the general formalism to the relativistic theory of non-linear scalar fields, and we compare our results with the formalism developed by I. Segal for this case.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Communications in mathematical physics 13 (1969), S. 24-44 
    ISSN: 1432-0916
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Abstract Our aim in this paper the first one of a series concerned with the problem of field quantization starting from the symplectic structure underlying the classical theory, is to build up the variational theory necessary to all further constructions. The basic notions are the vertical bundle $$\bar B$$ and thestructure 1-form θ used to define thegeneralized infinitesimal contact transformation which allows us to state and solve the variational problem related to field physics.Giving a system of modulevalued differential forms of different degree on the vertical bundle which solutions are the stationary cross sections is the main result in the paper. In this scheme the Euler-Lagrange classical equations are the expressions induced by such a system of differential forms on any cross section of the vertical bundle. This gives us a complete linearization of the Euler-Lagrange equations and, starting from it, a natural globalization of these equations. Finally, the notion of variational problem invariant by a Lie group is defined in this scheme, Noether's theorem related to such invariant problem is formulated and an intrinsic version of the so-called Noether invariants of classical variational calculus is obtained.
    Type of Medium: Electronic Resource
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