2014
DOI: 10.1063/1.4862855
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Differential geometry, Palatini gravity and reduction

Abstract: The present article deals with a formulation of the so called (vacuum) Palatini gravity as a general variational principle. In order to accomplish this goal, some geometrical tools related to the geometry of the bundle of connections of the frame bundle LM are used. A generalization of Lagrange-Poincaré reduction scheme to these types of variational problems allows us to relate it with the Einstein-Hilbert variational problem. Relations with some other variational problems for gravity found in the literature a… Show more

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Cited by 15 publications
(37 citation statements)
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“…(1) To set a Griffiths variational problem for this theory, and (2) to construct the classical Lepage-equivalent variational problem for this variational problem, proving also that it is a contravariant Lepage-equivalent in the sense of Definition 9. As we know, a Griffiths variational problem describing vacuum Palatini gravity exists [Cap14]. In short, it is the variational problem specified by the triple…”
Section: The Unified Formalism For Palatini Gravitymentioning
confidence: 99%
See 1 more Smart Citation
“…(1) To set a Griffiths variational problem for this theory, and (2) to construct the classical Lepage-equivalent variational problem for this variational problem, proving also that it is a contravariant Lepage-equivalent in the sense of Definition 9. As we know, a Griffiths variational problem describing vacuum Palatini gravity exists [Cap14]. In short, it is the variational problem specified by the triple…”
Section: The Unified Formalism For Palatini Gravitymentioning
confidence: 99%
“…Our starting point will be the Griffiths variational problem considered in [Cap14] for Palatini gravity; this variational problem can be considered as an alternative Lagrangian version for the formulation of vacuum GR equations in terms of exterior differential systems, as it is given for example in [Est05]. The method chosen for the construction of the unified formalism comes from the work of Gotay [Got91a,Got91b], and it consists into the employment of a classical Lepageequivalent variational problem (in the sense defined by Gotay in these works) as a replacement for the Griffiths variational problem at hands.…”
Section: Introductionmentioning
confidence: 99%
“…We denote by ker 4 π 1 Ω L EP the set of locally decomposable and π 1 -transverse multivector fields satisfying equations (4) but not being (semi)holonomic necessarily. Then, ker 4 SH Ω L EP and ker 4 H Ω L EP denote the sets of semi-holonomic and the holonomic multivector fields which are solutions to the equations (4), respectively. Obviously we have…”
Section: Compatibility and Consistency Constraintsmentioning
confidence: 99%
“…The multisymplectic and polysymplectic techniques have been also applied to treat different aspects of one of the most classical approaches in General Relativity: the Einstein-Palatini or Metric-Affine model [4,5,31,37,38]. In particular, in [5] an exhaustive study of the multisymplectic description of the model has been done, using a unified formalism which joins both the Lagrangian and Hamiltonian formalisms into a single one.…”
Section: Introductionmentioning
confidence: 99%
“…As a result we present here a successful approach to the discretization of a variational theory that involves a field theory with several dependent and independent variables on arbitrary manifolds, in a situation that includes non-trivial bundles with non-commutative groups of symmetries, where a reduction procedure allows to describe critical fields through a system of partial differential equations formulated for a reduced field. More precisely, we shall deal with a general problem of Euler-Poincaré reduction for a field theory in a principal bundle [13,14,15], a common situation in several scientific branches, like motion and control of mechanical systems [33,32], elasticity [18,19], liquid crystal theory [27], Palatini gravity [7], and other gauge field theories. We show how to formulate the discrete counterparts of the smooth elements present in the theory and in its reduction, and present the needed objects that allow to relate smooth and discrete fields.…”
Section: Introductionmentioning
confidence: 99%