2011
DOI: 10.1007/s10773-011-0871-2
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Unified Field Theoretical Models from Generalized Affine Geometries III

Abstract: In this work the underlying structure of new type of Unified Field Theoretical model introduced in by the authors is elucidated and analyzed from the geometrical and group theoretical point of view. Our goal is to take advantage of the geometrical and topological properties of this theory in order to determine the minimal group structure of the resultant spacetime manifold able to support a fermionic structure. From this fact, the relation between antisymmetric torsion and Dirac structure of the spacetime is d… Show more

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Cited by 11 publications
(32 citation statements)
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“…Similar thing happens in the non-Riemannian case, as pointed out in [12] [13] [14][15] [16], where the corresponding affine geometrical structure induces naturally the following constraint: K g = constant. This natural constraint impose a condition (ratio) between both basic tensors through their determinants: the metric determinant g and the fundamental one K (in the sense of a nonsymmetric theory that contains the antisymmetric structures),…”
Section: Introductionsupporting
confidence: 52%
“…Similar thing happens in the non-Riemannian case, as pointed out in [12] [13] [14][15] [16], where the corresponding affine geometrical structure induces naturally the following constraint: K g = constant. This natural constraint impose a condition (ratio) between both basic tensors through their determinants: the metric determinant g and the fundamental one K (in the sense of a nonsymmetric theory that contains the antisymmetric structures),…”
Section: Introductionsupporting
confidence: 52%
“…As it was shown in [19][20][21][22][23][24] for this model of gravity (see Ref. [25], for astrophysical neutrino applications), the Dirac equation is derived from the same space-time manifold and acquires a coupling modification of the form…”
Section: Introductionmentioning
confidence: 85%
“…As pointed out in references [19][20][21][22][23][24], the torsion vector h = h α dx α (the 4-dimensional dual of the torsion field T βγδ ) plays multiple roles and can be constrained in several different physical situations. Mathematically, it is defined by the Hodge-de Rham decomposition given by the 4-dimensional Helmholtz theorem which states:…”
Section: Generalized Hodge-de Rham Decomposition the Vector Torsmentioning
confidence: 99%
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“…Notice that f a µ , in a sharp contrast with the tetrad field e a µ , carries the symmetry e aµ f a ν = f µν = −f νµ . See [5,6] for more mathematical and geometrical details of the theory. Consequently, the generalized Ricci tensor splits into a symmetric and antisymmetric part, namely:…”
Section: New Affine Gravity With Torsionmentioning
confidence: 99%