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      PP-waves with Torsion - a Metric-affine Model for the Massless Neutrino

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          Abstract

          In this paper we deal with quadratic metric-affine gravity, which we briefly introduce, explain and give historical and physical reasons for using this particular theory of gravity. Further, we introduce a generalisation of well known spacetimes, namely pp-waves. A classical pp-wave is a 4-dimensional Lorentzian spacetime, which admits a nonvanishing parallel spinor field; here the connection is assumed to be Levi-Civita. This definition was generalised in our previous work to metric compatible spacetimes with torsion and used to construct new explicit vacuum solutions of quadratic metric-affine gravity, namely generalised pp-waves of parallel Ricci curvature. The physical interpretation of these solutions we propose in this article is that they represent a conformally invariant metric-affine model for a massless elementary particle. We give a comparison with the classical model describing the interaction of gravitational and massless neutrino fields, namely Einstein-Weyl theory and construct pp-wave type solutions of this theory. We point out that generalised pp-waves of parallel Ricci curvature are very similar to pp-wave type solutions of the Einstein-Weyl model and therefore propose that our generalised pp-waves of parallel Ricci curvature represent a metric-affine model for the massless neutrino.

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          General relativity with spin and torsion: Foundations and prospects

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            Interaction of Neutrinos and Gravitational Fields

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              Metric-Affine Gauge Theory of Gravity: Field Equations, Noether Identities, World Spinors, and Breaking of Dilation Invariance

              In Einstein's gravitational theory, the spacetime is Riemannian, that is, it has vanishing torsion and vanishing nonmetricity (covariant derivative of the metric). In the gauging of the general affine group \({A}(4,R)\) and of its subgroup \({GL}(4,R)\) in four dimensions, energy--momentum and hypermomentum currents of matter are canonically coupled to the one--form basis and to the connection of a metric--affine spacetime with nonvanishing torsion and nonmetricity, respectively. Fermionic matter can be described in this framework by half--integer representations of the \(\overline{SL}(4,R)\) covering subgroup. --- We set up a (first--order) Lagrangian formalism and build up the corresponding Noether machinery. For an arbitrary gauge Lagrangian, the three gauge field equations come out in a suggestive Yang-Mills like form. The conservation--type differential identities for energy--momentum and hypermomentum and the corresponding complexes and superpotentials are derived. Limiting cases such as the Einstein--Cartan theory are discussed. In particular we show, how the \({A}(4,R)\) may ``break down'' to the Poincar\'e (inhomogeneous Lorentz) group. In this context, we present explicit models for a symmetry breakdown in the cases of the Weyl (or homothetic) group, the \({SL}(4,R)\), or the \({GL}(4,R)\).
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                Author and article information

                Journal
                2014-06-07
                2014-09-03
                Article
                10.1007/s10714-014-1787-y
                1406.1930
                2d9fd5b7-2f38-4b24-94cc-2ba9fd1ff2fd

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
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                General Relativ Gravit (2014) 46:1787
                24 pages. Corrected two references. The final publication is available at springerlink.com. arXiv admin note: text overlap with arXiv:gr-qc/0505157; and text overlap with arXiv:gr-qc/0304028, arXiv:gr-qc/9402012 by other authors
                gr-qc math.DG

                General relativity & Quantum cosmology,Geometry & Topology
                General relativity & Quantum cosmology, Geometry & Topology

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