2019
DOI: 10.1140/epjc/s10052-019-7536-3
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Einstein–Cartan–Dirac gravity with U(1) symmetry breaking

Abstract: Einstein-Cartan theory is an extension of the standard formulation of General Relativity where torsion (the antisymmetric part of the affine connection) is non-vanishing. Just as the space-time metric is sourced by the stress-energy tensor of the matter fields, torsion is sourced via the spin density tensor, whose physical effects become relevant at very high spin densities. In this work we introduce an extension of the Einstein-Cartan-Dirac theory with an electromagnetic (Maxwell) contribution minimally coupl… Show more

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Cited by 11 publications
(22 citation statements)
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References 86 publications
(120 reference statements)
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“…These imprints could be probed by cosmological GWs [25], neutrino [26], and radiation (CMB) [27] backgrounds. This may have a profound impact on scale-invariance regimes and its symmetry breaking, parity breaking [20][21][22], CP breaking and matter/antimatter asymmetries [28,29], Uð1Þ-gauge breaking [30], Higgs-like mechanisms, etc.…”
Section: Introductionmentioning
confidence: 99%
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“…These imprints could be probed by cosmological GWs [25], neutrino [26], and radiation (CMB) [27] backgrounds. This may have a profound impact on scale-invariance regimes and its symmetry breaking, parity breaking [20][21][22], CP breaking and matter/antimatter asymmetries [28,29], Uð1Þ-gauge breaking [30], Higgs-like mechanisms, etc.…”
Section: Introductionmentioning
confidence: 99%
“…In a previous work [30], we considered an extension of the ECSK theory by adding a minimal coupling to fermionic (Dirac) and bosonic (Maxwell) fields in the RC geometry. The resulting Einstein-Cartan-Dirac-Maxwell (ECDM) model contains new nonlinear generalized Dirac-Hehl-Data and electromagnetic equations with nonminimal interactions between fermionic and bosonic fields.…”
Section: Introductionmentioning
confidence: 99%
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“…We present here field equations for ECSK theory 22 . Thus, we will neither assume the possibility of a propagating torsion (and we will always keep non-identically vanishing Riemann curvature [14]) nor display a lagrangian for a totally independent torsion field; rather, we will only set the Palatini-Cartan lagrangian for gravity, as done in Reference [15], and a matter lagrangian as the source.…”
Section: Field Equations and Conservation Lawsmentioning
confidence: 99%
“…We will focus more on the geometrical side of these equations and we will not dwell on deepening matter interaction (couplings, symmetry breaking, etc. ), as done for instance in References [20,21,24,22,23].…”
Section: Field Equations and Conservation Lawsmentioning
confidence: 99%