The Maxwell–Chern–Simons gravity, and its cosmological implications
Abstract We consider the cosmological implications of a gravitational theory containing two vector fields coupled via a generalized Chern–Simons term. One of the vector fields is the usual Maxwell field, while the other is a constrained vector field with constant norm included in the action via a La...
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Series: | European Physical Journal C: Particles and Fields |
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doaj-f019cea344dd46ef9e161c1e9b7757ab2020-11-25T00:35:06ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522017-08-0177811810.1140/epjc/s10052-017-5078-0The Maxwell–Chern–Simons gravity, and its cosmological implicationsZahra Haghani0Tiberiu Harko1Shahab Shahidi2School of Physics, Damghan UniversityDepartment of Physics, Babes-Bolyai UniversitySchool of Physics, Damghan UniversityAbstract We consider the cosmological implications of a gravitational theory containing two vector fields coupled via a generalized Chern–Simons term. One of the vector fields is the usual Maxwell field, while the other is a constrained vector field with constant norm included in the action via a Lagrange multiplier. The theory admits a de Sitter type solution, with healthy cosmological perturbations. We also show that there are seven degrees of freedom that propagate on top of de Sitter space-time, consisting of two tensor polarizations, four degrees of freedom related to the two vector fields, and a scalar degree of freedom that makes one of the vector fields massive. We investigate the cosmological evolution of Bianchi type I space-time, by assuming that the matter content of the Universe can be described by the stiff and dust. The cosmological evolution of the Bianchi type I Universe strongly depends on the initial conditions of the physical quantities, as well as on the model parameters. The mean anisotropy parameter, and the deceleration parameter, are also studied, and we show that independently of the matter equation of state the cosmological evolution of the Bianchi type I Universe always ends in an isotropic de Sitter type phase.http://link.springer.com/article/10.1140/epjc/s10052-017-5078-0 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Zahra Haghani Tiberiu Harko Shahab Shahidi |
spellingShingle |
Zahra Haghani Tiberiu Harko Shahab Shahidi The Maxwell–Chern–Simons gravity, and its cosmological implications European Physical Journal C: Particles and Fields |
author_facet |
Zahra Haghani Tiberiu Harko Shahab Shahidi |
author_sort |
Zahra Haghani |
title |
The Maxwell–Chern–Simons gravity, and its cosmological implications |
title_short |
The Maxwell–Chern–Simons gravity, and its cosmological implications |
title_full |
The Maxwell–Chern–Simons gravity, and its cosmological implications |
title_fullStr |
The Maxwell–Chern–Simons gravity, and its cosmological implications |
title_full_unstemmed |
The Maxwell–Chern–Simons gravity, and its cosmological implications |
title_sort |
maxwell–chern–simons gravity, and its cosmological implications |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2017-08-01 |
description |
Abstract We consider the cosmological implications of a gravitational theory containing two vector fields coupled via a generalized Chern–Simons term. One of the vector fields is the usual Maxwell field, while the other is a constrained vector field with constant norm included in the action via a Lagrange multiplier. The theory admits a de Sitter type solution, with healthy cosmological perturbations. We also show that there are seven degrees of freedom that propagate on top of de Sitter space-time, consisting of two tensor polarizations, four degrees of freedom related to the two vector fields, and a scalar degree of freedom that makes one of the vector fields massive. We investigate the cosmological evolution of Bianchi type I space-time, by assuming that the matter content of the Universe can be described by the stiff and dust. The cosmological evolution of the Bianchi type I Universe strongly depends on the initial conditions of the physical quantities, as well as on the model parameters. The mean anisotropy parameter, and the deceleration parameter, are also studied, and we show that independently of the matter equation of state the cosmological evolution of the Bianchi type I Universe always ends in an isotropic de Sitter type phase. |
url |
http://link.springer.com/article/10.1140/epjc/s10052-017-5078-0 |
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