Cosmological axial gravitational waves in the f(R) Starobinsky model

We investigate the propagation of cosmological axial (or odd parity) gravitational waves (GWs) in the framework of the f ( R ) gravity with f ( R ) = R + λ R 2 , the Starobinsky model. The metric tensor and the energy–momentum tensor of matter are perturbed by using the Regge–Wheeler axial perturbat...

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Published inEuropean physical journal plus Vol. 136; no. 4; p. 415
Main Authors Siddiqa, Aisha, Mehwish, Syeda Z. B., Alves, Márcio E. S.
Format Journal Article
LanguageEnglish
Published Berlin/Heidelberg Springer Berlin Heidelberg 20.04.2021
Springer Nature B.V
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Abstract We investigate the propagation of cosmological axial (or odd parity) gravitational waves (GWs) in the framework of the f ( R ) gravity with f ( R ) = R + λ R 2 , the Starobinsky model. The metric tensor and the energy–momentum tensor of matter are perturbed by using the Regge–Wheeler axial perturbations framework. We solve the coupled system of differential equations of the perturbation parameters for two cosmological eras in which simply analytical solutions can be found, namely the radiation-dominated epoch and the de Sitter stage. In the former case, the Starobinsky model predicts exactly the same result of the General Relativity theory. On the other hand, remembering that in the Starobinsky inflation, the Universe starts within a metastable de Sitter state, we find the evolution of the axial GWs for this early epoch. In this sense, our results should be interpreted as the initial conditions for axial GWs in the Starobinsky model. We show how the initial evolution of axial GWs is affected by the presence of the higher-order curvature term and how it depends on the model parameter λ . Certainly, such an effect could leave an imprint on the spectrum of axial GWs at the end of the Starobinsky inflation, but this is a subject of further investigations.
AbstractList We investigate the propagation of cosmological axial (or odd parity) gravitational waves (GWs) in the framework of the f ( R ) gravity with f ( R ) = R + λ R 2 , the Starobinsky model. The metric tensor and the energy–momentum tensor of matter are perturbed by using the Regge–Wheeler axial perturbations framework. We solve the coupled system of differential equations of the perturbation parameters for two cosmological eras in which simply analytical solutions can be found, namely the radiation-dominated epoch and the de Sitter stage. In the former case, the Starobinsky model predicts exactly the same result of the General Relativity theory. On the other hand, remembering that in the Starobinsky inflation, the Universe starts within a metastable de Sitter state, we find the evolution of the axial GWs for this early epoch. In this sense, our results should be interpreted as the initial conditions for axial GWs in the Starobinsky model. We show how the initial evolution of axial GWs is affected by the presence of the higher-order curvature term and how it depends on the model parameter λ . Certainly, such an effect could leave an imprint on the spectrum of axial GWs at the end of the Starobinsky inflation, but this is a subject of further investigations.
We investigate the propagation of cosmological axial (or odd parity) gravitational waves (GWs) in the framework of the f(R) gravity with f(R)=R+λR2, the Starobinsky model. The metric tensor and the energy–momentum tensor of matter are perturbed by using the Regge–Wheeler axial perturbations framework. We solve the coupled system of differential equations of the perturbation parameters for two cosmological eras in which simply analytical solutions can be found, namely the radiation-dominated epoch and the de Sitter stage. In the former case, the Starobinsky model predicts exactly the same result of the General Relativity theory. On the other hand, remembering that in the Starobinsky inflation, the Universe starts within a metastable de Sitter state, we find the evolution of the axial GWs for this early epoch. In this sense, our results should be interpreted as the initial conditions for axial GWs in the Starobinsky model. We show how the initial evolution of axial GWs is affected by the presence of the higher-order curvature term and how it depends on the model parameter λ. Certainly, such an effect could leave an imprint on the spectrum of axial GWs at the end of the Starobinsky inflation, but this is a subject of further investigations.
ArticleNumber 415
Author Siddiqa, Aisha
Alves, Márcio E. S.
Mehwish, Syeda Z. B.
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  givenname: Syeda Z. B.
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  givenname: Márcio E. S.
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Snippet We investigate the propagation of cosmological axial (or odd parity) gravitational waves (GWs) in the framework of the f ( R ) gravity with f ( R ) = R + λ R 2...
We investigate the propagation of cosmological axial (or odd parity) gravitational waves (GWs) in the framework of the f(R) gravity with f(R)=R+λR2, the...
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SubjectTerms Applied and Technical Physics
Atomic
Black holes
Complex Systems
Condensed Matter Physics
Cosmology
Dark energy
Differential equations
Evolution
Exact solutions
Gravitational waves
Initial conditions
Mathematical and Computational Physics
Mathematical models
Molecular
Optical and Plasma Physics
Parameters
Parity
Perturbation
Physics
Physics and Astronomy
Propagation
Radiation
Regular Article
Relativity
Spacetime
Tensors
Theoretical
Theory of relativity
Universe
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Title Cosmological axial gravitational waves in the f(R) Starobinsky model
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