Cosmological perturbations in a class of fully covariant modified theories: application to models with the same background as standard LQC
Abstract Bouncing cosmologies are obtained by adding to the Einstein–Hilbert action a term of the form $$\sqrt{-\,g}f(\chi )$$ -gf(χ) , with $$\chi $$ χ a scalar depending on the Hubble parameter only, not on its derivatives, and which is here shown to arise from the divergence of the unitary time-l...
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2018-09-01
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Series: | European Physical Journal C: Particles and Fields |
Online Access: | http://link.springer.com/article/10.1140/epjc/s10052-018-6193-2 |
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doaj-7ad3189216f145eb8c37aa4ee4d0b7f72020-11-25T00:54:44ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522018-09-0178911410.1140/epjc/s10052-018-6193-2Cosmological perturbations in a class of fully covariant modified theories: application to models with the same background as standard LQCJaume de Haro0Llibert Aresté Saló1Emilio Elizalde2Departament de Matemàtiques, Universitat Politècnica de CatalunyaDepartament de Matemàtiques, Universitat Politècnica de CatalunyaInstitute for Space Sciences, ICE/CSIC-IEECAbstract Bouncing cosmologies are obtained by adding to the Einstein–Hilbert action a term of the form $$\sqrt{-\,g}f(\chi )$$ -gf(χ) , with $$\chi $$ χ a scalar depending on the Hubble parameter only, not on its derivatives, and which is here shown to arise from the divergence of the unitary time-like eigenvector of the stress tensor. At background level, the dynamical equations for a given f-theory are calculated, showing that the simplest bouncing cosmology resulting leads to exactly the same equations as those for holonomy corrected Loop Quantum Cosmology (LQC). When dealing with perturbations, the equation for tensor ones is the same as in General Relativity (GR); for scalar perturbations, when one uses the f-theory which leads to the same background as the standard version of holonomy corrected LQC, one obtains similar equations (although a bit more elaborated) as those coming from LQC in the so-called deformed algebra approach.http://link.springer.com/article/10.1140/epjc/s10052-018-6193-2 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Jaume de Haro Llibert Aresté Saló Emilio Elizalde |
spellingShingle |
Jaume de Haro Llibert Aresté Saló Emilio Elizalde Cosmological perturbations in a class of fully covariant modified theories: application to models with the same background as standard LQC European Physical Journal C: Particles and Fields |
author_facet |
Jaume de Haro Llibert Aresté Saló Emilio Elizalde |
author_sort |
Jaume de Haro |
title |
Cosmological perturbations in a class of fully covariant modified theories: application to models with the same background as standard LQC |
title_short |
Cosmological perturbations in a class of fully covariant modified theories: application to models with the same background as standard LQC |
title_full |
Cosmological perturbations in a class of fully covariant modified theories: application to models with the same background as standard LQC |
title_fullStr |
Cosmological perturbations in a class of fully covariant modified theories: application to models with the same background as standard LQC |
title_full_unstemmed |
Cosmological perturbations in a class of fully covariant modified theories: application to models with the same background as standard LQC |
title_sort |
cosmological perturbations in a class of fully covariant modified theories: application to models with the same background as standard lqc |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2018-09-01 |
description |
Abstract Bouncing cosmologies are obtained by adding to the Einstein–Hilbert action a term of the form $$\sqrt{-\,g}f(\chi )$$ -gf(χ) , with $$\chi $$ χ a scalar depending on the Hubble parameter only, not on its derivatives, and which is here shown to arise from the divergence of the unitary time-like eigenvector of the stress tensor. At background level, the dynamical equations for a given f-theory are calculated, showing that the simplest bouncing cosmology resulting leads to exactly the same equations as those for holonomy corrected Loop Quantum Cosmology (LQC). When dealing with perturbations, the equation for tensor ones is the same as in General Relativity (GR); for scalar perturbations, when one uses the f-theory which leads to the same background as the standard version of holonomy corrected LQC, one obtains similar equations (although a bit more elaborated) as those coming from LQC in the so-called deformed algebra approach. |
url |
http://link.springer.com/article/10.1140/epjc/s10052-018-6193-2 |
work_keys_str_mv |
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