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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Main Authors: Jaume de Haro, Llibert Aresté Saló, Emilio Elizalde
Format: Article
Language:English
Published: SpringerOpen 2018-09-01
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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spelling 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
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