Adiabaticity and gravity theory independent conservation laws for cosmological perturbations

We carefully study the implications of adiabaticity for the behavior of cosmological perturbations. There are essentially three similar but different definitions of non-adiabaticity: one is appropriate for a thermodynamic fluid δPnad, another is for a general matter field δPc,nad, and the last one i...

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Main Authors: Antonio Enea Romano, Sander Mooij, Misao Sasaki
Format: Article
Language:English
Published: Elsevier 2016-04-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269316001507
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spelling doaj-eac3ffff86b64b94b66f932fe0f561a22020-11-25T00:15:29ZengElsevierPhysics Letters B0370-26932016-04-01755464468Adiabaticity and gravity theory independent conservation laws for cosmological perturbationsAntonio Enea Romano0Sander Mooij1Misao Sasaki2Instituto de Física, Universidad de Antioquia, A.A. 1226, Medellin, Colombia; Department of Physics, University of Crete, 71003 Heraklion, Greece; Corresponding author.Grupo de Cosmología y Astrofísica Teórica, Departamento de Física, FCFM, Universidad de Chile, Blanco Encalada 2008, Santiago, ChileYukawa Institute for Theoretical Physics, Kyoto University, Kyoto 606-8502, JapanWe carefully study the implications of adiabaticity for the behavior of cosmological perturbations. There are essentially three similar but different definitions of non-adiabaticity: one is appropriate for a thermodynamic fluid δPnad, another is for a general matter field δPc,nad, and the last one is valid only on superhorizon scales. The first two definitions coincide if cs2=cw2 where cs is the propagation speed of the perturbation, while cw2=P˙/ρ˙. Assuming the adiabaticity in the general sense, δPc,nad=0, we derive a relation between the lapse function in the comoving slicing Ac and δPnad valid for arbitrary matter field in any theory of gravity, by using only momentum conservation. The relation implies that as long as cs≠cw, the uniform density, comoving and the proper-time slicings coincide approximately for any gravity theory and for any matter field if δPnad=0 approximately. In the case of general relativity this gives the equivalence between the comoving curvature perturbation Rc and the uniform density curvature perturbation ζ on superhorizon scales, and their conservation. This is realized on superhorizon scales in standard slow-roll inflation.We then consider an example in which cw=cs, where δPnad=δPc,nad=0 exactly, but the equivalence between Rc and ζ no longer holds. Namely we consider the so-called ultra slow-roll inflation. In this case both Rc and ζ are not conserved. In particular, as for ζ, we find that it is crucial to take into account the next-to-leading order term in ζ's spatial gradient expansion to show its non-conservation, even on superhorizon scales. This is an example of the fact that adiabaticity (in the thermodynamic sense) is not always enough to ensure the conservation of Rc or ζ.http://www.sciencedirect.com/science/article/pii/S0370269316001507
collection DOAJ
language English
format Article
sources DOAJ
author Antonio Enea Romano
Sander Mooij
Misao Sasaki
spellingShingle Antonio Enea Romano
Sander Mooij
Misao Sasaki
Adiabaticity and gravity theory independent conservation laws for cosmological perturbations
Physics Letters B
author_facet Antonio Enea Romano
Sander Mooij
Misao Sasaki
author_sort Antonio Enea Romano
title Adiabaticity and gravity theory independent conservation laws for cosmological perturbations
title_short Adiabaticity and gravity theory independent conservation laws for cosmological perturbations
title_full Adiabaticity and gravity theory independent conservation laws for cosmological perturbations
title_fullStr Adiabaticity and gravity theory independent conservation laws for cosmological perturbations
title_full_unstemmed Adiabaticity and gravity theory independent conservation laws for cosmological perturbations
title_sort adiabaticity and gravity theory independent conservation laws for cosmological perturbations
publisher Elsevier
series Physics Letters B
issn 0370-2693
publishDate 2016-04-01
description We carefully study the implications of adiabaticity for the behavior of cosmological perturbations. There are essentially three similar but different definitions of non-adiabaticity: one is appropriate for a thermodynamic fluid δPnad, another is for a general matter field δPc,nad, and the last one is valid only on superhorizon scales. The first two definitions coincide if cs2=cw2 where cs is the propagation speed of the perturbation, while cw2=P˙/ρ˙. Assuming the adiabaticity in the general sense, δPc,nad=0, we derive a relation between the lapse function in the comoving slicing Ac and δPnad valid for arbitrary matter field in any theory of gravity, by using only momentum conservation. The relation implies that as long as cs≠cw, the uniform density, comoving and the proper-time slicings coincide approximately for any gravity theory and for any matter field if δPnad=0 approximately. In the case of general relativity this gives the equivalence between the comoving curvature perturbation Rc and the uniform density curvature perturbation ζ on superhorizon scales, and their conservation. This is realized on superhorizon scales in standard slow-roll inflation.We then consider an example in which cw=cs, where δPnad=δPc,nad=0 exactly, but the equivalence between Rc and ζ no longer holds. Namely we consider the so-called ultra slow-roll inflation. In this case both Rc and ζ are not conserved. In particular, as for ζ, we find that it is crucial to take into account the next-to-leading order term in ζ's spatial gradient expansion to show its non-conservation, even on superhorizon scales. This is an example of the fact that adiabaticity (in the thermodynamic sense) is not always enough to ensure the conservation of Rc or ζ.
url http://www.sciencedirect.com/science/article/pii/S0370269316001507
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