Measuring Gravity at Cosmological Scales
This review is a pedagogical introduction to models of gravity and how they are constrained through cosmological observations. We focus on the Horndeski scalar-tensor theory and on the quantities that can be measured with a minimum of assumptions. Alternatives or extensions of general relativity hav...
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doaj-ef207b1c44c145d193c0154afaee18e52020-11-25T01:42:34ZengMDPI AGUniverse2218-19972020-01-01622010.3390/universe6020020universe6020020Measuring Gravity at Cosmological ScalesLuca Amendola0Dario Bettoni1Ana Marta Pinho2Santiago Casas3ITP, Ruprecht-Karls-Universität Heidelberg, Philosophenweg 16, 69120 Heidelberg, GermanyITP, Ruprecht-Karls-Universität Heidelberg, Philosophenweg 16, 69120 Heidelberg, GermanyITP, Ruprecht-Karls-Universität Heidelberg, Philosophenweg 16, 69120 Heidelberg, GermanyAIM, CEA, CNRS, Université Paris-Saclay, Université Paris Diderot, Sorbonne Paris Cité, F-91191 Gif-sur-Yvette, FranceThis review is a pedagogical introduction to models of gravity and how they are constrained through cosmological observations. We focus on the Horndeski scalar-tensor theory and on the quantities that can be measured with a minimum of assumptions. Alternatives or extensions of general relativity have been proposed ever since its early years. Because of the Lovelock theorem, modifying gravity in four dimensions typically means adding new degrees of freedom. The simplest way is to include a scalar field coupled to the curvature tensor terms. The most general way of doing so without incurring in the Ostrogradski instability is the Horndeski Lagrangian and its extensions. Testing gravity means therefore, in its simplest term, testing the Horndeski Lagrangian. Since local gravity experiments can always be evaded by assuming some screening mechanism or that baryons are decoupled, or even that the effects of modified gravity are visible only at early times, we need to test gravity with cosmological observations in the late universe (large-scale structure) and in the early universe (cosmic microwave background). In this work, we review the basic tools to test gravity at cosmological scales, focusing on model-independent measurements.https://www.mdpi.com/2218-1997/6/2/20dark energymodified gravitylarge-scale structure |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Luca Amendola Dario Bettoni Ana Marta Pinho Santiago Casas |
spellingShingle |
Luca Amendola Dario Bettoni Ana Marta Pinho Santiago Casas Measuring Gravity at Cosmological Scales Universe dark energy modified gravity large-scale structure |
author_facet |
Luca Amendola Dario Bettoni Ana Marta Pinho Santiago Casas |
author_sort |
Luca Amendola |
title |
Measuring Gravity at Cosmological Scales |
title_short |
Measuring Gravity at Cosmological Scales |
title_full |
Measuring Gravity at Cosmological Scales |
title_fullStr |
Measuring Gravity at Cosmological Scales |
title_full_unstemmed |
Measuring Gravity at Cosmological Scales |
title_sort |
measuring gravity at cosmological scales |
publisher |
MDPI AG |
series |
Universe |
issn |
2218-1997 |
publishDate |
2020-01-01 |
description |
This review is a pedagogical introduction to models of gravity and how they are constrained through cosmological observations. We focus on the Horndeski scalar-tensor theory and on the quantities that can be measured with a minimum of assumptions. Alternatives or extensions of general relativity have been proposed ever since its early years. Because of the Lovelock theorem, modifying gravity in four dimensions typically means adding new degrees of freedom. The simplest way is to include a scalar field coupled to the curvature tensor terms. The most general way of doing so without incurring in the Ostrogradski instability is the Horndeski Lagrangian and its extensions. Testing gravity means therefore, in its simplest term, testing the Horndeski Lagrangian. Since local gravity experiments can always be evaded by assuming some screening mechanism or that baryons are decoupled, or even that the effects of modified gravity are visible only at early times, we need to test gravity with cosmological observations in the late universe (large-scale structure) and in the early universe (cosmic microwave background). In this work, we review the basic tools to test gravity at cosmological scales, focusing on model-independent measurements. |
topic |
dark energy modified gravity large-scale structure |
url |
https://www.mdpi.com/2218-1997/6/2/20 |
work_keys_str_mv |
AT lucaamendola measuringgravityatcosmologicalscales AT dariobettoni measuringgravityatcosmologicalscales AT anamartapinho measuringgravityatcosmologicalscales AT santiagocasas measuringgravityatcosmologicalscales |
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