Do solar system experiments constrain scalar–tensor gravity?

Abstract It is now established that, contrary to common belief, (electro-)vacuum Brans–Dicke gravity does not reduce to general relativity (GR) for large values of the Brans–Dicke coupling $$\omega $$ ω . Since the essence of experimental tests of scalar–tensor gravity consists of providing lower bo...

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Main Authors: Valerio Faraoni, Jeremy Côté, Andrea Giusti
Format: Article
Language:English
Published: SpringerOpen 2020-02-01
Series:European Physical Journal C: Particles and Fields
Online Access:https://doi.org/10.1140/epjc/s10052-020-7721-4
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spelling doaj-18432376d6e748bb8d14a65697a61a7a2021-02-14T12:44:27ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522020-02-018021610.1140/epjc/s10052-020-7721-4Do solar system experiments constrain scalar–tensor gravity?Valerio Faraoni0Jeremy Côté1Andrea Giusti2Department of Physics and Astronomy, Bishop’s UniversityDepartment of Physics and Astronomy, Bishop’s UniversityDepartment of Physics and Astronomy, Bishop’s UniversityAbstract It is now established that, contrary to common belief, (electro-)vacuum Brans–Dicke gravity does not reduce to general relativity (GR) for large values of the Brans–Dicke coupling $$\omega $$ ω . Since the essence of experimental tests of scalar–tensor gravity consists of providing lower bounds on $$\omega $$ ω , in light of the misguided assumption of the equivalence between the limit $$\omega \rightarrow \infty $$ ω→∞ and the GR limit of Brans–Dicke gravity, the parametrized post-Newtonian (PPN) formalism on which these tests are based could be in jeopardy. We show that, in the linearized approximation used by the PPN formalism, the anomaly in the limit to general relativity disappears. However, it survives to second (and higher) order and in strong gravity. In other words, while the weak gravity regime cannot tell apart GR and $$\omega \rightarrow \infty $$ ω→∞ Brans–Dicke gravity, when higher order terms in the PPN analysis of Brans–Dicke gravity are included, the latter never reduces to the one of GR in this limit. This fact is relevant for experiments aiming to test second order light deflection and Shapiro time delay.https://doi.org/10.1140/epjc/s10052-020-7721-4
collection DOAJ
language English
format Article
sources DOAJ
author Valerio Faraoni
Jeremy Côté
Andrea Giusti
spellingShingle Valerio Faraoni
Jeremy Côté
Andrea Giusti
Do solar system experiments constrain scalar–tensor gravity?
European Physical Journal C: Particles and Fields
author_facet Valerio Faraoni
Jeremy Côté
Andrea Giusti
author_sort Valerio Faraoni
title Do solar system experiments constrain scalar–tensor gravity?
title_short Do solar system experiments constrain scalar–tensor gravity?
title_full Do solar system experiments constrain scalar–tensor gravity?
title_fullStr Do solar system experiments constrain scalar–tensor gravity?
title_full_unstemmed Do solar system experiments constrain scalar–tensor gravity?
title_sort do solar system experiments constrain scalar–tensor gravity?
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2020-02-01
description Abstract It is now established that, contrary to common belief, (electro-)vacuum Brans–Dicke gravity does not reduce to general relativity (GR) for large values of the Brans–Dicke coupling $$\omega $$ ω . Since the essence of experimental tests of scalar–tensor gravity consists of providing lower bounds on $$\omega $$ ω , in light of the misguided assumption of the equivalence between the limit $$\omega \rightarrow \infty $$ ω→∞ and the GR limit of Brans–Dicke gravity, the parametrized post-Newtonian (PPN) formalism on which these tests are based could be in jeopardy. We show that, in the linearized approximation used by the PPN formalism, the anomaly in the limit to general relativity disappears. However, it survives to second (and higher) order and in strong gravity. In other words, while the weak gravity regime cannot tell apart GR and $$\omega \rightarrow \infty $$ ω→∞ Brans–Dicke gravity, when higher order terms in the PPN analysis of Brans–Dicke gravity are included, the latter never reduces to the one of GR in this limit. This fact is relevant for experiments aiming to test second order light deflection and Shapiro time delay.
url https://doi.org/10.1140/epjc/s10052-020-7721-4
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