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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Online Access: | https://doi.org/10.1140/epjc/s10052-020-7721-4 |
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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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AT valeriofaraoni dosolarsystemexperimentsconstrainscalartensorgravity AT jeremycote dosolarsystemexperimentsconstrainscalartensorgravity AT andreagiusti dosolarsystemexperimentsconstrainscalartensorgravity |
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