2019
DOI: 10.48550/arxiv.1905.13720
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Review on tests of General Relativity And Modified Gravity Using Pulsar Timing

Abstract: In this report we aim to describe the most stringent tests of the strong equivalence principle, the fundamental principle of General Relativity, using pulsar timing. For this purpose, we first construct the parametrized post-Newtonian and post-Keplerian formalism together with their parameters. Then we constrain the post-Newtonian parameters associated to the violation of the strong equivalence principle with the most stringent tests using pulsar timing techniques. We will in particular see that these bounds a… Show more

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Cited by 5 publications
(9 citation statements)
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“…Additional contributions to the binary's period decay may come from dipole radiation or scalarization (see e.g. [34,35,[55][56][57]). In order to quantify these effects one must specify the underlying theory considered, however in this Letter we have taken an agnostic approach.…”
Section: We Thus Neglect the Quadratic Term ġ2mentioning
confidence: 99%
“…Additional contributions to the binary's period decay may come from dipole radiation or scalarization (see e.g. [34,35,[55][56][57]). In order to quantify these effects one must specify the underlying theory considered, however in this Letter we have taken an agnostic approach.…”
Section: We Thus Neglect the Quadratic Term ġ2mentioning
confidence: 99%
“…This degeneracy allows us to choose a reconstructed theory with predetermined cosmological behaviour that exhibits a screening mechanism. Because of its screening property, such a theory is more likely to satisfy stringent astrophysical constraints [2,6]. We shall now develop a technique to test for, and if needed incorporate, a screening mechanism in a reconstructed theory of the form (2.21).…”
Section: Screening Reconstructed Horndeski Theoriesmentioning
confidence: 99%
“…We have now shown how to implement various screening mechanisms in Horndeski theories reconstructed from the cosmological EFT of dark energy at lowest order in the scaling parameter α. This GR limit is required in order to satisfy the numerous astrophysical constraints from Solar System tests and pulsar timing observations [2,6]. However, in order to describe corrections to the Einstein field equations we need to derive the metric field equations at next-to-leading order in α.…”
Section: Connecting Ppn and Eft Via Reconstructed Horndeski Modelsmentioning
confidence: 99%
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“…A significant parameter space of this class of models has traditionally been explored as an explanation of cosmic acceleration. Often, a significant modification of gravity on cosmological scales was invoked as the driver of cosmic acceleration, while so-called screening mechanisms would allow a recovery of GR in high-density environments or at short distances such as in galaxies or in the Solar System, where tight constraints on deviations from GR have been established [1,[27][28][29][30][31][32]. However, this concept has become severely challenged by the luminal propagation of gravitational waves (GWs) [33,34], and cosmic acceleration may be limited to the dark energy aspects of a Horndeski field rather than its direct dynamical change of gravity.…”
Section: Introductionmentioning
confidence: 99%