2017
DOI: 10.1007/s10509-017-3197-6
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Effects of Scalar-Tensor-Vector Gravity on relativistic jets

Abstract: Scalar-Tensor-Vector Gravity (STVG) is a theory that does not require dark components to describe astrophysical data. We aim at constraining the free parameters of STVG based on recent observations of the jet in M87. We derive the equations of motion for particles in STVG-Kerr spacetime, we develop a numerical code that integrates such equations, and apply it to the jet of M87. We find that STVG deviates from GR and we set new upper limits for the free parameters of the former. We conclude that STVG is not con… Show more

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Cited by 17 publications
(16 citation statements)
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“…It is natural to expect deviations from GR also in the strong field limit. MOG black holes have been widely investigated in the literature, for example see [13]- [17]. While MOG is consistent with the recently discovered gravitational wave signals [12], it has been shown in [11] that the quasinormal modes of gravitational perturbations in the ringdown phase of the merging of two MOG black holes have different frequencies compared to those of GR.…”
Section: Introductionmentioning
confidence: 81%
“…It is natural to expect deviations from GR also in the strong field limit. MOG black holes have been widely investigated in the literature, for example see [13]- [17]. While MOG is consistent with the recently discovered gravitational wave signals [12], it has been shown in [11] that the quasinormal modes of gravitational perturbations in the ringdown phase of the merging of two MOG black holes have different frequencies compared to those of GR.…”
Section: Introductionmentioning
confidence: 81%
“…A similar calculation of the circular orbits of massive particles in the Kerr-MOG spacetime was performed in [52]; moreover, in [53] the authors have also studied more general trajectories of massive particles moving around this spacetime metric.…”
Section: A Geodesics Of Massive Particlesmentioning
confidence: 97%
“…The highest value of γ observationally estimated for M87 corresponds to the spine of jet and is γ ≈ 10. 124 Thus, the upper limit imposed to κ is: 121 κ ≤ 10 2 α G N . (52) In the second run, Lopez Armengol and Romero took Moffat's weak field limit prescription κ = √ αG N , and set θ A ej = 0.…”
Section: Effects On Jetsmentioning
confidence: 99%