2021
DOI: 10.1016/j.dark.2021.100835
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Einstein-Æther gravity in the light of event horizon telescope observations of M87*

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Cited by 65 publications
(11 citation statements)
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“…In order to describe the shadow as seen by large distances, one introduces the two celestial coordinates X and Y [85], namely X = lim r * →∞ −r 2 * sin θ 0 dφ dr and Y = lim r * →∞ r 2 * dθ dr , with r * the distance between the black hole and the observer, and θ 0 the inclination angle between the observer's line of sight and the black hole rotational axis. Using the geodesics equations we finally obtain [86].…”
Section: Barrow Entropy Effect On Black Hole Shadowsmentioning
confidence: 99%
“…In order to describe the shadow as seen by large distances, one introduces the two celestial coordinates X and Y [85], namely X = lim r * →∞ −r 2 * sin θ 0 dφ dr and Y = lim r * →∞ r 2 * dθ dr , with r * the distance between the black hole and the observer, and θ 0 the inclination angle between the observer's line of sight and the black hole rotational axis. Using the geodesics equations we finally obtain [86].…”
Section: Barrow Entropy Effect On Black Hole Shadowsmentioning
confidence: 99%
“…We adopt a rough analysis by using the generalized metric (66). Given that the leading term of the black hole spin parameter is only presence in the nondiagonal component tϕ of the Kerr black hole metric and this component does not deform the photon ring [95], we expect the qualitative conclusions will not be changed if we only focus on the overall size of photon ring. Nevertheless, given that the Eq.…”
Section: B Methods and Resultsmentioning
confidence: 99%
“…Recently, the polarization of the ring and magnetic field structure near the horizon was studied based on the first picture of M87* [36,37]. Up to now, black hole shadows have been studied widely [38][39][40][41][42][43][44][45][46][47][48][49][50][51][52].…”
Section: Introductionmentioning
confidence: 99%