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    Shadow sizes around black holes as possible signatures of Horndeski gravity

    Zdeněk Stuchlík · Červenec 01, 2018 · Fyzika · 0 comments
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    Publication date: Jul 2018

    Abstract:
    The classical general relativity (GR) is remarkably confirmed in
    different astronomical tests. Recently, gravitational waves have been
    detected from binary black holes and binary neutron starsystems.
    Moreover, constraints on alternative theories of gravity have been
    obtained, so thatgraviton mass bounds have been found such as m_g <
    7.7 × 10^{-23} eV. It means that theories of massive gravity,if they are
    realized in nature, have to be very close to GR.In spite of a great
    progress of GR now there exist a number of alternative theories of
    gravity,such as f(R) theories, theories of massive gravity, scalar-
    tensor theories etc.Scalar-tensor theories proposed by Hordeski are
    among popular alternatives for classical general relativity (GR).There
    are no-hair theorems in such a theory, however, there exist hairy black
    hole solutions under some assumptions.for instantce, Babichev et al.
    (2017) constructed a set of hairy static black hole solutions (for
    quarticHordeski Lagrangian of scalar-tensor theory of gravity). We show
    that analytical expressions for shadow sizeobtained for Reissner –
    Nordström metric (with electric and tidal charges) may be usedto compare
    theoretical predictions and observations for asymptotically flat black
    holes with a scalar hair which mimics an electric charge.We present
    analytical expressions for shadow size for static black hole solutions
    with de-Sitter and anti-de-Sitter asymptotics.The relations could be
    used for comparison of the theoretical models with observational data
    obtained with the Event Horizon Telescope for the black hole at the
    Galactic Center or in galaxy M87.

    Authors:
    Zakharov, Alexander; Stuchlik, Zdenek; Jaluvkova, Pavlina; Tursunov, Arman;

    https://ui.adsabs.harvard.edu/abs/2018cosp…42E3802Z

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