2015
DOI: 10.1007/978-3-319-20046-0_7
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On the Black Holes in Alternative Theories of Gravity: The Case of Non-linear Massive Gravity

Abstract: I derive general conditions in order to explain the origin of the Vainshtein radius inside dRGT. The set of equations, which I have called "Vainshtein" conditions are extremal conditions of the dynamical metric (g µν ) containing all the degrees of freedom of the theory. The Vainshtein conditions are able to explain the coincidence between the Vainshtein radius in dRGT and the scale r 0 = 3 2 r s r 2 Λ

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Cited by 1 publication
(4 citation statements)
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“…[26,27], the Schwarzschild(-de Sitter) solutions in ref. [76][77][78][79], the LTB solution in ref. [27], and the RN solution in ref.…”
Section: Conclusion and Discussionmentioning
confidence: 99%
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“…[26,27], the Schwarzschild(-de Sitter) solutions in ref. [76][77][78][79], the LTB solution in ref. [27], and the RN solution in ref.…”
Section: Conclusion and Discussionmentioning
confidence: 99%
“…In the case of dRGT massive gravity, f µν is not a dynamical but a fixed metric, and hence we need not consider the equations of motion for f µν . The class of solutions with C(t, r) = 0 includes the cosmological solutions [26,27], the black hole solutions [76][77][78][79], the Lemaître-Tolman-Bondi (LTB) solution [27], and the Reissner-Nordström (RN) solution [77]. Since the equations of motion for g µν (and, in fact, those for f µν as well) reduce to the Einstein equations with a cosmological constant, any spherically symmetric solution in GR is also a solution of the one-parameter subclass (3.11) of bi-gravity and massive gravity with a suitable fiducial metric.…”
Section: Bi-spherically Symmetric Background Solutionsmentioning
confidence: 99%
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