2020
DOI: 10.1140/epjc/s10052-020-7909-7
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Schwarzschild-like black holes: Light-like trajectories and massless scalar absorption

Abstract: Black holes are among the most intriguing objects in nature. They are believed to be fully described by General Relativity (GR), and the astrophysical black holes are expected to belong to the Kerr family, obeying the nohair theorems. Alternative theories of gravity or parameterized deviations of GR allow black hole solutions, which have additional parameters other than mass and angular momentum. We analyze a Schwarzschild-like metric, proposed by Johannsen and Psaltis, characterized by its mass and a deformat… Show more

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Cited by 20 publications
(19 citation statements)
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“…It is well-known that for a spherically symmetric blackhole the zero-frequency limit of the absorption cross section associated with a minimally coupled massless scalar field coincides with the area of its event horizon [41]. See also [42,43]. Equation (57) shows that using the extreme lowenergy scattering data for a massless field the observer O + cannot distinguish between the wormhole and a blackhole with event horizon area A (radius ρ).…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…It is well-known that for a spherically symmetric blackhole the zero-frequency limit of the absorption cross section associated with a minimally coupled massless scalar field coincides with the area of its event horizon [41]. See also [42,43]. Equation (57) shows that using the extreme lowenergy scattering data for a massless field the observer O + cannot distinguish between the wormhole and a blackhole with event horizon area A (radius ρ).…”
Section: Discussionmentioning
confidence: 99%
“…The behavior of the absorption cross section of more general blackholes for low-energy massless scalar fields has been investigated in Refs. [41][42][43].…”
Section: Introductionmentioning
confidence: 99%
“…It is important to point out that for positive values of the parameter 3 , the line element (3) has only one singularity, located at r = 0, while for negative values of 3 , the line element has an additional singularity at r = | 3 | 1/3 M [12,29]. If the parameter 3 is sufficiently negative, namely 3 ≤ −8, the singularity lies outside ( 3 < −8) or on ( 3 = −8) the event horizon.…”
Section: Non-schwarzschild Spacetimementioning
confidence: 99%
“…In particular, two processes, namely the absorption and scattering of fundamental fields by BHs, have been studied over the years considering different fields propagating in various BH spacetimes [19][20][21][22][23][24][25][26][27]. More recently, the absorption of massless scalar waves by parameterized BHs has been investigated considering two distinct parametrized static solutions [28,29].…”
Section: Introductionmentioning
confidence: 99%

Scattering by deformed black holes

Magalhães,
Leite,
Crispino
2021
Preprint
Self Cite
“…Consequently, this effective idea of absorption and emission of particles in the strong gravity region gets physicist attentions [10][11][12][13][14][15]. There are stimulating phenomena between the interactions of fields and black holes such as scattering [16,17], emission [18][19][20][21][22][23][24] and absorption [25][26][27][28][29][30][31][32][33][34][35][36][37][38].…”
Section: Introductionmentioning
confidence: 99%