2018
DOI: 10.1142/s0218271818500347
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Quasinormal modes of black holes in Einstein-power-Maxwell theory

Abstract: In the present work we compute the spectrum of quasinormal frequencies of four-dimensional charged black holes in Einstein-power-Maxwell theory. In particular we study scalar perturbations adopting the 6th order WKB approximation. We analyze in detail the behaviour of the spectrum depending on the charge of the black hole, the quantum number of angular momentum and the overtone number. In addition, a comparison is made between the results obtained here and the results valid for charged black holes in other the… Show more

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Cited by 59 publications
(37 citation statements)
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“…The comparison of the analytical result with the numerical result was done in [35]. For more studies, see [36][37][38][39][40][41][42][43][44][45][46][47][48]. Adopting a similar radial coordinate, we are able to derive the analytical results for the greybody factors for arbitrary partial modes of a scalar field in the EGB-dS black hole spacetime as well.…”
Section: Introductionmentioning
confidence: 99%
“…The comparison of the analytical result with the numerical result was done in [35]. For more studies, see [36][37][38][39][40][41][42][43][44][45][46][47][48]. Adopting a similar radial coordinate, we are able to derive the analytical results for the greybody factors for arbitrary partial modes of a scalar field in the EGB-dS black hole spacetime as well.…”
Section: Introductionmentioning
confidence: 99%
“…The imaginary part becomes more and more negative with the electric charge, and less and less negative with the angular momentum, like in the RN case [82]. Notice that the characteristic minimum of the imaginary part (or maximum if one plots −Im(ω) versus q) for a certain value of the electric charge close to its extremal value is observed, like in the RN case (also observed in [76] for charged BHs in the EpM theory) and contrary to Born-Infeld NLE and Gauss-Bonnet gravity, where the imaginary part is a monotonic function of the electric charge [71,72].…”
Section: Numerical Resultsmentioning
confidence: 58%
“…[68][69][70][71][72][73], and for more recent works see e.g. [43,[74][75][76][77], and references therein. The QN frequencies may be computed using the formula…”
Section: Numerical Resultsmentioning
confidence: 99%
“…For an incomplete list see e.g. [97][98][99][100][101][102], and for more recent works [103][104][105][106][107], and references therein. The QN frequencies are given by where n = 0, 1, 2... is the overtone number, ν = n + 1/2, V 0 is the maximum of the effective potential, V 0 is the second derivative of the effective potential evaluated at the maximum, while Λ(n), Ω(n) are complicated expressions of ν and higher derivatives of the potential evaluated at the maximum, and can be seen e.g.…”
Section: Numerical Resultsmentioning
confidence: 99%