2006
DOI: 10.1007/s10714-006-0358-2
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Electromagnetic quasinormal modes of D-dimensional black holes

Abstract: Using the monodromy method we calculate the asymptotic quasinormal (QN) frequencies of an electromagnetic field moving in D-dimensional Schwarzschild and Schwarzschild de Sitter (SdS) black holes (D ≥ 4). For the D-dimensional Schwarzschild anti-de Sitter (SadS) black hole we also compute these frequencies with a similar method. Moreover, we calculate the electromagnetic normal modes of the D-dimensional anti-de Sitter (AdS) spacetime.

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Cited by 47 publications
(57 citation statements)
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“…Another important direction of research is to study the quasinormal modes in higher dimensions. The results obtained in these directions so far restricts mainly to non-rotating (or not generally rotating) black holes (see, e.g., [112], [20], [21], [22], [23], [142], [143], [23], [24], [237], [127], [165], [164], [166], [144], [167], [138], [140], [34], [184], and references therein).…”
Section: Discussionmentioning
confidence: 99%
“…Another important direction of research is to study the quasinormal modes in higher dimensions. The results obtained in these directions so far restricts mainly to non-rotating (or not generally rotating) black holes (see, e.g., [112], [20], [21], [22], [23], [142], [143], [23], [24], [237], [127], [165], [164], [166], [144], [167], [138], [140], [34], [184], and references therein).…”
Section: Discussionmentioning
confidence: 99%
“…Generic master equations governing the highly-damped quasi-normal frequencies [QNFs] of one-horizon, two-horizon, and even three-horizon spacetimes can be obtained through either semi-analytic [1,2,3] or monodromy techniques [4,5,6,7,8,9,10,11,12,13,14,15,16]. (For general background, see also [17,18,19,20,21,22,23,24,25,26,27].)…”
Section: Introductionmentioning
confidence: 99%
“…[17] we showed that the modes I and II of the electromagnetic field have a different spectrum of the de Sitter QN frequencies (for fixed angular momentum number l, the QN frequencies have different parity in odd dimensions, while in even dimensions a finite number of QN frequencies, which depend on the spacetime dimension, are different). 7 For the massless Dirac field propagating in the BTZ black hole we can simplify the equations of motion to Schrödinger type equations with effective potentials equal to (see expression (74) in [17] and Ref. [35])…”
mentioning
confidence: 99%