2000
DOI: 10.1103/physrevd.62.024027
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Quasinormal modes of AdS black holes and the approach to thermal equilibrium

Abstract: We investigate the decay of a scalar field outside a Schwarzschild anti de Sitter black hole. This is determined by computing the complex frequencies associated with quasinormal modes. There are qualitative differences from the asymptotically flat case, even in the limit of small black holes. In particular, for a given angular dependence, the decay is always exponential -there are no power law tails at late times. In terms of the AdS/CFT correspondence, a large black hole corresponds to an approximately therma… Show more

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Cited by 871 publications
(1,479 citation statements)
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References 32 publications
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“…In addition to these large r boundary conditions, we must also demand that our solution be smooth across the horizon at r = a in order to uniquely determine a solution. As shown in [19], this condition is equivalent to demanding the presence of purely ingoing modes at the future horizon.…”
Section: Jhep04(2009)048mentioning
confidence: 99%
“…In addition to these large r boundary conditions, we must also demand that our solution be smooth across the horizon at r = a in order to uniquely determine a solution. As shown in [19], this condition is equivalent to demanding the presence of purely ingoing modes at the future horizon.…”
Section: Jhep04(2009)048mentioning
confidence: 99%
“…Differentiating this equation with respect to τ and using τ t in the nonrelativistic limit, one gets 45) which is nothing but the Newton's law of gravitation. Thus, M in the Schwarzschild black hole (2.30) represents the black hole mass.…”
Section: Particle Motionmentioning
confidence: 99%
“…By the S 1 -compactification, the five-dimensional 13 Quasinormal mode computations are traditionally carried out for asymptotically flat black holes, and one imposes the "outgoing-wave" boundary condition at r → ∞. But it is natural to impose the Dirichlet condition for an asymptotically AdS spacetime [45] since the spacetime has a potential barrier by the cosmological constant (Sect. 6.2).…”
Section: Perturbation Equationmentioning
confidence: 99%
“…From equation (3.29), we get that the Wronskian between Ψ I , Ψ II is W = aω(k)Ψ I /(r − r 0 ). Using (3.34) we then find that for r > r 0 , 48) where the function aω depends only on k = k 2 1 + k 2 2 + k 2 3 . At r ∼ r 0 , recall we have from eq.…”
Section: Yukawa-like Potential At Large Distancesmentioning
confidence: 99%
“…This method is an extension of a Frobenius expansion used originally in refs. [48][49][50] (see also ref. [44] for a review).…”
Section: Determination Of Eigenmodes By Frobenius Expansionsmentioning
confidence: 99%