2023
DOI: 10.1007/s00220-023-04776-9
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Analyticity of Quasinormal Modes in the Kerr and Kerr–de Sitter Spacetimes

Abstract: We prove that quasinormal modes (or resonant states) for linear wave equations in the subextremal Kerr and Kerr–de Sitter spacetimes are real analytic. The main novelty of this paper is the observation that the bicharacteristic flow associated to the linear wave equations for quasinormal modes with respect to a suitable Killing vector field has a stable radial point source/sink structure rather than merely a generalized normal source/sink structure. The analyticity then follows by a recent result in the microl… Show more

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Cited by 3 publications
(3 citation statements)
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“…we conclude that ker(P σ ) is non-trivial precisely on a discrete set A ⊂ C. Following the arguments in the proof of[7, Theorem 1.2] line by line, using Theorem 3.1 in place of the [8, Theorem 1.1], it follows that the elements in ker(P σ ) are real analytic if the coefficients of P are real analytic. ■Proof of Theorem 1.13.…”
mentioning
confidence: 68%
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“…we conclude that ker(P σ ) is non-trivial precisely on a discrete set A ⊂ C. Following the arguments in the proof of[7, Theorem 1.2] line by line, using Theorem 3.1 in place of the [8, Theorem 1.1], it follows that the elements in ker(P σ ) are real analytic if the coefficients of P are real analytic. ■Proof of Theorem 1.13.…”
mentioning
confidence: 68%
“…The bicharacteristic flow at the event horizon is, however, slightly different. Though a similar computation was already done in the proof of [7,Theorem 1.7], let us explicitly compute the Hamiltonian vector field at N * {r = r e } in case r 0 = r e . The principal symbol p σ of P σ is given by In particular, P σ is invertible everywhere in Ω s apart form a discrete set.…”
Section: Fredholm Theorymentioning
confidence: 99%
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