2016
DOI: 10.1016/j.jfa.2016.06.013
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Instability results for the wave equation in the interior of Kerr black holes

Abstract: We prove that a large class of smooth solutions ψ to the linear wave equation g ψ = 0 on subextremal rotating Kerr spacetimes which are regular and decaying along the event horizon become singular at the Cauchy horizon. More precisely, we show that assuming appropriate upper and lower bounds on the energy along the event horizon, the solution has infinite (non-degenerate) energy on any spacelike hypersurfaces intersecting the Cauchy horizon transversally. Extrapolating from known results in the Reissner-Nordst… Show more

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Cited by 52 publications
(73 citation statements)
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“…See also upcoming results by Franzen [26]. The above inextendibility result (Theorem B) has been extended to subextremal Kerr by Luk-Sbierski [38], under suitable lower bound assumptions for solutions to (1.1) along the event horizon. A similar inextendibility result has also been obtained by Dafermos-Shlapentokh-Rothman via a scattering theory approach [23].…”
Section: Previous Results For the Linear Wave Equation On Black Hole mentioning
confidence: 89%
“…See also upcoming results by Franzen [26]. The above inextendibility result (Theorem B) has been extended to subextremal Kerr by Luk-Sbierski [38], under suitable lower bound assumptions for solutions to (1.1) along the event horizon. A similar inextendibility result has also been obtained by Dafermos-Shlapentokh-Rothman via a scattering theory approach [23].…”
Section: Previous Results For the Linear Wave Equation On Black Hole mentioning
confidence: 89%
“…Proof. As was already pointed out in [27] and also [47], in Kerr spacetime, by ϕ τ and ϕ φ we denote diffeomorphisms generated by the Killing fields ∂ t and ∂ φ , respectively. These contain the diffeomorphisms generated by T H + , defined in (C3).…”
Section: Statement Of the Theorem And Outline Of The Proof In The Neimentioning
confidence: 93%
“…In the following we will carry out the coordinate transformation (r, t, φ, θ) → (u, v,φ, θ ), since double null coordinates will turn out more convenient for our interior analysis. Using (46), (47) and dt = dv − du in (23) we obtain…”
Section: Eddington-finkelstein Normalized Double Null Coordinatesmentioning
confidence: 99%
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