1,720,965 research outputs found

    Quantitative Mode Stability for the Wave Equation on the Kerr Spacetime

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    We give a quantitative refinement and simple proofs of mode stability type statements for the wave equation on Kerr backgrounds in the full sub-extremal range (|a| <  M). As an application, we are able to quantitatively control the energy flux along the horizon and null infinity and establish integrated local energy decay for solutions to the wave equation in any bounded-frequency regime. Keywords: Black Hole, Wave Equation, Half Plane, Quasinormal Mode, Mode Stabilit

    Exponentially Growing Finite Energy Solutions for the Klein–Gordon Equation on Sub-Extremal Kerr Spacetimes

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    For any sub-extremal Kerr spacetime with non-zero angular momentum, we find an open family of non-zero masses for which there exist smooth, finite energy, and exponentially growing solutions to the corresponding Klein–Gordon equation. If desired, for any non-zero integer m, an exponentially growing solution can be found with mass arbitrarily close to |am|/2Mr+. In addition to its direct relevance for the stability of Kerr as a solution to the Einstein–Klein–Gordon system, our result provides the first rigorous construction of a superradiant instability. Finally, we note that this linear instability for the Klein–Gordon equation contrasts strongly with recent work establishing linear stability for the wave equation.National Science Foundation (U.S.) (Grant DMS-0943787

    On the Scattering Theory for Schwarzschild

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    The wave equation on the exterior of a Schwarzschild black hole

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    This thesis investigates a wave equation on the Minkowski and Schwarzschild spacetimes. We rely on the vector field method and the rp-weighted inequalities discovered by Dafermos and Rodnianski to show the decay of energy and solutions in the cases studied

    Twisted Self-Similarity and the Einstein Vacuum Equations

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    In the previous works [I. Rodnianski and Y. Shlapentokh-Rothman, Naked Singularities for the Einstein Vacuum Equations: The Exterior Solution, arXiv:1912.08478 and Y. Shlapentokh-Rothman, Naked Singularities for the Einstein Vacuum Equations: The Interior Solution, arXiv:2204.09891] we have introduced a new type of self-similarity for the Einstein vacuum equations characterized by the fact that the homothetic vector field may be spacelike on the past light cone of the singularity. In this work we give a systematic treatment of this new self-similarity. In particular, we provide geometric characterizations of spacetimes admitting the new symmetry and show the existence and uniqueness of formal expansions around the past null cone of the singularity which may be considered analogues of the well-known Fefferman--Graham expansions. In combination with previous results, our analysis will show that the twisted self-similar solutions are sufficiently general to describe all possible asymptotic behaviors for spacetimes in the small data regime which are self-similar and whose homothetic vector field is everywhere spacelike on an initial spacelike hypersurface. We present an application of this later fact to the understanding of the global structure of Fefferman--Graham spacetimes and the naked singularity exteriors of [I. Rodnianski and Y. Shlapentokh-Rothman, Naked Singularities for the Einstein Vacuum Equations: The Exterior Solution, arXiv:1912.08478]. Lastly, we observe that by an amalgamation of techniques from previous works, one may associate true solutions to the Einstein vacuum equations to each of our formal expansions in a suitable region of spacetime.Comment: 45 pages, 5 figures, final versio

    Mode stabilities and instabilities for scalar fields on Kerr exterior spacetimes

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    Thesis: Ph. D., Massachusetts Institute of Technology, Department of Mathematics, 2015.Cataloged from PDF version of thesis.Includes bibliographical references (pages 131-136).In this thesis we study wave and Klein-Gordon equations on Kerr exterior spacetimes. For the wave equation, we give a quantitative refinement and simple proofs of mode stability type statements on Kerr backgrounds in the full sub-extremal range ([absolute value of]a < M). As an application, we are able to quantitatively control the energy flux along the horizon for solutions to the wave equation in any bounded-frequency regime. This estimate plays a crucial role in the author's recent proof, joint with Mihalis Dafermos and Igor Rodnianski, of boundedness and decay for the solutions to the wave equation on the full range of sub-extremal Kerr spacetimes. For the Klein-Gordon equation, we show that given any Kerr exterior spacetime with non-zero angular momentum, we may find an open family of non-zero Klein-Gordon masses for which there exist smooth, finite energy, and exponentially growing solutions to the corresponding Klein-Gordon equation. If desired, for any non-zero integer m, an exponentially growing solution can be found with mass arbitrarily close to [absolute value of]am/2Mr+.by Yakov Shlapentokh-Rothman.Ph. D

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    The weak cosmic censorship conjecture posits that, generically, all singularities in General Relativity arising from regular asymptotically flat initial data should have a complete future null infinity. While this conjecture remains wide open, it has inspired many mathematical works concerning topics such as trapped surface formation and the construction of naked singularities. In this article we will review some of these works and attempt to emphasize their interconnectedness

    Naked Singularities for the Einstein Vacuum Equations: The Exterior Solution

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    In this work we initiate the mathematical study of naked singularities for the Einstein vacuum equations in 3+13+1 dimensions by constructing solutions which correspond to the exterior region of a naked singularity. A key element is our introduction of a new type of self-similarity for the Einstein vacuum equations. Connected to this is a new geometric twisting phenomenon which plays the leading role in singularity formation. Prior to this work, the only known examples of naked singularities were the solutions constructed by Christodoulou for the spherically symmetric Einstein-scalar-field system, as well as other solutions explored numerically for either the spherically symmetric Einstein equations coupled to suitable matter models or for the Einstein equations in higher dimensions.Comment: 116 pages, final versio

    Polynomial time decay for solutions of the Klein--Gordon equation on a subextremal Reissner--Nordstr\"{o}m black hole

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    We consider the massive scalar field equation gRNϕ=m2ϕ\Box_{g_{RN}} \phi = m^2 \phi on any subextremal Reissner--Nordstr\"{o}m exterior metric gRNg_{RN}. We prove that solutions with localized initial data decay pointwise-in-time at the polynomial rate t56+δt^{-\frac{5}{6}+\delta} in any spatially compact region (including the event horizon), for some small δ123 \delta\leq \frac{1}{23} . Moreover, assuming the validity of the Exponent Pair Conjecture on exponential sums in Number Theory, our result implies that decay upper bounds hold at the rate t56+ϵt^{-\frac{5}{6}+\epsilon}, for any arbitrarily small ϵ>0\epsilon>0. In our previous work, we proved that each fixed angular mode decays at the exact rate t56t^{-\frac{5}{6}}, thus the upper bound t56+ϵt^{-\frac{5}{6}+\epsilon} is sharp, up to a tϵt^{\epsilon} loss. Without the restriction to a fixed angular mode, the solution turns out to have an unbounded Fourier transform due to discrete frequencies associated to quasimodes, and caused by the occurrence of stable timelike trapping. Our analysis nonetheless shows that inverse-polynomial asymptotics in tt still hold after summing over all angular modes.Comment: 76 pages, 2 figure
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