TY - JOUR
T1 - A proof of Price's Law on Schwarzschild black hole manifolds for all angular momenta
AU - Donninger, Roland
AU - Schlag, Wilhelm
AU - Soffer, Avy
N1 - Funding Information:
* Corresponding author. E-mail addresses: donninger@uchicago.edu (R. Donninger), schlag@math.uchicago.edu (W. Schlag), soffer@math.rutgers.edu (A. Soffer). 1 The author is an Erwin Schrödinger Fellow of the FWF (Austrian Science Fund) Project No. J2843 and he wants to thank Peter C. Aichelburg for his support. Furthermore, all three authors would like to thank Piotr Bizoń for a number of helpful remarks on a first version of this paper. 2 The author was partly supported by the National Science Foundation DMS-0617854. 3 The author wants to thank A. Ori and T. Damour for helpful discussions, the IHES France for the invitation and the NSF DMS-0903651 for partial support.
PY - 2011/1/15
Y1 - 2011/1/15
N2 - Price's Law states that linear perturbations of a Schwarzschild black hole fall off as t-2ℓ-3 for t→∞ provided the initial data decay sufficiently fast at spatial infinity. Moreover, if the perturbations are initially static (i.e., their time derivative is zero), then the decay is predicted to be t-2ℓ-4. We give a proof of t-2ℓ-2 decay for general data in the form of weighted L1 to L∞ bounds for solutions of the Regge-Wheeler equation. For initially static perturbations we obtain t-2ℓ-3. The proof is based on an integral representation of the solution which follows from self-adjoint spectral theory. We apply two different perturbative arguments in order to construct the corresponding spectral measure and the decay bounds are obtained by appropriate oscillatory integral estimates.
AB - Price's Law states that linear perturbations of a Schwarzschild black hole fall off as t-2ℓ-3 for t→∞ provided the initial data decay sufficiently fast at spatial infinity. Moreover, if the perturbations are initially static (i.e., their time derivative is zero), then the decay is predicted to be t-2ℓ-4. We give a proof of t-2ℓ-2 decay for general data in the form of weighted L1 to L∞ bounds for solutions of the Regge-Wheeler equation. For initially static perturbations we obtain t-2ℓ-3. The proof is based on an integral representation of the solution which follows from self-adjoint spectral theory. We apply two different perturbative arguments in order to construct the corresponding spectral measure and the decay bounds are obtained by appropriate oscillatory integral estimates.
KW - Dispersive estimates for wave equation
KW - Schwarzschild black hole
KW - Spectral and scattering theory
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U2 - 10.1016/j.aim.2010.06.026
DO - 10.1016/j.aim.2010.06.026
M3 - Article
AN - SCOPUS:77958476020
SN - 0001-8708
VL - 226
SP - 484
EP - 540
JO - Advances in Mathematics
JF - Advances in Mathematics
IS - 1
ER -