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A new method to integrate (2+1)-wave equations with Dirac's delta functions as sources

Carlos O Lousto and Hiroyuki Nakano

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Unlike in the Schwarzschild black hole background, gravitational perturbations in a Kerr black hole background cannot be decomposed into simple tensor harmonics in the time domain. Here, we make mode decompositions only in the azimuthal direction. As a first step, we discuss the resulting (2+1)-dimensional Klein–Gordon differential equation for scalar perturbations with a two-dimensional Dirac's δ-function as a source representing a point particle orbiting a much larger black hole. To make this equation amenable for numerical integrations we explicitly remove analytically the singular behavior of the source and compute a global, well-behaved, effective source for the corresponding waveform.


PACS

04.70.-s Physics of black holes

04.25.-g Approximation methods; equations of motion

MSC

83C57 Black holes

Subjects

Gravitation and cosmology

Dates

Issue 14 (21 July 2008)

Received 29 February 2008, in final form 21 May 2008

Published 30 June 2008



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