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Self-force regularization in the Schwarzschild spacetime

Wataru Hikida1, Hiroyuki Nakano2 and Misao Sasaki1

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We discuss the gravitational self-force on a particle in a black-hole spacetime. For a point particle, the full (bare) self-force diverges. The metric perturbation induced by a particle can be divided into two parts, the direct part (or the S part) and the tail part (or the R part), in the Lorenz gauge, and the regularized self-force is derived from the R part which is regular and satisfies the source-free perturbed Einstein equations. But this formulation is abstract, so when we apply it to black-hole-particle systems, there are many problems to be overcome in order to derive a concrete self-force. These problems are roughly divided into two parts. They are the problem of regularizing the divergent self-force, i.e., 'subtraction problem' and the problem of the singularity in gauge transformation, i.e., 'gauge problem'. In this paper, we discuss these problems in the Schwarzschild background and report some recent progress.


PACS

04.70.Bw Classical black holes

04.25.Nx Post-Newtonian approximation; perturbation theory; related approximations

MSC

83C05 Einstein's equations (general structure, canonical formalism, Cauchy problems)

83C57 Black holes

Subjects

Gravitation and cosmology

Dates

Issue 15 (7 August 2005)

Received 2 December 2004, in final form 23 March 2005

Published 18 July 2005



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