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      Gravitational self-force correction to the innermost stable circular orbit of a Schwarzschild black hole

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          Abstract

          The innermost stable circular orbit (ISCO) of a test particle around a Schwarzschild black hole of mass \(M\) has (areal) radius \(r_{\rm isco}= 6M G/c^2\). If the particle is endowed with mass \(\mu(\ll M)\), it experiences a gravitational self-force whose conservative piece alters the location of the ISCO. Here we calculate the resulting shifts \(\Delta r_{\rm isco}\) and \(\Delta\Omega_{\rm isco}\) in the ISCO's radius and frequency, at leading order in the mass ratio \(\mu/M\). We obtain, in the Lorenz gauge, \(\Delta r_{\rm isco}=-3.269 (\pm 0.003)\mu G/c^2\) and \(\Delta\Omega_{\rm isco}/\Omega_{\rm isco}=0.4870 (\pm 0.0006) \mu/M\). We discuss the implications of our result within the context of the extreme-mass-ratio binary inspiral problem.

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          A consequence of the gravitational self-force for circular orbits of the Schwarzschild geometry

          A small mass \mu in orbit about a much more massive black hole M moves along a world line that deviates from a geodesic of the black hole geometry by O(\mu/M). This deviation is said to be caused by the gravitational self-force of the metric perturbation h_{ab} from \mu. For circular orbits about a non-rotating black hole we numerically calculate the O(\mu/M) effects upon the orbital frequency and upon the rate of passage of proper time on the worldline. These two effects are independent of the choice of gauge for h_{ab} and are observable in principle. For distant orbits, our numerical results agree with a post-Newtonian analysis including terms of order (v/c)^6.
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            Calculating the gravitational self force in Schwarzschild spacetime

            We present a practical method for calculating the local gravitational self-force (often called ``radiation-reaction force'') for a pointlike particle orbiting a Schwarzschild black hole. This is an implementation of the method of {\it mode-sum regularization}, in which one first calculates the (finite) contribution to the force due to each individual multipole mode of the perturbation, and then applies a certain regularization procedure to the mode sum. Here we give the values of all the ``regularization parameters'' required for implementing this regularization procedure, for any geodesic orbit in Schwarzschild spacetime.
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              Mode sum regularization approach for the self-force in black hole spacetime

              We present a method for calculating the self-force (the ``radiation reaction force'') acting on a charged particle moving in a strong field orbit in black hole spacetime. In this approach, one first calculates the contribution to the self-force due to each multipole mode of the particle's field. Then, the sum over modes is evaluated, subject to a certain regularization procedure. Here we develop this regularization procedure for a scalar charge on a Schwarzschild background, and present the results of its implementation for radial trajectories (not necessarily geodesic).
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                Author and article information

                Journal
                03 February 2009
                2009-04-22
                Article
                10.1103/PhysRevLett.102.191101
                0902.0573
                65b04072-f599-4c06-9178-bd3b4d7fe8ff

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                Phys.Rev.Lett.102:191101,2009
                4 pages. v2: Added clarifications re. the definition of the conservative self-force and the gauge dependence of the frequency; some other minor changes. Accepted for publication in PRL
                gr-qc astro-ph.HE

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