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Phys. Rev. D 80, 084021 (2009) [22 pages]

Self-force with (3+1) codes: A primer for numerical relativists

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Ian Vega1, Peter Diener2,3, Wolfgang Tichy4, and Steven Detweiler1
1Institute for Fundamental Theory, Department of Physics, University of Florida, Gainesville, Florida 32611-8440, USA
2Center for Computation and Technology, Louisiana State University, Baton Rouge, Louisiana 70803, USA
3Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA
4Department of Physics, Florida Atlantic University, Boca Raton, Florida 33431, USA

Received 29 August 2009; published 15 October 2009

Prescriptions for numerical self-force calculations have traditionally been designed for frequency-domain or (1+1) time-domain codes which employ a mode decomposition to facilitate in carrying out a delicate regularization scheme. This has prevented self-force analyses from benefiting from the powerful suite of tools developed and used by numerical relativists for simulations of the evolution of comparable-mass black hole binaries. In this work, we revisit a previously-introduced (3+1) method for self-force calculations and demonstrate its viability by applying it to the test case of a scalar charge moving in a circular orbit around a Schwarzschild black hole. Two (3+1) codes originally developed for numerical relativity applications were independently employed, and in each we were able to compute the two independent components of the self-force and the energy flux correctly to within <1%. We also demonstrate consistency between the t component of the self-force and the scalar energy flux. Our results constitute the first successful calculation of a self-force in a (3+1) framework, and thus open opportunities for the numerical relativity community in self-force analyses and the perturbative modeling of extreme-mass-ratio inspirals.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevD.80.084021
DOI:
10.1103/PhysRevD.80.084021
PACS:
04.25.D−, 04.25.dg, 04.25.Nx, 04.20.Cv

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