REDUCTION OF THE TWO-BODY PROBLEM WITH SPIN IN (2+1)-DIMENSIONAL GRAVITY

1993 ◽  
Vol 08 (26) ◽  
pp. 2503-2508 ◽  
Author(s):  
F. MANSOURI ◽  
M.K. FALBO-KENKEL

The two-body problem with spin in (2+1)-dimensional gravity is analyzed nonperturbatively. Utilizing topological methods similar to those used in the reduction of the spinless case, we show that the general two-body problem with spin can again be reduced to an equivalent one-body formalism. We give exact expressions for the mass and spin of the reduced problem.

1992 ◽  
Vol 07 (24) ◽  
pp. 2173-2178 ◽  
Author(s):  
M. K. FALBO-KENKEL ◽  
F. MANSOURI

By a suitable choice of phase space variables, which is natural for the reduction of a two-body problem, we couple two sources to the Chern-Simons-Witten action and obtain the exact two-body Hamiltonian. For particles of (nearly) equal mass and of small momenta, the Hamiltonian reduces to that of 't Hooft. In the corresponding geometry, when viewed from a particular frame, the relative coordinate moves on a cone of deficit angle equal to the classical Hamiltonian.


Author(s):  
Nathalie Deruelle ◽  
Jean-Philippe Uzan

This chapter embarks on a study of the two-body problem in general relativity. In other words, it seeks to describe the motion of two compact, self-gravitating bodies which are far-separated and moving slowly. It limits the discussion to corrections proportional to v2 ~ m/R, the so-called post-Newtonian or 1PN corrections to Newton’s universal law of attraction. The chapter first examines the gravitational field, that is, the metric, created by the two bodies. It then derives the equations of motion, and finally the actual motion, that is, the post-Keplerian trajectories, which generalize the post-Keplerian geodesics obtained earlier in the chapter.


Author(s):  
Nathalie Deruelle ◽  
Jean-Philippe Uzan

This chapter presents the basics of the ‘effective-one-body’ approach to the two-body problem in general relativity. It also shows that the 2PN equations of motion can be mapped. This can be done by means of an appropriate canonical transformation, to a geodesic motion in a static, spherically symmetric spacetime, thus considerably simplifying the dynamics. Then, including the 2.5PN radiation reaction force in the (resummed) equations of motion, this chapter provides the waveform during the inspiral, merger, and ringdown phases of the coalescence of two non-spinning black holes into a final Kerr black hole. The chapter also comments on the current developments of this approach, which is instrumental in building the libraries of waveform templates that are needed to analyze the data collected by the current gravitational wave detectors.


2011 ◽  
Author(s):  
A. A. Kosti ◽  
Z. A. Anastassi ◽  
T. E. Simos ◽  
Theodore E. Simos ◽  
George Psihoyios ◽  
...  

1982 ◽  
Vol 25 (12) ◽  
pp. 3433-3437 ◽  
Author(s):  
Martin Walker ◽  
Clifford M. Will

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