Abstract

We discuss various aspects of the post-Newtonian approximation in general relativity. After presenting the foundation based on the Newtonian limit, we show a method to derive post-Newtonian equations of motion for relativistic compact binaries based on a surface integral approach and the strong field point particle limit. As an application we derive third post-Newtonian equations of motion for relativistic compact binaries which respect the Lorentz invariance in the post-Newtonian perturbative sense, admit a conserved energy, and are free from any ambiguity.

Highlights

  • Because a Living Reviews article can evolve over time, we recommend to cite the article as follows: Toshifumi Futamase and Yousuke Itoh, “The Post-Newtonian Approximation for Relativistic Compact Binaries”, Living Rev

  • Using the so-obtained RA-independent field, we evaluate the surface integrals in the general form of the 3 PN equations of motion by discarding the RA dependence emerging from the surface integrals, and obtain the equations of motion

  • The surface integral approach is achieved by using the local conservation of the energy momentum, which led us to the general form of the equations of motion that are expressed entirely in terms of surface integrals

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Summary

Gravitational wave detection and post-Newtonian approximation

The motion and associated emission of gravitational waves (GW) of self-gravitating systems have been a main research interest in general relativity. The most systematic among those works that have succeeded in achieving higher order iteration are the ones by Blanchet, Damour, and Iyer who have developed a scheme to calculate the waveform at a higher order, where the post-Minkowskian approximation is used to construct the external field and the post-Newtonian approximation is used to construct the field near the material source They and their collaborators have obtained the waveform up to 3.5 PN order which is of order 7 higher than the lowest quadrupole wave [23, 24, 29, 31, 32] by using the equations of motion up to that order [22, 91, 93, 111, 123, 130].

Post-Newtonian equations of motion
Plan of this paper
Foundation of the Post-Newtonian Approximation
Newtonian limit along a regular asymptotic Newtonian sequence
Post-Newtonian hierarchy
Explicit calculation in harmonic coordinates
Post-Newtonian Equations of Motion for Compact Binaries
Strong field point particle limit
Surface integral approach and body zone
Scalings on the initial hypersurface
Newtonian equations of motion for extended bodies
Formulation
Field equations
Near zone contribution
ZAkij rAk rA3
Lorentz contraction and multipole moments
General form of the equations of motion
On the arbitrary constant RA
RA dependence of the field
RA dependence of the equations of motion
Newtonian equations of motion
First post-Newtonian equations of motion
Body zone boundary dependent terms
Third Post-Newtonian Gravitational Field
Super-potential method
Super-potential-in-series method
Direct-integration method
Third Post-Newtonian Mass-Energy Relation
Meaning of PAτΘ
P2τ r12
Third Post-Newtonian Momentum-Velocity Relation
Third post-Newtonian equations of motion with logarithmic terms
PN field affects the
Arbitrary constant RA
Consistency relation
Third post-Newtonian equations of motion
Comparison
Summary
Going further
Spin-orbit coupling force
Spin-spin coupling force
Quadrupole-orbit coupling force
Spin geodesic precession
Remarks
Introduction
Equations of motion
Full Text
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