Metric matrix for binary star system?

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The discussion centers on the metric matrix for binary star systems, questioning whether each star follows its usual geodesic around the other. It highlights the absence of an exact two-body metric in General Relativity (GR), noting that an approximate metric exists for n-body systems based on harmonic coordinates. The 2000 IAU resolution provides a complex presentation of this metric, transitioning from a scalar gravitational vector potential to a four-vector potential. This change includes a scalar part and a three-vector part, with metric coefficients now expressed in terms of the four-potential. The conversation also references ongoing research into higher-order approximations for future experiments.
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What does the metric matrix look like for a binary star system? Does each follow its usual geodesic about the other? It seems like the solution would have to be different somehow than that for a tiny planet circling a big sun.
 
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There isn't any exact 2-body metric in GR. We do have an approximate metric for the n-body solar system, though, based on the theory of harmonic coordinates. I think it is of order 1.5. A terse and not terribly understandable presentation of the resulting metric can be found in the IAU (International Astronomical Union) resolution B1.3 for the year 2000, see for instance http://syrte.obspm.fr/IAU_resolutions/Resol-UAI.htm. There are a variety of sources that try to explain the resolution in more detail. See for instance "THE IAU 2000 RESOLUTIONS FOR ASTROMETRY, CELESTIAL MECHANICS, AND METROLOGY IN THE RELATIVISTIC FRAMEWORK: EXPLANATORY SUPPLEMENT", http://iopscience.iop.org/1538-3881/126/6/2687/fulltext/202343.text.html. The "explanations" are still not light reading.

An earlier (I forget the year) IAU version had a scalar gravitational vector potential u, which can be thought of as the Newtonian potential, defined by a Newtonian-like integral, and a set of corresponding metric coefficients. It is rather similar to the PPN formula you'll find in many papers and textbooks. The year 2000 version has a 4-vector potential, broken down by the resolution into a scalar part w, and a 3-vector part ##w^i##. The metric coefficeints are are written as functions of u (in the simple earlier version), and the 4-potential ##(w, w^i)## in the current 2000 version. There are already papers that discuss higher-order, higher accuracy approximations for some upcoming experiments
 
MOVING CLOCKS In this section, we show that clocks moving at high speeds run slowly. We construct a clock, called a light clock, using a stick of proper lenght ##L_0##, and two mirrors. The two mirrors face each other, and a pulse of light bounces back and forth betweem them. Each time the light pulse strikes one of the mirrors, say the lower mirror, the clock is said to tick. Between successive ticks the light pulse travels a distance ##2L_0## in the proper reference of frame of the clock...

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