In physics, precisely in the general theory of relativity, post-Minkowskian expansions (PM) or post-Minkowskian approximations are mathematical methods used to find approximate solutions of Einstein's equations by means of a power series development of the metric tensor.
Unlike post-Newtonian expansions (PN), in which the series development is based on a combination of powers of the velocity (which must be negligible compared to that of light) and the gravitational constant, in the post-Minkowskian case the developments are based only on the gravitational constant, allowing analysis even at velocities close to that of light (relativistic).[1]
0PN | 1PN | 2PN | 3PN | 4PN | 5PN | 6PN | 7PN | ||||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1PM | (1 | + | v2 | + | v4 | + | v6 | + | v8 | + | v10 | + | v12 | + | v14 | + | ...) | G1 | |
2PM | (1 | + | v2 | + | v4 | + | v6 | + | v8 | + | v10 | + | v12 | + | ...) | G2 | |||
3PM | (1 | + | v2 | + | v4 | + | v6 | + | v8 | + | v10 | + | ...) | G3 | |||||
4PM | (1 | + | v2 | + | v4 | + | v6 | + | v8 | + | ...) | G4 | |||||||
5PM | (1 | + | v2 | + | v4 | + | v6 | + | ...) | G5 | |||||||||
6PM | (1 | + | v2 | + | v4 | + | ...) | G6 | |||||||||||
Comparison table of powers used for PN and PM approximations in the case of two non-rotating bodies.0PN corresponds to the case of Newton's theory of gravitation. 0PM (not shown) corresponds to the Minkowski flat space.[2] |