Linearized gravity / Linearized Einstein Field Equations / GEM

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SUMMARY

The discussion clarifies that "Linearized gravity," "Linearized Einstein Field Equations," and "GEM (gravitoelectrodynamics)" are mathematically distinct approximations of Einstein's full non-linear field equations. The order of approximation from least to most terms approximated away is not explicitly defined but is implied to be significant. The term "linearized gravity" is deprecated due to the existence of multiple classical relativistic field theories of gravitation. For strong-field general relativity (GR) verification, references to experimental data and arXiv eprints are provided, particularly highlighting the importance of the Bel decomposition of the Riemann tensor and its applicability to strong-field scenarios.

PREREQUISITES
  • Understanding of Einstein's General Relativity (GR)
  • Familiarity with the Einstein Field Equations (EFE)
  • Knowledge of gravitoelectrodynamics (GEM)
  • Basic grasp of Riemann tensor decomposition
NEXT STEPS
  • Research the differences between linearized and non-linear Einstein Field Equations
  • Study the Bel decomposition of the Riemann tensor in strong-field GR
  • Explore experimental tests of strong-field general relativity
  • Review relevant arXiv eprints on gravitoelectrodynamics and its applications
USEFUL FOR

Physicists, researchers in gravitational theory, and students of general relativity seeking to deepen their understanding of gravitational approximations and their experimental validations.

JustinLevy
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Are the phrases "Linearized gravity", "Linearized Einstein Field Equations", "GEM (gravitoelectrodynamics)", all referring to mathematically equivalent approximations of Einstein's full non-linear field equations?

If not, could someone tell me what order (in some rough sense) these would be listed in order of "approximating away" more terms from the full equations?

And is there any experimental data yet that let's us verify "strong field" GR as opposed to just weak field tests (ie. distinguish between the linear approximations and the full non-linear field equations)?
 
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I deprecate using the term "linearized gravity", since gtr is not the only theory of gravitation, not even the only classical relativistic field theory of gravitation, not even the only currently viable classical relativistic field theory of gravitation. However, the "linearized EFE" plays the same role in "linearized gtr" that the EFE plays in gtr proper.

There are several things one might mean by "gravitomagnetism"; see for example this review paper, which discusses two theories, one using the Bel decomposition of the Riemann tensor which always valid (in particular, works for strong-field gtr), and the other the GEM formalism which is indeed basically a reformulation of weak-field gtr (vacuum fields).

As for observational tests of strong-field gtr, see for example http://arxiv.org/abs/gr-qc/0402007
 
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