Degrees of freedom in the curvature tensor

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SUMMARY

The discussion centers on the degrees of freedom in the Riemannian curvature tensor and the Einstein field equations (EFE) in four dimensions. The EFE has 10 degrees of freedom, while the Riemannian curvature tensor possesses 20 degrees of freedom. The traceless part of the curvature tensor, known as the Weyl tensor, accounts for the remaining degrees of freedom. The conversation raises the question of whether these additional degrees of freedom are determined by the EFE and their potential observable effects in physics.

PREREQUISITES
  • Understanding of Einstein field equations (EFE)
  • Familiarity with Riemannian geometry
  • Knowledge of curvature tensors, specifically the Riemannian and Weyl tensors
  • Basic grasp of differential geometry concepts
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This discussion is beneficial for theoretical physicists, mathematicians specializing in geometry, and students studying general relativity who seek a deeper understanding of curvature tensors and their implications in physics.

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The Einstein field equations (EFE) in 4 dimensions have 10 degrees of freedom; The Riemannian curvature tensor in 4 dimensions has 20. If I understood this correctly, one can split up the curvature tensor and describe the remaining degrees of freedom by its traceless part, which is called the Weyl tensor.

I wonder now if these remaining degrees of freedom are actually determined by the EFE, because the metric is uniquely determined, and the full curvature tensor is defined completely by derivatives of the metric. So my question is, what is the solution to this (apperent only, i guess) contradiction 10 vs. 20 degrees of freedom?

And in case some degrees of freedom of the curvature tensor do remain undetermined by the EFE, can they have an observable effect on physics?

Thanks for your answers.
 
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