Big Bang: A True Singularity That is Coordinate Independent

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SUMMARY

The discussion centers on the nature of the Big Bang singularity, emphasizing its coordinate independence. It highlights that while the singularity at \(t=0\) may appear coordinate dependent, it is essential to rigorously analyze curvature invariants to confirm its true singularity status. The Kretschmann scalar, derived from the Riemann tensor, is identified as a critical invariant that should diverge at genuine curvature singularities, thereby affirming the Big Bang as a true singularity.

PREREQUISITES
  • Understanding of the Robertson-Walker metric
  • Familiarity with curvature invariants in differential geometry
  • Knowledge of the Riemann tensor and its properties
  • Concept of diffeomorphism invariance in general relativity
NEXT STEPS
  • Research the properties of the Kretschmann scalar in general relativity
  • Study the implications of curvature invariants on singularities
  • Examine the role of the Ricci tensor in cosmological models
  • Explore various coordinate systems in the context of general relativity
USEFUL FOR

The discussion is beneficial for theoretical physicists, cosmologists, and students of general relativity who are investigating the nature of singularities and the mathematical frameworks that describe them.

victorvmotti
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Consider a flat Robertson-Walker metric.

When we say that there is a singularity at

$$t=0$$

Clearly it is a coordinate dependent statement. So it is a "candidate" singularity.

In principle there is "another coordinate system" in which the corresponding metric has no singularity as we approach that point in the manifold.

However, we know that Big Bang is "a true" singularity, but how should we test that?

Is it intuitively self-evident, or should we check rigorously all scalars based on the Ricci tensor? If so "which order of scalar" goes to infinity at that point called Big Bang?
 
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The idea is to examine a curvature invariant: a quantity built out of the various curvature tensors that is diffeomorphism invariant (unchanged by coordinate transformation). These should be infinite at true curvature singularities. One such invariant, the Kretschmann scalar, is found from the Riemann tensor, K = R_{\mu \nu \rho \sigma}R^{\mu \nu \rho \sigma}.
 

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