Can Conformal Transformations Explain Torsion in Different Spacetimes?

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Conformal transformations (CTs) represent an actual change in geometry rather than merely a change of coordinates. They can transform Minkowski spacetime into Riemannian or Riemann-Cartan spacetimes, the latter of which exhibits torsion, unlike the torsion-free Minkowski spacetime. The discussion raises questions about the nature of torsion, suggesting it may not be an intrinsic geometrical quantity but rather a result of the CT. Additionally, the relationship between conformal mapping and torsion is questioned, indicating a need for clarification on how these concepts interact. Understanding these transformations is crucial for grasping the implications of torsion in different spacetimes.
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CTs are not a change of coordinates but an actual change of the geometry, right? In principle, we can change the Minkowski spacetime into Riemannian one even Riemann-Cartan one by some kind of CT. In the Riemann-Cartan spacetime there is torsion while it is torsion-free for Minkowski spacetime. So how do we understand the problem? Can we consider the torsion coming from the CT and torsion is not an intrinsic geometrical quantity ? Thanks for any reply!
 
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xiaomaclever said:
CTs are not a change of coordinates but an actual change of the geometry, right? In principle, we can change the Minkowski space-time into Riemann one even Riemann-Cartan one by some kind of CT. In the Riemann-Cartesian space-time there is torsion while it is torsion-free for Minkowski space time. So how do we understand the problem? Can we consider the torsion coming from the CT and torsion is not an intrinsic geometrical quantity ? Thanks for any reply!

1. It is a change of geometry not just coordinates.

2. Minkowski space has nothing to do with conformal mapping.

3. I have no idea what you are talking about when you mention torsion.
 
I'm not sure what you're looking for. But consider a coordinate system where the coordinates system XY is normal at all points, though not necessarily orthonormal. The off-diagonal elements of the metric are zero for all points (x,y).

\hat{e}_i \hat{e}_j = 0, \ when \ i \neq j

In a conformal transform of coordinates, XY --> UV the off diagonal elements in the UV basis remain zero.
 
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