Clifton-Pohl torus

The Clifton-Pohl torus is a counterexample to show that it is possible to have a geodesically incomplete compact semi-Riemannian manifold.

1. History

2. Topology

As the name implies, the Clifton-Pohl torus is topologically homeomorphic to a torus. It can be obtained from $\mathbb{R}^2 \setminus \{ 0 \}$ quotiented with some isometry $\Gamma$, as seen below.

3. Metrics and coordinates

The torus is constructed from the following metric on $M = \mathbb{R}^2 \setminus \{ 0 \}$

$$ds^2 = 2 \frac{dtdx}{t^2 + y^2}$$

Homotheties are isometries of this metric :

$$(t,x) = (\lambda t, \lambda x)$$

in particular the case $\lambda = 2$. If we consider the group $\Gamma$ generated by that transformation (homotheties by a factor of $2^n$, $\Gamma$ has a proper, discontinuous action on $M$.

4. Tensor quantities

5. Symmetries

6. Stress-energy tensor

7. Curves

8. Equations

9. Causal structure

10. Asymptotic structure

11. Energy conditions

12. Limits and related spacetimes

13. Misc.

Bibliography