Higher-dimensional black-hole topology conjecture with maximal rotational symmetry

About 14 years old · traced to

Let (TM,g)(\mathbb{T}{M},g) be a spin spacetime that is asymptotically flat or Kaluza–Klein, whose Ricci tensor satisfies the null-convergence condition, and that admits an action of U(1)D−3U(1)^{D-3}. Let Σ\Sigma be a Cauchy surface and let BH{\rm BH} denote the black-hole region. The asymptotic region is determined by the precise boundary conditions; for example, in the standard Kaluza–Klein setup it is R3×TD−4\mathbb{R}^3\times\mathbb{T}^{D-4}. Higher-dimensional black-hole topology conjecture. The Cauchy surface Σ\Sigma can be decomposed as

Σ≅[#k=2D−3mk⋅(Sk×SD−1−k) # (asymptotic region)]∖BH.\Sigma \cong \left[\#_{k=2}^{D-3} m_k\cdot\left(S^k\times S^{D-1-k}\right)\ \#\ ({\rm asymptotic\ region})\right]\setminus {\rm BH}.

This conjecture proposes a classification of the topology of Cauchy surfaces under maximal U(1)D−3U(1)^{D-3} symmetry, extending the restrictions known in lower dimensions. The multiplicities mkm_k and the precise asymptotic summand depend on the spacetime and boundary conditions.

References

Primary source

Stefan Hollands and Akihiro Ishibashi, “Black hole uniqueness theorems in higher dimensional spacetimes”, arXiv:1206.1164 (2012).

Progress summary

Never refreshed

Nothing recorded yet. Refresh searches the literature and the public web for attempts on this problem, and writes the first summary here.

Solutions 0

No solutions have been posted yet.