Quantum Weyl conjecture

For every spacetime (M,g)(M,g) with a singularity S,S, if the Coulomb component of the Weyl tensor diverges at SS—equivalently, if the Newman--Penrose scalar Ψ2\Psi_2 diverges there—then quantum-field probes cannot reach S.S. Singularities for which only the radiative Weyl components Ψ0\Psi_0 or Ψ4\Psi_4 diverge need not obstruct quantum-field propagation and may remain accessible.

References

Primary source

Physical Review D

Additional references

Progress summary

Refreshed
Claimed progress

A 2026 paper gives evidence for a new rule about which singularities quantum fields can reach, but the conjecture has not been proved generally.

Ivo Sachs and Marc Schneider propose that quantum fields are blocked by singularities where the Coulomb component of spacetime curvature diverges, while certain other singular structures may remain accessible. The conjecture is motivated by explicit colliding-wave examples, not established in full generality.

2026 supporting examples

The analysis finds that quantum fields cannot reach the strong curvature singularity in the Khan–Penrose spacetime, but may reach and pass through the relevant Cauchy horizon in the Ferrari–Ibáñez spacetime. It formulates the proposed criterion using divergence of the Penrose–Newman scalar Ψ2\Psi_2; divergences only in Ψ0\Psi_0 or Ψ4\Psi_4 do not produce the same obstruction. No proof, counterexample, or verification of the conjecture was found.

Current status (as of August 2026): the conjecture has supporting calculations in the analyzed spacetimes but remains open in full generality.

Sources

Solutions 0

No solutions have been posted yet.