The conformal-equivalence conjecture for GenRel without localized time symmetry
Let be the first-order axiom system for general relativity, let denote the localized time-symmetry axiom, and let Lorentzian manifolds be the standard models of general relativity. Conformal-equivalence conjecture. If we leave out from , it will still capture Lorentzian manifolds up to conformal equivalence. This conjecture concerns the role of localized symmetry axioms in the first-order framework for general relativity: omitting them is expected to leave only the freedom of changing measurement units locally. The supplied text gives no resolution, so the conjecture remains open.
References
Primary source
Gergely Székely, “On some Symmetry Axioms in Relativity Theories”, arXiv:1601.03701 (2016).
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