Geometric significance of modular objects for non-conformally covariant quantum fields
Determine whether the Tomita–Takesaki modular conjugation J and modular automorphism group Δ associated with the local von Neumann algebra N(O) and the vacuum vector Ω in algebraic quantum field theory possess a geometric action for non-conformally covariant quantum fields, and, if so, characterize the corresponding spacetime transformations (analogous to Lorentz boosts for wedges or conformal transformations for double cones).
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The question if the Tomita-Takesaki modular objects of $\mathsf{N}(O)$, $\Omega$ have geometric significance for non-conformally covariant quantum fields is a longstanding question.
It is therefore conceivable that one could identify a Hadamard state whose modular flow approximately acts as the boost around $l$ and that satisfies an approximate KMS condition --- though whether such a state exists and whether it would be sufficient to recover a Type II algebra globally, remain open questions that need further investigation.