Work

Propagators in Curved Spacetimes from Operator Theory

Year: 2025
Type: article
Abstract: We discuss two distinct operator-theoretic settings useful for describing (or defining) propagators associated with a scalar Klein–Gordon field on a Lorentzian manifold M . Typically, we assume that M is globally hyperbolic. The term propagator here refers to any Green function or bisolution of the Klein–Gordon equation pertinent to Quantum Field Theory. The off-shell setting is based on the Hilbert space $$L^2(M)$$ L 2 ( M ) . It leads to the definition of the operator-theoretic Feynman and anti-Feynman propagators, which often coincide with the so-called in-out Feynman and out-in anti-Feynman propagator. On some special spacetimes, the sum of the operator-theoretic Feynman and anti-Feynman propagator equals the sum of the forward and backward propagator. This is always true on static stable spacetimes and, curiously, in some other cases as well. The on-shell setting is based on the Krein space $$\mathcal {W}_\textrm{KG}$$ W KG of solutions of the Klein–Gordon equation. It allows us to define 2-point functions associated with two, possibly distinct, Fock states as the Klein–Gordon kernels of projectors onto maximal uniformly positive subspaces of $$\mathcal {W}_\textrm{KG}$$ W KG . After a general discussion, we review a number of examples. We start with static and asymptotically static spacetimes, which are especially well suited for Quantum Field Theory. Then we discuss FLRW spacetimes, reducible by a mode decomposition to 1-dimensional Schrödinger operators. We compare various approaches to de Sitter space where, curiously, the off-shell approach gives non-physical propagators. Finally, we discuss the universal cover of anti-de Sitter spaces, where the on-shell approach may require boundary conditions, unlike the off-shell approach.
Language: English
Open Access status: hybrid
Estimated APC paid: $3,090
OpenAlex ID: W4417419877
FWCI: 4.841
Cites: 62
Cited by: 3
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