Modular Theory and the Bell-CHSH inequality in relativistic scalar Quantum Field Theory

The Tomita-Takesaki modular theory is employed to discuss the Bell-CHSH inequality in wedge regions.

By using the Bisognano-Wichmann results, the construction of a set of wedge localized vectors in the one-particle Hilbert space of a relativistic massive scalar field in $1+1$ dimensions is devised to establish whether violations of the Bell-CHSH inequality might occur for different choices of Bell's operators.

In particular, the construction of the wedge localized vectors employed in the seminal work by Summers-Werner is scrutinized and applied to Weyl and other operators.

We also outline a possible path towards the saturation of Tsirelson's bound.