“…The non-analyticity of the correlators (14), and especially (16), in general overlooked in the literature, is required in order to achieve C 12 → 0 for large time-or space-separations, viz. All two-point functions (12,14,16) have indeed the symmetries C 12 (t 1 , t 2 ; r, r) = C 21 (t 2 , t 1 ; r, r) and C 12 (t, t; r 1 , r 2 ) = C 21 (t, t; r 2 , r 1 ), under permutation ϕ 1 ↔ ϕ 2 of the two scaling operators, as physically required for a correlator. The shape of the scaling functions of these three two-point functions is compared in figure 3.…”