“…Further, we defined g k,i (τ i ) = χ(τ i )g k,i = χg k,i , where g k,i is the usual coupling appearing in Q(τ i ). We note that, in case we consider the Minkowski vacuum, the state of the Rinder modes is given by the entangled state (10), such that the field in each wedge is in a thermal state, i.e., ρ I…”