Figure 6
Functional dependence of the rescaled value of \({\bar{R}}_{{\rm{BP}}}({\tau }_{1},{\tau }_{2})\) of Eq. (39) (blue continuous line) and \({\bar{R}}_{{\rm{CP}}}({\tau }_{1},{\tau }_{2})\) of Eq. (40) (red dashed line) upon τ2 for assigned values of τ1. Both of them get the symmetric dips when τ2 = ±τ1, moreover, \({\bar{R}}_{{\rm{BP}}}({\tau }_{1},{\tau }_{2})\) presents the maximum at τ2 = 0. As input state for the CP configuration we assume a Gaussian envelop of width Δω = ΔΩ− corresponding to have ΔΩ+ = 0 (i.e. ΔΩ− ≫ ΔΩ+) in Eq. (15). As in Fig. 5 all coincidences have been rescaled by their corresponding plateau values, i.e. respectively \({\bar{R}}_{{\rm{BP}}}({\tau }_{1},\infty )=1/2\) and \({\bar{R}}_{{\rm{CP}}}({\tau }_{1},\infty )={A}^{2}\).
