“…As it was demonstrated in [41], the coupling coefficient, K (z), required to obtain a target frequency response, S 11 (β), can also be calculated through the kernel functions A 1 (z, τ ) and A 2 (z, τ ) of the GLM equations (50). Formulating the problem in the τ domain, by taking the inverse Fourier transform of the coupled-mode equations (32), substituting the solutions obtained (46), (48), (49), expressed also in the τ domain, and taking into account causality considerations (52), it can be deduced after several mathematical manipulations [41]…”