“…The first geometry is defiened by {ρ = a, z ∈ (−∞, 0)} ∪ {ρ ∈ (a, b), z = 0} ∪ {ρ = b, z ∈ (0, ∞)}, and the second geometry is defined by {ρ = b, z ∈ (−∞, l)} ∪ {ρ ∈ (b, c), z = l} ∪ {ρ = c, z ∈ (l, ∞)}. The problem is reformulated according to geometries and scattering matrices are found by the help of Wiener-Hopf equation (Demir, 2017). Matrix sizes vary according to the number of incoming, reflected or transmitted modes.…”