“…But compared with the second-and fourth-order schemes and the parameter one, the sixthorder method investigated here can achieve the best computational accuracy in all tested cases. Finally, we consider a practical model which is reduced from the large cavity electromagnetic scattering and has been investigated in [6,[34][35][36]. In this problem, Ω := (0, 1)×(0, 1 4 ), 1 4 ], Γ t := [1, 0] × { 1 4 }, Γ l := {0} × [ 1 4 , 0], f = 0, u = 0 on Γ b ∪ Γ r ∪ Γ l , ∂u ∂y + iku = g t on Γ t , which is the lowest-order approximation of the radiation boundary condition (see [6,18]).…”