2011
DOI: 10.4208/jcm.1009-m3303
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A Fast High Order Method for Electromagnetic Scattering by Large Open Cavities

Abstract: In this paper, the electromagnetic scattering from a rectangular large open cavity embedded in an infinite ground plane is studied. By introducing a nonlocal artificial boundary condition, the scattering problem from the open cavity is reduced to a bounded domain problem. A compact fourth order finite difference scheme is then proposed to discrete the cavity scattering model in the rectangular domain, and a special treatment is enforced to approximate the boundary condition, which makes truncation errors reach… Show more

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Cited by 26 publications
(17 citation statements)
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“…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]). Setting g t = -2ik cos θ e ik sin θx and θ = π 4 (see [6,36]), we show that the real part, the image part and magnitude of the solution with k = 128π, N = 512 in Figs. 3-4, which is consistent with that illustrated in [6,36].…”
Section: Figurementioning
confidence: 88%
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“…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]). Setting g t = -2ik cos θ e ik sin θx and θ = π 4 (see [6,36]), we show that the real part, the image part and magnitude of the solution with k = 128π, N = 512 in Figs. 3-4, which is consistent with that illustrated in [6,36].…”
Section: Figurementioning
confidence: 88%
“…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]).…”
Section: Figurementioning
confidence: 99%
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“…It is well known that high-order methods are more attractive for solving Helmholtz problems with large wave numbers because they can offer relative higher accurate solutions by utilizing fewer mesh points; eg, see other works. 21,[57][58][59][60][61][62][63] Efficient high-order methods and the corresponding fast algorithms for large wave number cavity problems with impedance boundary conditions are being considered.…”
Section: Discussionmentioning
confidence: 99%
“…LI nature of the large cavity problem, which is a perfect example for the long-standing high frequency scattering problems. Tremendous effort was made to develop various fast and accurate numerical methods to solve the large cavity problem [1,11,17,18,26,27,40,41,44,45]. The challenging mathematical issue is to establish the stability estimates with explicit dependence on the high wavenumber [12,13,27], which help us gain a deeper understanding on high frequency problems.…”
Section: Introductionmentioning
confidence: 99%