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λm is not exactly 0 at the resonance frequencies, due to the finite resistivity ρ 0 and cutoff parameter Mmax adopted here. We expect that λm reaches zero exactly at the resonance frequencies in the limit of ρ 0, Mmax →.
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λm is not exactly 0 at the resonance frequencies, due to the finite resistivity ρ 0 and cutoff parameter Mmax adopted here. We expect that λm reaches zero exactly at the resonance frequencies in the limit of ρ 0, Mmax →.
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Simulations were performed using the package CONCERTO 4.0, developed by Vector Fields, Limited, England, 2005. We have applied the perfect-metal boundary conditions for the air/metal interfaces. A basic cell sized 0.15 mm×0.15 mm×0.25 mm is employed to discretize the structure, and we have adopted finer meshes wherever necessary.
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Simulations were performed using the package CONCERTO 4.0, developed by Vector Fields, Limited, England, 2005. We have applied the perfect-metal boundary conditions for the air/metal interfaces. A basic cell sized 0.15 mm×0.15 mm×0.25 mm is employed to discretize the structure, and we have adopted finer meshes wherever necessary.
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33746085712
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We cannot unambiguously identify the modes with order higher than three since their strengths are too weak. The resonance frequencies do not perfectly match the theoretical values suggested in Fig. 2, which is suspected to be caused by the interactions between adjacent SRR's in the periodic array.
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We cannot unambiguously identify the modes with order higher than three since their strengths are too weak. The resonance frequencies do not perfectly match the theoretical values suggested in Fig. 2, which is suspected to be caused by the interactions between adjacent SRR's in the periodic array.
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