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Arrangement of supercells MM1–MM3 with lattice constant .
Simulated transmission of samples MM1, MM2, and MM3 as a function of the periodicity for an incident -field perpendicularly polarized to the gap-bearing sides of the SRRs.
(a) Measured and (b) simulated transmission spectra of samples MM1–MM3; the incident -field is polarized perpendicular to the gap-bearing sides of the SRRs. (c) Measured spectra of MM1–MM3 and (d) simulated spectrum of MM1 with the incident -field polarized parallel to the gap-bearing sides. (e) Measured and (f) simulated spectra of MM4–MM6.
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