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Design of a Tunable Optical Filter by Using a One-Dimensional Ternary Photonic Band Gap Material

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Figure

Figure 1. Depiction of a one-dimensional ternary periodic lattice.
Table 1.Photonic bandgap for [n1 = 1.5, n2 = 2.2, n3 = 1.5,d1 = 0.85d, d2 = 0.85 × (0.15d), d3 = 0.15 × (0.15d), d = 140 nm].
Figure 3. Variation ofd Lλ0 with λ0 for [n1 = 3.6, n2 = 1.52, n3 = 3.6,1 = 0.85d, d2 = 0.85 × (0.15d), d3 = 0.15 × (0.15d) and d = 3000 nmat angles of incidence equal to 0◦, 30◦, and 60◦.
Figure 4. Variation ofat angles of incidence equal to 0d Lλ0 with λ0 for [n1 = 2.6, n2 = 1.52, n3 = 2.6,1 = 0.85d, d2 = 0.85 × (0.15d), d3 = 0.15 × (0.15d) and d = 600 nm◦, 30◦, and 60◦.
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