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Table 1
Modeling the FDTD spectra of the anisotropic material with spectra of hypothetical isotropic materials.
Setup | Prolate particles | Setup | Oblate particles |
---|---|---|---|
1_1p | Cabs = cos2(α)⋅Cab, short+sin2(α)⋅Cc, short | 1_1o | Cabs = cos2(α)⋅Cab, long+sin2(α)⋅Cc, long |
1_2p | Cabs = cos2(α)⋅Cab, short+sin2(α)⋅Cc, long | 1_2o | Cabs = cos2(α)⋅Cab, long+sin2(α)⋅Cc, short |
1_3p | Cabs = cos2(α)⋅Cab, long+sin2(α)⋅Cc, short | 1_3o | Cabs = cos2(α)⋅Cab, short+sin2(α)⋅Cc, long |
2_1p | Prolate of isotropic material with dielectric function of a–b-plane, incident along long axis of prolate, polarized along short axis. | 2_1o | Oblate of isotropic material with dielectric function of a–b-plane, incident along short axis of oblate, polarized along long axis. |
2_2p | Prolate of isotropic material with dielectric function of a–b-plane, incident and polarized along short axis of prolate. | 2_2o | Oblate of isotropic material with dielectric function of a–b-plane, incident and polarized along long axis of oblate. |
2_3p | Prolate of isotropic material with dielectric function of a–b-plane, incident along Y, polarization angles 0°, 30°, 60°, 90°, starting from Z-axis | 2_3o | Oblate of isotropic material with dielectric function of a–b-plane, incident along Y, polarization angles 0°, 30°, 60°, 90°, starting from Z-axis |
3_1p | Cabs = sin2(θ)⋅Cab, short+cos2(θ)⋅Cc, short | 3_1o | Cabs = sin2(θ)⋅Cab, long+cos2(θ)⋅Cc, long |
3_2p | Cabs = sin2(θ)⋅Cab, long+cos2(θ)⋅Cc, long | 3_2o | Cabs = sin2(θ)⋅Cab, short+cos2(θ)⋅Cc, short |
3_3p | Cabs = sin2(θ)⋅Cab, short+cos2(θ)⋅Cc, short | 3_3o | Cabs = sin2(θ)⋅Cab, long+cos2(θ)⋅Cc, long |
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