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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 ab-plane, incident along long axis of prolate, polarized along short axis. 2_1o Oblate of isotropic material with dielectric function of ab-plane, incident along short axis of oblate, polarized along long axis.

2_2p Prolate of isotropic material with dielectric function of ab-plane, incident and polarized along short axis of prolate. 2_2o Oblate of isotropic material with dielectric function of ab-plane, incident and polarized along long axis of oblate.

2_3p Prolate of isotropic material with dielectric function of ab-plane, incident along Y, polarization angles 0°, 30°, 60°, 90°, starting from Z-axis 2_3o Oblate of isotropic material with dielectric function of ab-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

Notes. There is the dielectric function of the c-axis (index c), the other has the dielectric function of the ab-plane (index ab). The indices short, long describe the polarization direction of the incident light parallel to the short or long axis of the particle.

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