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Perfectly matched layers in negative index metamaterials and plasmas

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Academic year: 2021

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Figure 2. The slowness curve for the isotropic wave equation. The geometrical criterion is satisfied on every point of the curve.
Figure 5. The slowness curves of S waves for two media. The geometrical criterion is satisfied for the left material but is not satisfied on the bold parts of the curve for the right one.
Figure 6. Illustration of the three frequency bands for the Drude model for the case ω e > ω m
Figure 7. Snapshots of the field H = H x + H y at different times t: the forward waves are well absorbed but the backward waves blow up exponentially
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