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Application of cylindrical IE-GSTC to physical metasurfaces

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<div>This work validates cylindrical IE-GSTC by applying it to physical metasurfaces, i.e. metasurfaces defined by material properties and dimensions rather than by susceptibility tensor components. Previously reported IE-GSTC which was formulated for zero thickness GSTC discontinuity is extended to handle finite thickness of physical metasurfaces. A simple analytical approach is used to extract the bianisotropic susceptibility tensor of concentric, multilayered, magneto-dielectric shell. Plane wave scattering by a physical metasurface constructed of four segments of multilayered, magneto-dielectric metasurface scatterers is used as an example problem to validate cylindrical IEGSTC. A second example considers an opening on the cylindrical metasurface, confirming IE-GSTC can handle metasurfaces with openings. Good agreement is obtained between IE-GSTC results and full wave simulation results for both cases.</div>
Institute of Electrical and Electronics Engineers (IEEE)
Title: Application of cylindrical IE-GSTC to physical metasurfaces
Description:
<div>This work validates cylindrical IE-GSTC by applying it to physical metasurfaces, i.
e.
metasurfaces defined by material properties and dimensions rather than by susceptibility tensor components.
Previously reported IE-GSTC which was formulated for zero thickness GSTC discontinuity is extended to handle finite thickness of physical metasurfaces.
A simple analytical approach is used to extract the bianisotropic susceptibility tensor of concentric, multilayered, magneto-dielectric shell.
Plane wave scattering by a physical metasurface constructed of four segments of multilayered, magneto-dielectric metasurface scatterers is used as an example problem to validate cylindrical IEGSTC.
A second example considers an opening on the cylindrical metasurface, confirming IE-GSTC can handle metasurfaces with openings.
Good agreement is obtained between IE-GSTC results and full wave simulation results for both cases.
</div>.

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