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Finite-Difference Time-Domain Modeling of Space–Time-Modulated Metasurfaces
93
Citations
22
References
2017
Year
Numerical AnalysisElectromagnetic WaveEngineeringPhysicsApplied PhysicsNumerical SimulationMetasurfacesMetamaterialsSpace-time Varying MetasurfacesTemporal HarmonicsComputational ElectromagneticsFinite-difference Time-domain ModelingDynamic MetamaterialsFinitesize ZeroElectromagnetic MetamaterialsNumerical Method For Partial Differential Equation
A finite-difference time-domain modeling of finitesize zero thickness space-time-modulated Huygens' metasurfaces based on generalized sheet transition conditions is proposed and numerically demonstrated. A typical all-dielectric Huygens' unit cell is taken as an example and its material permittivity is modulated in both space and time, to emulate a traveling-type spatio-temporal perturbation on the metasurface. By mapping the permittivity variation onto the parameters of the equivalent Lorentzian electric and magnetic susceptibility densities, χ <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">ee</sub> and χ <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">mm</sub> , the problem is formulated into a set of second-order differential equations in time with nonconstant coefficients. The resulting field solutions are then conveniently solved using an explicit finite-difference technique and integrated with a Yee-cellbased propagation region to visualize the scattered fields taking into account the various diffractive effects from the metasurface of finite size. Several examples are shown for both linear and space-time varying metasurfaces which are excited with normally incident plane and Gaussian beams, showing detailed scattering field solutions. While the time-modulated metasurface leads to the generation of new collinearly propagating temporal harmonics, these harmonics are angularly separated in space, when an additional space modulation is introduced in the metasurface.
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