Diffraction Phenomena in Time-varying Metal-based Metasurfaces

TL;DR

This paper develops an analytical framework for analyzing time-varying metal-based metasurfaces, revealing their dynamic response, dispersion, and potential applications like pulsed sources and beamformers, validated by numerical simulations.

Contribution

It introduces a Floquet-Bloch modal expansion and an analytical circuit model for time-modulated metal metasurfaces, providing new insights into their diffraction and dispersion properties.

Findings

Good agreement with FDTD simulations.

Time-modulated screens can act as pulsed sources.

Potential for beamforming and analog sampling.

Abstract

This paper presents an analytical framework for the analysis of time-varying metal-based metamaterials. Concretely, we particularize the study to time-modulated metal-air interfaces embedded between two different semi-infinite media that are illuminated by monochromatic plane waves of frequency $\omega_0$. The formulation is based on a Floquet-Bloch modal expansion, which takes into account the time periodicity of the structure ($T_s = 2\pi / \omega_s)$, and integral-equation techniques. It allows to extract the reflection/transmission coefficients as well as to derive nontrivial features about the dynamic response and dispersion curves of time-modulated metal-based screens. In addition, the proposed formulation has an associated analytical equivalent circuit that gives physical insight to the diffraction phenomenon. Similarities and differences between space- and time-modulated metamaterials are discussed via the proposed circuit model. Finally, some analytical results are presented to validate the present framework. A good agreement is observed with numerical computations provided by a self-implemented finite-difference time-domain (FDTD) method. Interestingly, the present results suggest that time-modulated metal-based screens can be used as pulsed sources (when $\omega_s \ll \omega_0$), beamformers ($\omega_s \sim \omega_0$) to redirect energy in specific regions of space, and analog samplers ($\omega_s \gg \omega_0$).