“…The absorption peaks can be tuned by optimizing the shaped metallic grating structure located at the top of the MA. Recently, many efforts have been studied to widen the absorption bandwidth by using multi-shaped metallic configurations stacking of dielectric-meta layers [18,19], hole-arrays working as resonators [20], the shaped rectangular grating [21], shaped L grating [22,23], cylinder array [24], epsilon-near-zero (ENZ) materials [25,26], nanoporous materials that exhibit high efficiency in terms of broadband absorption, as well as their high applicability in sensors and easily fabricable devices [27][28][29][30]. However, these MA structures still have many disadvantages such as narrow absorption bandwidth, and polarization sensitivity due to the asymmetry structures having a low order of rotational symmetry, whereas many practical applications require the polarization-insensitive feature.…”