Abstract

Microwave absorbers have important applications in various areas including stealth, camouflage, and antenna. Here, we have designed an ultra-broadband light absorber by integrating two different-sized tapered hyperbolic metamaterial (HMM) waveguides, each of which has wide but different absorption bands due to broadband slow-light response, into a unit cell. Both the numerical and experimental results demonstrate that in such a design strategy, the low absorption bands between high absorption bands with a single-sized tapered HMM waveguide array can be effectively eliminated, resulting in a largely expanded absorption bandwidth ranging from 2.3 to 40 GHz. The presented ultra-broadband light absorber is also insensitive to polarization and robust against incident angle. Our results offer a further step in developing practical artificial electromagnetic absorbers, which will impact a broad range of applications at microwave frequencies.

Highlights

  • Waveguide consists of alternating metal and dielectric layers with thickness denoted as tm and td, respectively

  • For the tapered Hyperbolic metamaterials (HMMs) waveguide array, the absorption frequency range is determined by the top width, bottom width, and the thickness filling ratio of the metal layer

  • Assuming the width grade of the tapered HMM waveguide array [left upper side of Fig. 1(a)] is sufficiently small, it can be deemed as a series of uniform HMM waveguide array [left down side of Fig. 1(a)]

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Summary

Results

The TM0 mode propagates along the tapered waveguide, and localizes at a specific position due to significant reduction of group velocity [see (1) in Fig. 1(d) as an example] It presents more high absorption bands above 5.2 GHz [see (2)–(6) in Fig. 1(c)], which can be attributed to the excitation of slow light of higher order TM modes. Some slow-light modes occur by chance at the bottom of the HMM waveguide array, a portion of EM wave will be reflected back into the air by the metal substrate, forming several low absorption bands (8)–(11) It can be given a further explanation that the slow-light modes cannot confine the light well comparing with the conventional single-layered absorbers[15,16,17].

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