Abstract

A novel design for an ultra-wide bandwidth and thin microwave absorber is introduced utilizing two frequency selective surfaces (FSSs) with different patterns of resonating frequencies. The circuit parameters, inductance and capacitance, of the three types of FSS (square loop, cross, square patch) were determined using an equivalent circuit and strip wire conductor model. The square loop FSS indicates a low frequency resonance (10 GHz) due to its high inductance and capacitance. On the other hand, the square patch of small inductance reveals a high resonating frequency (36 GHz). By optimizing the combination of the two FSSs, an ultra-wide absorption bandwidth (6.3–40.0 GHz for −10 dB reflection loss) was designed with a small total thickness of 5.5 mm, which is close to the theoretical limit. The free space measurement result with a test sample prepared by the screen printing method was in good agreement with the simulation result and verified the validity of the proposed design method. For these periodic array structures, however, the grating lobes were observed above the high frequency limit, and it needs to be emphasized that the further control of the unit cell periodicity is important, particularly for large oblique incidence angles.

Highlights

  • Further enhancement of absorption bandwidth has been reported by using the multilayers of frequency selective surfaces (FSSs) or metasurfaces[22,23,24,25,26,27]

  • Through a combination of two FSS patterns, an ultra-wide absorption bandwidth (6.3–40.0 GHz for −10 dB reflection loss) could be designed with a small total thickness of 5.5 mm, which is close to the theoretical limit

  • Resonance frequency can be determined from the transmission loss for the FSS structures which can be represented as an equivalent circuit of shunted L-C series circuit

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Summary

Frequency Selective Surfaces with Different Patterns

A novel design for an ultra-wide bandwidth and thin microwave absorber is introduced utilizing two frequency selective surfaces (FSSs) with different patterns of resonating frequencies. By optimizing the combination of the two FSSs, an ultra-wide absorption bandwidth (6.3–40.0 GHz for −10 dB reflection loss) was designed with a small total thickness of 5.5 mm, which is close to the theoretical limit. The free space measurement result with a test sample prepared by the screen printing method was in good agreement with the simulation result and verified the validity of the proposed design method. For these periodic array structures, the grating lobes were observed above the high frequency limit, and it needs to be emphasized that the further control of the unit cell periodicity is important, for large oblique incidence angles. A hexagonal pattern of resistive FSS was proposed for a broadband absorber with 10 dB bandwidth of 6.4–24.9 GHz at a thickness of 4 mm[17]

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FSS Square Loop Cross Square Patch
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