Abstract

We propose and design a tunable triple-band millimeter-wave absorbing metasurface based on nematic liquid crystal (NLC). Numerical results based on both effective circuit model and full-wave simulations verify the triple-band absorption property. All triple absorption peaks can be shifted by changing the bias voltage applied to the nematic liquid crystal. We fabricate and measure a triple-band absorbing metasurface sample, which covers 100 × 100 mm2 and is composed of 20 × 20 unit cells. In experiments, when no bias voltage is applied to the NLC layer, the resonant frequencies of the absorbing metasurface are 25.4, 28.7, and 32.8 GHz, respectively. When a 5-V bias voltage is applied, all the absorbing peaks redshift, and a frequency tunability range of 9.5%, 9.1%, and 8.58% is observed in three resonant frequencies, respectively. The experimental results are in good agreement with the numerical simulations. The proposed tunable absorbing metasurface provides a way forward for the realization of tunable millimeter-wave metasurface devices that can be applied in multi-band detection and imaging.

Highlights

  • Limited by processing and parasitic effects, it is hard to extend the tunable devices with common semiconductor components adopted in the microwave band to a higher frequency band

  • There are some advantages of nematic liquid crystal (NLC)-based active metasurface devices:23,24 First, using NLCs can reduce the scale of the biasing network for the active metasurface devices

  • NLCs hold a relatively large tuning range of relative permittivity with varying bias voltage, which is beneficial in more advanced wave manipulations

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Summary

Introduction

Limited by processing and parasitic effects, it is hard to extend the tunable devices with common semiconductor components adopted in the microwave band to a higher frequency band. We propose and design a tunable NLC-based absorbing metasurface that works in the mmW frequency band. Based on the tunability of NLC materials, the absorbing metasurface can be adjusted by the bias voltage.

Results
Conclusion
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