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Dual-Mode Tunable Near-Perfect Terahertz Absorber Based on GST Micro-Cavity
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A micro-cavity based on phase-change material is a very important strategy for the realization of tunable absorption and conversion of terahertz waves. In this work, a tunable terahertz metamaterial absorber based on the phase-change material germanium–antimony–tellurium (GST) is demonstrated. The device features a metal–insulator–metal triple-layer structure, where the dynamic switching of absorption characteristics is achieved via thermally controlled GST phase transition. In the amorphous state, the absorber exhibits a single absorption peak at 7.7 THz. Upon crystallization, the absorption switches to dual peaks at 5.1 THz and 8.3 THz, achieving near-perfect absorption in both states. Full-wave electromagnetic simulations and theoretical analysis based on a multiple-reflection interference model indicate that this performance tuning originates from the GST-phase-transition-induced change in the equivalent optical cavity length. This corresponds to a switch between two resonant modes: coupled inner–outer ring resonance and independent outer ring resonance. These results provide a foundation for developing dynamically tunable terahertz devices with promising applications in terahertz communications, imaging, and sensing.
Title: Dual-Mode Tunable Near-Perfect Terahertz Absorber Based on GST Micro-Cavity
Description:
A micro-cavity based on phase-change material is a very important strategy for the realization of tunable absorption and conversion of terahertz waves.
In this work, a tunable terahertz metamaterial absorber based on the phase-change material germanium–antimony–tellurium (GST) is demonstrated.
The device features a metal–insulator–metal triple-layer structure, where the dynamic switching of absorption characteristics is achieved via thermally controlled GST phase transition.
In the amorphous state, the absorber exhibits a single absorption peak at 7.
7 THz.
Upon crystallization, the absorption switches to dual peaks at 5.
1 THz and 8.
3 THz, achieving near-perfect absorption in both states.
Full-wave electromagnetic simulations and theoretical analysis based on a multiple-reflection interference model indicate that this performance tuning originates from the GST-phase-transition-induced change in the equivalent optical cavity length.
This corresponds to a switch between two resonant modes: coupled inner–outer ring resonance and independent outer ring resonance.
These results provide a foundation for developing dynamically tunable terahertz devices with promising applications in terahertz communications, imaging, and sensing.
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