Optimum design of a novel plasmonic absorber-based material sensor using metaheuristic algorithm
This paper presents a miniaturized plasmonic absorber-based material sensor operating at 0.8 THz, designed using a multilayer graphene-polyimide structure. The absorber achieves theoretical near-unity absorptivity (100%) at the resonance frequency and exhibits strong polarization insensitivity and a...
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| Published in | Physica scripta Vol. 100; no. 7; pp. 75535 - 75547 |
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| Main Authors | , , |
| Format | Journal Article |
| Language | English |
| Published |
IOP Publishing
01.07.2025
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| Subjects | |
| Online Access | Get full text |
| ISSN | 0031-8949 1402-4896 |
| DOI | 10.1088/1402-4896/ade40b |
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| Summary: | This paper presents a miniaturized plasmonic absorber-based material sensor operating at 0.8 THz, designed using a multilayer graphene-polyimide structure. The absorber achieves theoretical near-unity absorptivity (100%) at the resonance frequency and exhibits strong polarization insensitivity and angular stability up to 80° for both polarization modes, attributed to its symmetric and compact geometry of 65 × 65 μm. The electrical size is approximately λ 0 /5, where λ 0 is the free-space wavelength at 0.8 THz, supporting subwavelength operation and enhanced confinement. The structure integrates a cross-slot, cross-dipole, and folded inductive loops to enhance coupling and impedance matching, resulting in a high-Q resonance. A metaheuristic Spider Monkey Algorithm (SMA) is employed to optimize the geometric parameters based on user-defined target frequency specifications, outperforming traditional inbuilt optimizers. The SMA achieves a Root Mean Square Error (RMSE) as low as 0.0131 and a Mean Absolute Percentage Error (MAPE) of 0.105%, indicating high prediction accuracy and model reliability. The optimized structure demonstrates a full width at half maximum (FWHM) of 17 GHz and a quality factor (Q) of approximately 47. The sensor’s refractive index sensitivity is measured at 725 GHz RIU −1 , and the figure of merit (FoM) is calculated to be 42.6. These results confirm the sensor’s potential for highly accurate dielectric material characterization in THz sensing applications. |
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| Bibliography: | PHYSSCR-142756.R1 |
| ISSN: | 0031-8949 1402-4896 |
| DOI: | 10.1088/1402-4896/ade40b |