Thermally Tunable Bi-Functional Metasurface Based on InSb for Terahertz Applications
In this work, we propose and analyze a thermally tunable metasurface based on indium antimonide (InSb), designed to operate in the terahertz (THz) frequency range. The metasurface exhibits dual functionalities: single-band perfect absorption and efficient polarization conversion, enabled by the temperature-dependent permittivity of InSb. At approximately 280 K, InSb transitions into a metallic state, enabling the metasurface to achieve near-unity absorptance (100%) at 0.408 THz under normal incidence, independent of polarization. Conversely, when InSb behaves as a dielectric at 200 K, the metasurface operates as an efficient polarization converter. By exploiting structural anisotropy, it achieves a polarization conversion ratio exceeding 85% over the frequency range from 0.56 to 0.93 THz, while maintaining stable performance for incident angles up to 45°. Parametric analyses show that the resonance frequency and absorption intensity can be effectively tuned by varying the InSb square size and the silica (SiO<sub>2</sub>) layer thickness, achieving maximum absorptance at a SiO<sub>2</sub> thickness of 16 μm. The proposed tunable metasurface offers significant potential for applications in THz sensing, imaging, filtering, and wavefront engineering.
Authors
- Mark Clemente-Arenas (ORCID: https://orcid.org/0000-0002-2806-1513)
- Ruth E. Rubio-Noriega (ORCID: https://orcid.org/0000-0003-0869-8995)
- Rupesh Kumar (ORCID: https://orcid.org/0000-0003-4890-196X)
- Rafael Charca-Benavente (ORCID: https://orcid.org/0000-0001-8110-2540)
Institutions
- Universidad Nacional Tecnológica de Lima Sur (PE)
- SRM University (IN)
- National University of Engineering (PE)
- Pontificia Universidad Católica del Perú (PE)
Publication Details
- Journal
- Materials
- Published
- 2025-06-17
- DOI
- https://doi.org/10.3390/ma18122847
- Citations
- 8
- Primary Topic
- Metamaterials and Metasurfaces Applications
- Type
- article
- Field-Weighted Citation Impact
- 3.42