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DC Field | Value | Language |
---|---|---|
dc.contributor.author | Singhal, Rahul | - |
dc.date.accessioned | 2024-12-16T09:29:44Z | - |
dc.date.available | 2024-12-16T09:29:44Z | - |
dc.date.issued | 2023 | - |
dc.identifier.uri | https://ieeexplore.ieee.org/abstract/document/10464074 | - |
dc.identifier.uri | http://dspace.bits-pilani.ac.in:8080/jspui/handle/123456789/16631 | - |
dc.description.abstract | Conventional designs of arrays of metallo-dielectric frequency selective surface (FSS) for terahertz (THz) frequency range such as square conducting pads (Pixels), metallic mesh, mesh-loop (ML), square loop (SL) and complementary square loop (CSL) are analyzed and compared through simulations. Pixel FSS demonstrates 0.58 THz wide stop-band and 0.14 THz wide pass-band centered at 2.96 THz and 3.35 THz respectively. By complementing, the pixel array becomes a mesh array that appears as a band-pass FSS from 1.89 THz to 3.45 THz. ML array is formed by removing a square ring from the mesh array and provides a 0.32 THz wide pass-band and 0.3 THz stop-band centered at 0.82 THz and 1.15 THz. After eliminating the outer mesh of ML array, SL array yields a 0.32 THz wide band-stop FSS centered at 1.22 THz. Later, the CSL array is formed when SL array is complemented, and the array demonstrates a 0.6 THz wide pass-band at 1.14 THz. The pixel array provides a high signal rejection capability and the widest −10dB stop-band in the frequency range of 2.58-3.16 THz. This analysis and comparison is significant for reduction of EM coupling or interference in THz based integrated circuits. | en_US |
dc.language.iso | en | en_US |
dc.publisher | IEEE | en_US |
dc.subject | EEE | en_US |
dc.subject | Terahertz | en_US |
dc.subject | Band stop | en_US |
dc.subject | Band pass | en_US |
dc.title | Electromagnetic Scattering Analysis of Conventional Frequency Selective Surfaces for Terahertz Applications | en_US |
dc.type | Article | en_US |
Appears in Collections: | Department of Electrical and Electronics Engineering |
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