Compact three‐dimensional bandpass FSS with high selectivity based on split square coaxial waveguide. Issue 21 (1st October 2019)

• Record Type: Journal Article
• Authors: Yu, Zhengyong; Yang, Xia; Tang, Wanchun; Shi, Yongrong; Zhu, Jianping; Wang, Cheng
• Is Part Of: Electronics letters. Volume 55:Issue 21(2019)
• Page Start: 1135
• Page End: 1137
• Publication Date: 2019-10-01
• Subjects: frequency selective surfaces -- coaxial waveguides -- electromagnetic coupling -- band‐pass filters -- poles and zeros -- parallel plate waveguides -- resonator filters -- waveguide filters; compact three‐dimensional bandpass FSS -- split square coaxial waveguide -- three‐dimensional frequency selective surface -- bandpass filtering response -- parallel‐plate waveguide propagation path -- SSCW propagation path -- identical short SCWs -- centred annular slot -- original single square slot resonant mode -- 3D FSS -- unit cell -- odd‐resonant modes -- even‐resonant modes -- transmission poles -- transmission zeros -- electromagnetic waves -- electric‐field distributions -- TM polarisations -- incident angles -- TE polarisations; Electronics -- Periodicals; 621.381
• DOI: 10.1049/el.2019.2189
• Languages: English
• ISSNs: 0013-5194

Abstract

Abstract : In this Letter, a compact three‐dimensional (3D) frequency selective surface (FSS), exhibiting a bandpass filtering response with high selectivity, is proposed based on the split square coaxial waveguide (SSCW). The unit cell of the presented 3D FSS consists of one parallel‐plate waveguide propagation path and one SSCW propagation path. In the SSCW path, two identical short SCWs are produced by employing a centred annular slot. Each short SCW intrinsically provides a square slot resonance. Owing to the electromagnetic coupling between these two square slot resonances, original single square slot resonant mode will split into even‐/odd‐resonant modes, resulting in a flat passband with two transmission poles. Moreover, two transmission zeros located at both sides of the passband are introduced for high selectivity, because the electromagnetic waves passing through these two different paths are combined out of phase. By investigating the electric‐field distributions at the frequencies of the transmission zeros/poles, the operating principle of the proposed 3D FSS is described. A prototype of the proposed 3D FSS is fabricated and measured. The measured results show that the proposed design can achieve a stable response under the incident angles up to 60° for both TE and TM polarisations.