{"title":"EIT-Like Effect in Metamaterials based on Two-Layer Arrays for High-Gain Antennas","authors":"K. Kanjanasit, Sutasinee Sanesaowarod, N. Homsup","doi":"10.1109/ECTI-CON49241.2020.9158277","DOIUrl":null,"url":null,"abstract":"In this paper we present the comparative study of an electromagnetically induced transparent (EIT) effect in a two-layer metamaterial (MM) for a high-gain planar antenna application. The proposed mechanism of a low-profile EIT-like MM is based on an identical resonant square ring arrays in a sandwich structure with a small dielectric thickness. The EIT-like effect was observed connected with a resonance condition in a narrow transmission window due to the near-field coupling of the identical ring resonators behaved as a unit-cell element in periodic arrangement. The simulation study shows that the property of electric conductivity in a perfect electric conductor (PEC) and copper influences on a resonant transmission peak. The EIT-like MM was utilized for a high-gain directive planar antenna design by applying a blank conductor surface at a planar line symmetry acting as an electromagnetic mirror. The narrow aperture fed by short-end coplanar waveguide (CPW) feed-line was incorporated into a conductor surface as a driven radiator. The EIT-like MM antenna can be operated close to the targeted resonant frequency of the EIT-like MM (~10 GHz). The proposed planar antenna provides a thickness of λ/60 (0.5 mm). The simulation of the proposed planar antenna design was performed and it reports the antenna gain of 14.45 dBi and 13.32 dBi in cases of using the PEC- and copper-based square ring resonator array respectively. The antenna-gain difference is due to the ohmic-loss absorption regarding to electric conductivity.","PeriodicalId":371552,"journal":{"name":"2020 17th International Conference on Electrical Engineering/Electronics, Computer, Telecommunications and Information Technology (ECTI-CON)","volume":"5 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2020-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2020 17th International Conference on Electrical Engineering/Electronics, Computer, Telecommunications and Information Technology (ECTI-CON)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ECTI-CON49241.2020.9158277","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
In this paper we present the comparative study of an electromagnetically induced transparent (EIT) effect in a two-layer metamaterial (MM) for a high-gain planar antenna application. The proposed mechanism of a low-profile EIT-like MM is based on an identical resonant square ring arrays in a sandwich structure with a small dielectric thickness. The EIT-like effect was observed connected with a resonance condition in a narrow transmission window due to the near-field coupling of the identical ring resonators behaved as a unit-cell element in periodic arrangement. The simulation study shows that the property of electric conductivity in a perfect electric conductor (PEC) and copper influences on a resonant transmission peak. The EIT-like MM was utilized for a high-gain directive planar antenna design by applying a blank conductor surface at a planar line symmetry acting as an electromagnetic mirror. The narrow aperture fed by short-end coplanar waveguide (CPW) feed-line was incorporated into a conductor surface as a driven radiator. The EIT-like MM antenna can be operated close to the targeted resonant frequency of the EIT-like MM (~10 GHz). The proposed planar antenna provides a thickness of λ/60 (0.5 mm). The simulation of the proposed planar antenna design was performed and it reports the antenna gain of 14.45 dBi and 13.32 dBi in cases of using the PEC- and copper-based square ring resonator array respectively. The antenna-gain difference is due to the ohmic-loss absorption regarding to electric conductivity.