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Dual-band terahertz dielectric resonator antenna with graphene loading

机译:带石墨烯负载的双频太赫兹介质谐振器天线

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Abstract A graphene-based dual-band terahertz rectangular dielectric resonator antenna (DRA) is proposed in this work. The upper wall of the rectangular DRA is coated with graphene, which acts as an impedance surface to tune the resonant frequencies of the TE111ydocumentclass12pt{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} begin{document}$${{varvec{T}}{varvec{E}}}_{111}^{{varvec{y}}}$$end{document} and TE113ydocumentclass12pt{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} begin{document}$${{varvec{T}}{varvec{E}}}_{113}^{{varvec{y}}}$$end{document} modes of the antenna by varying its chemical potential. Also, it is observed that for some values of the chemical potential of graphene, the TE113ydocumentclass12pt{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} begin{document}$${{varvec{T}}{varvec{E}}}_{113}^{{varvec{y}}}$$end{document} mode is not well excited. In another part of the paper, an approximate formula for obtaining the resonant frequency of the graphene-loaded DRA is presented for the first time. The resonance frequency results obtained from this theoretical method for different chemical potential values are compared with the simulation results, and it is concluded that there is a good agreement between them.
机译:摘要 本文提出了一种基于石墨烯的双波段太赫兹矩形介质谐振天线(DRA)。矩形 DRA 的上壁涂有石墨烯,石墨烯充当阻抗面,用于调谐 TE111ydocumentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} begin{document}$${{varvec{T}}{varvec{E}}}_{111}^{{varvec{y}}}$$end{document} 和 TE113ydocumentclass[12pt]{minimal} usepackage{amsmath} usePackage{wasysym} usePackage{amsfonts} usePackage{amssymb} usePackage{amsbsy} usePackage{MathRSFS} usePackage{Upgreek} setLength{oddsidemargin}{-69pt} begin{document}$${{varvec{T}}{varvec{E}}}_{113}^{{varvec{y}}}$$end{document} 通过改变天线的化学势来表示模式。此外,观察到对于石墨烯化学势的某些值,TE113ydocumentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} begin{document}$${{varvec{T}}{varvec{E}}}_{113}^{{varvec{y}}}$$end{document}模式没有很好地激发。在论文的另一部分,首次提出了获得石墨烯负载DRA谐振频率的近似公式。将该理论方法得到的不同化学势值的共振频率结果与仿真结果进行了比较,得出了较好的一致性。

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