
Electromagnetic model of a nanodipole array above a double‐layer graphene by periodic green's function
Author(s) -
Cruz André,
Costa Karlo,
Dmitriev Victor,
Souza Nadson,
Zaman Quaid,
Del Rosso Tommaso
Publication year - 2020
Publication title -
iet microwaves, antennas and propagation
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.555
H-Index - 69
eISSN - 1751-8733
pISSN - 1751-8725
DOI - 10.1049/iet-map.2020.0161
Subject(s) - graphene , terahertz radiation , electromagnetic field , green's function , electromagnetic radiation , plasmon , optics , electric field , optoelectronics , physics , parametric statistics , function (biology) , materials science , convergence (economics) , surface plasmon , mathematics , quantum mechanics , evolutionary biology , biology , statistics , economics , economic growth
In this study, the authors present an electromagnetic model of a nanodipole array above a double‐layer Graphene (DLG) operating at Terahertz. The graphene layers deposited between the dielectric mediums are modelled as surface impedances with conductivities described by the Kubo model. The electromagnetic fields are defined by the spectral representation of the periodic Green's function with impedance condition between the mediums. The main objective of this work is to propose an equivalent and analytical electromagnetic model of a nanodipole array above a DLG, which can be used to describe a surface plasmon resonance sensor that operates at the terahertz frequency. As a way of validating the method, the authors compared the proposed model with a software based on the finite element method. In addition, still, as a form of validation, the authors verified the convergence of the method from the spectral analysis of the proposed Green's Function. As results, spatial and spectral parametric analyses are shown as a function of the concentration of nanodipoles in the array, and the chemical potential applied to the graphene layers. In these results, the authors verify the appearance of plasmonic, optical and acoustic modes, and their contributions in the total field.