2015 IEEE Global Communications Conference (GLOBECOM) 2015
DOI: 10.1109/glocom.2015.7417131
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Three Dimensional End-to-End Modeling and Directivity Analysis for Graphene-Based Antennas in the Terahertz Band

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Cited by 6 publications
(16 citation statements)
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“…Starting from the classic harmonic macroscopic Maxwell's equations, we con-2 sider the electro-magnetic propagation inside a generic complex material, under 3 the assumption that it is a linear and chiral medium. 4 Unconventional materials (i.e., metamaterials) are specifically considered since 5 the GOA is reinforced by using thin metallic crossed-structure impurities in the 6 host dielectric medium, that is chiral-metamaterials [10]. Therefore, we consider 7 a time-harmonic generic linear material, where chiral (magneto/electric-optical) 8 effects are included in the following constitutive relations, written as: 10 where we remind that B is the magnetic displacement and H is the magnetic field, 11 as well as D is the electric displacement and E is the electric field.…”
Section: Full-wave Propagation Model In a Chiral-metamaterialsmentioning
confidence: 99%
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“…Starting from the classic harmonic macroscopic Maxwell's equations, we con-2 sider the electro-magnetic propagation inside a generic complex material, under 3 the assumption that it is a linear and chiral medium. 4 Unconventional materials (i.e., metamaterials) are specifically considered since 5 the GOA is reinforced by using thin metallic crossed-structure impurities in the 6 host dielectric medium, that is chiral-metamaterials [10]. Therefore, we consider 7 a time-harmonic generic linear material, where chiral (magneto/electric-optical) 8 effects are included in the following constitutive relations, written as: 10 where we remind that B is the magnetic displacement and H is the magnetic field, 11 as well as D is the electric displacement and E is the electric field.…”
Section: Full-wave Propagation Model In a Chiral-metamaterialsmentioning
confidence: 99%
“…where ω = 2πf , ε 0 , and µ 0 are the absolute permittivity and permeability, respec- 16 6 tively. Then, the constitutive parameters of interest are: 6 It is noted that the frequency resonant behavior of ξ r is a Drude-like one, and Ω ε , 7 Ω µ , Ω ξ , γ, and ω 0 are specific parameters of the GOA material [15]. 8 By simple computations, and assuming a lossy material, i.e.,…”
Section: Frommentioning
confidence: 99%
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