2018
DOI: 10.1016/j.jqsrt.2017.11.009
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Spontaneous emission in plasmonic graphene subwavelength wires of arbitrary sections

Abstract: Abstract. We present a theoretical study of the spontaneous emission of a line dipole source embedded in a graphene-coated subwavelength wire of arbitrary shape. The modification of the emission and the radiation efficiencies are calculated by means of a rigorous electromagnetic method based on Green's second identity. Enhancement of these efficiencies is observed when the emission frequency coincides with one of the plasmonic resonance frequencies of the wire. The relevance of the dipole emitter position and … Show more

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Cited by 15 publications
(18 citation statements)
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“…Thus, as we have verified, the ASP and SSP contributions dominate the energy transfer process on the frequency region presented in Figure 3 (where the SPs are well defined) and consequently the WG contributions can be neglected in Eq. (23). Since the imaginary part of the graphene conductivity (see Appendix C) Imσ changes sign from positive to negative at ω/µ c ≈ 1.667, due to the presence of the interband term in the conductivity, p-polarized SPs are well defined on the frequency range below such frequency.…”
Section: Resultsmentioning
confidence: 99%
“…Thus, as we have verified, the ASP and SSP contributions dominate the energy transfer process on the frequency region presented in Figure 3 (where the SPs are well defined) and consequently the WG contributions can be neglected in Eq. (23). Since the imaginary part of the graphene conductivity (see Appendix C) Imσ changes sign from positive to negative at ω/µ c ≈ 1.667, due to the presence of the interband term in the conductivity, p-polarized SPs are well defined on the frequency range below such frequency.…”
Section: Resultsmentioning
confidence: 99%
“…The coupled integral equations (9)-(10), or Eq. (11) in case of the single wire system, are converted into matrix equations which are solved numerically (see [44] and references therein). Once the functions ϕ 1 ( r j ) and ∂ ϕ1( rj ) ∂nj are determined, the scattered field, given by the first of Eqs.…”
Section: Surface Integral Equations Of the Electromagnetic Field Scatmentioning
confidence: 99%
“…is the total power radiated by an electric dipole in the unbounded medium 1 [44,45]. By using the Ampere-Maxwell equation the relation between the components of the electric field and the z-component of the magnetic field is derived,…”
Section: Emitted and Radiated Powersmentioning
confidence: 99%
“…We also provided analytical expressions for the scattered power when the graphene elliptical wire is excited by a plane wave. All scattering curves are compared with those obtained by applying a rigorous formalism based in the Green surface integral method [35,36] valid for arbitrary shaped cross sections.…”
Section: Introductionmentioning
confidence: 99%