2013
DOI: 10.1364/oe.21.017089
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Nanoscale dielectric-graphene-dielectric tunable infrared waveguide with ultrahigh refractive indices

Abstract: We propose in this paper a dielectric-graphene-dielectric tunable infrared waveguide based on multilayer metamaterials with ultrahigh refractive indices. The waveguide modes with different orders are systematically analyzed with numerical simulations based on both multilayer structures and effective medium approach. The waveguide shows hyperbolic dispersion properties from mid-infrared to far-infrared wavelength, which means the modes with ultrahigh mode indices could be supported in the waveguide. Furthermore… Show more

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Cited by 124 publications
(53 citation statements)
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“…However, this phenomenon can happen at low energy with an effective speed of light (10 6 m −1 s −1 ). These electrons' wave of the lattice has never failed to attract attention [125]. Graphene has applications in the field of electrodes in electrical and optical devices.…”
Section: Application Of Graphene In Ledmentioning
confidence: 99%
“…However, this phenomenon can happen at low energy with an effective speed of light (10 6 m −1 s −1 ). These electrons' wave of the lattice has never failed to attract attention [125]. Graphene has applications in the field of electrodes in electrical and optical devices.…”
Section: Application Of Graphene In Ledmentioning
confidence: 99%
“…Due to the two dimensional nature of graphene, the electric field that is polarized in the normal direction to the graphene layer cannot excite any current in it. So, the normal component of the permittivity or the extraordinary permittivity of graphene is given by ǫ g⊥ = 1 [20]. The ordinary or the tangential permittivity can be defined by [17] …”
Section: A the Optical Properties Of Graphene Sheetsmentioning
confidence: 99%
“…The surface-normal permittivity of graphene is ε g,n =2.5, based on the dielectric constant of graphite [21,22]. By treating the graphene layer as a ultrathin layer with thickness d g =1 nm, the tangential component of the effective permittivity of graphene could be expressed as ε g,t =2.5−iσ g / ωε 0 d g [23]. The optical phonon scattering rate needs to be taken into account for the frequencies ω>ω oph (ℏω oph ≈0.2 eV, corresponding to the frequency f≈50 THz) [24], which could increase the real part of the conductivity and decrease the propagation length of GSPs.…”
Section: Models and Materialsmentioning
confidence: 99%