2017
DOI: 10.1088/2040-8986/aa945d
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Characterization of surface-plasmon polaritons at lossy interfaces

Abstract: We characterize surface-plasmon polaritons at lossy planar interfaces between one dispersive and one nondispersive linear isotropic homogeneous media, i.e. materials or metamaterials. Specifically, we solve Maxwell's equations to obtain strict bounds for the permittivity and permeability of these media, such that satisfying these bounds implies surface-plasmon polaritons successfully propagate at the interface, and violation of the bounds impedes propagation, i.e. the field delocalizes from the surface into th… Show more

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Cited by 14 publications
(24 citation statements)
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“…Here, we employ metamaterial at the cladding of plasmonic waveguides, as an example of media with different EM properties, to check the sensitivity of the biosensor. Metamaterial with negative permittivity and positive permeability supports TM SPPs along the structure [7]. For Fishnet metamaterials with the structural parameters specified in Sec.3, TM SPPs propagate from 0.045ω e to 0.054ω e [16].…”
Section: Biosensor With Metamaterials At the Cladding Of Waveguidesmentioning
confidence: 99%
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“…Here, we employ metamaterial at the cladding of plasmonic waveguides, as an example of media with different EM properties, to check the sensitivity of the biosensor. Metamaterial with negative permittivity and positive permeability supports TM SPPs along the structure [7]. For Fishnet metamaterials with the structural parameters specified in Sec.3, TM SPPs propagate from 0.045ω e to 0.054ω e [16].…”
Section: Biosensor With Metamaterials At the Cladding Of Waveguidesmentioning
confidence: 99%
“…Surfaceplasmon polariton propagation depends on EM susceptibilities of media at the interface. Changing the sign of EM susceptibilities across the interface is the required condition for SPP propagation [7].…”
Section: Introductionmentioning
confidence: 99%
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“…We evaluate the optical properties of this NIMM layer employing macroscopic description of the metamaterial structure and we describe the permittivity and permeability of this structure using the Drude-Lorentz model [26,73,74] with permittivity for e ¥ andm ¥ the background constant for the permittivity and permeability, respectively. The other constants are ω l the perturbation frequency, ω e andω m are the electric and magnetic plasma frequencies, and γ e andγ m are the corresponding decay rates.…”
Section: Mathematical Formalism Of the Plasmonic Waveguidementioning
confidence: 99%
“…To characterize the optical properties of the NIMM layer, we employ macroscopic description of the permittivity (ε N ) and permeability (µ N ) following Drude-Lorentz model [57,58]. To this aim, we introduce the permittivity…”
Section: B Mathematical Description Of the Polaritonic Waveguidementioning
confidence: 99%