1992
DOI: 10.1109/50.144906
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TM-polarized surface-plasma modes on metal-coated dielectric cylinders

Abstract: The TM-polarized surface plasma modes on a thin metallic cylindrical shell imbedded in dielectric media are investigated. The dipersion characteristics of both bound modes and leaky waves are obtained for two sets of material parameters, the first corresponding to an optical fiber in which the metallic shell occupies a region between the core and the cladding and the second corresponding to a metal coated cylindrical rod in vacuum.

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Cited by 17 publications
(11 citation statements)
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“…The analysis of the natural modes supported by ENG (plasma) cylinders or cylindrical shells has been carried out in different papers (see, e.g., [23]- [26]), although mainly focused on surface wave propagation. An analogous analysis is applied here for the supported leaky-waves.…”
Section: Leaky-wave Dispersionmentioning
confidence: 99%
“…The analysis of the natural modes supported by ENG (plasma) cylinders or cylindrical shells has been carried out in different papers (see, e.g., [23]- [26]), although mainly focused on surface wave propagation. An analogous analysis is applied here for the supported leaky-waves.…”
Section: Leaky-wave Dispersionmentioning
confidence: 99%
“…The corresponding nonzero wave components, H , E r , and E z , obey the following relations [3]: where is the optical angular frequency, 0 is the vacuum permeability, 0 and are the permittivities of the vacuum and the medium respectively. For the analysis of TM waves, the inverse permittivity of the grating layer, 1/ , is used [4].For the CCMG waveguide under infinite length approximation, the solutions of (2) will be restricted to the 1 st -and 2 nd -type Hankel functions.…”
Section: A Equationsmentioning
confidence: 99%
“…O comportamento do ηefr e ηefi para espessura da cobertura extra (η3) de 0,01 a 2,44, são vistos nos gráficos 1.a e 1.b, enquanto que os de h superiores a 4, são mostrados nos gráficos 1c e 1d. Estes resultados são semelhantes aos encontrados na análise das estruturas convencionais de três regiões [4,7]. O que caracteriza a não influência da cobertura extra sobre os referidos modos.…”
Section: B Cálculo Das Componentes Dos Campos Eletromagnéticos Tangenciais As Fronteirasunclassified
“…No metal, os elétrons acoplados ao campo eletromagnético incidente oscilam dissipando energia por efeito Joule. Portanto, o modelo eletromagnético dos metais, sob a ação de ondas harmônicas da forma ( e +jwt ) é caracterizado pela permissividade: Є m = -Є 0 (Є mr + j Є mi ) [1,2,3,4] Neste artigo, são estudados os modos de Plasmon nas superfícies de um filme condutor (Є m ) de espessura (d) depositado sobre fibras ópticas fracamente guiadas (η 1 ) de raio (a). O filme condutor é recoberto por uma região dielétrica extra (η 3 ) de espessura (h) que por sua vez faz fronteira com a cobertura (η 4 ) infinita, como mostra a Figura.-1.…”
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