2018
DOI: 10.3390/photonics5030022
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Two Types of Localized States in a Photonic Crystal Bounded by an Epsilon near Zero Nanocomposite

Abstract: Abstract:The spectral properties of a one-dimensional photonic crystal bounded by a resonant absorbing nanocomposite layer with the near-zero permittivity have been studied. The problem of calculating the transmittance, reflectance, and absorptance spectra of such structures at the normal and oblique incidence of light has been solved. It is shown that, depending on the permittivity sign near zero, the nanocomposite is characterized by either metallic or dielectric properties. The possibility of simultaneous f… Show more

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Cited by 14 publications
(6 citation statements)
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“…One of the fascinating thin-film phenomena is the so-called Bragg reflector, a stratified medium usually built from multiple alternating dielectric layers of varying refractive indexes or layer thicknesses [ 58 , 59 , 60 ]. The resulting periodic variation in the effective refractive index leads to superimposed partial reflection in the incidence region and potentially to constructive interference (in reflection).…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…One of the fascinating thin-film phenomena is the so-called Bragg reflector, a stratified medium usually built from multiple alternating dielectric layers of varying refractive indexes or layer thicknesses [ 58 , 59 , 60 ]. The resulting periodic variation in the effective refractive index leads to superimposed partial reflection in the incidence region and potentially to constructive interference (in reflection).…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…The mode excited at 0.7 < ξ s < 0.9 in the short-wavelength PBG is the Fabry-Perot cavity eigenmode, which corresponds to the resonance with a relatively low quality factor. The Fabry-Perot cavity is formed by an NC layer localized between air and the first PC layer [45]. The dispersion curve of the Fabry-Perot mode is determined by solving the equation corresponding to the phase matching condition −r 12 + r 23 + 2δ = 2πm.…”
Section: Resultsmentioning
confidence: 99%
“…It should be noted that under excitation from the PhC side, at the TPP wavelength (Figure 7b), 2.5% of the radiation falling onto the structure is not absorbed, but passes through the NC layer. This is related to the TPP formation in the range of small positive epsilon values, where the NC plays the role of a dissipative dielectric [45].…”
Section: Numerical Calculationmentioning
confidence: 99%