2012
DOI: 10.1016/j.optcom.2012.01.082
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Optical Fabry–Perot filter based on photonic band gap quasi-periodic one-dimensional multilayer according to the definite Rudin–Shapiro distribution

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Cited by 17 publications
(6 citation statements)
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“…and wavevector k e ≡ (k x , k ze ) = k √ ε e sin θ i , k √ ε e cos θ i , with k = ω/c = 2π/λ denoting the vacuum wavenumber (and c and λ the corresponding wave velocity and wavelength, respectively). Previous studies on GRS-type multilayered dielectric structures [34][35][36][37][38][39] have focused on the diffractive (photonic-crystal) regime characterized by moderately thick layers, showing interesting light-transport properties in terms of bandgap, filtering and field-enhancement. Here, we focus instead on the insofar unexplored deeply subwavelength regime, characterized by d a,b λ, in which the optical properties of such metamaterials are typically well described by simple EMT models based on Maxwell-Garnett-type mixing formulas [7].…”
Section: Statementmentioning
confidence: 99%
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“…and wavevector k e ≡ (k x , k ze ) = k √ ε e sin θ i , k √ ε e cos θ i , with k = ω/c = 2π/λ denoting the vacuum wavenumber (and c and λ the corresponding wave velocity and wavelength, respectively). Previous studies on GRS-type multilayered dielectric structures [34][35][36][37][38][39] have focused on the diffractive (photonic-crystal) regime characterized by moderately thick layers, showing interesting light-transport properties in terms of bandgap, filtering and field-enhancement. Here, we focus instead on the insofar unexplored deeply subwavelength regime, characterized by d a,b λ, in which the optical properties of such metamaterials are typically well described by simple EMT models based on Maxwell-Garnett-type mixing formulas [7].…”
Section: Statementmentioning
confidence: 99%
“…Moreover, we focus on the deeply subwavelength parameter regime 0.01λ < d < 0.05λ, and on incidence directions assumed parameters, this angular-incidence range guarantees that the field is evanescent in the "a"-type layers and propagating in the "b"-type ones. The regime characterized by smaller angles of incidence (0 < θ i < 30 o ), in which the field is propagating in both layers, has been extensively investigated in previous studies on photonic crystals [34][35][36][37][38][39], and is not of interest here. Overall, the assumed parameter regime is rather unusual, as the phase-accumulation mechanism is essentially dominated by the discrete jumps (Fresnel-type reflection/transmission) at the layer interfaces rather than the delay acquired via propagation through the (deeply subwavelength) layers.…”
Section: Generalitiesmentioning
confidence: 99%
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“…In all the performed calculations, the value of the H material refractive index is taken to be 2.3, which corresponds to titanium dioxide (TiO 2 ). The refractive index for L material is taken to be 1.45 (SiO 2 silica glass) [29,30]. Both media are assumed to be lossless, optically passive, and dispersionless, for the sake of the calculations.…”
Section: Methodsmentioning
confidence: 99%
“…As a new type of artificial material, PC has been widely concerned because of its simple structure, easy process and low cost. The PC has been applied in many fields such as infrared detectors [3], polychromatic F-P filters [4], PC fibre [5], PC laser [6] Perovskite solar cells [7] and so on.…”
Section: Introductionmentioning
confidence: 99%