Recherches sur la propagation des ondes électromagnétiques sinusoïdales dans les milieux stratifiés

Abelès, F.

doi:10.1051/anphys/195012050706

Cited by 211 publications

(183 citation statements)

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“…For a multiple-layer stack, Maxwell's equations are conventionally implemented using a matrix formulation such as first provided by Abeles, 1 and further developed by Yeh. [2][3][4] The Snell invariant is born from the continuity of the field components along each interface.…”

Section: Introductionmentioning

confidence: 99%

Generalization of the Rouard method to an absorbing thin-film stack and application to surface plasmon resonance

Lecaruyer

Maillart²,

Canva³

et al. 2006

Appl. Opt.

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Section: Introductionmentioning

confidence: 99%

Generalization of the Rouard method to an absorbing thin-film stack and application to surface plasmon resonance

Lecaruyer

Maillart²,

Canva³

et al. 2006

Appl. Opt.

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“…And therefore the energy coefficients of the glazing system, from (4) can be written as, † It can be noted that this result is also obtained within the characteristic matrix theory, as shown by Abelès (1950), Theorem I: "The transmission factor of any stratified medium (absorbing or not) is independent of the sense of wave propagation". The proof of this theorem is made by induction, by showing that the product of characteristic matrices, ordered from front to back and vice versa, always has the same diagonal elements.…”

Section: General Solution For Laminated Glass With Internal and Extermentioning

confidence: 72%

“…Transfer matrix methods have been largely studied in the literature from different approaches (Centurioni 2005 These methods have their roots in the classical study of characteristic matrices (dependent on Fresnel coefficients for interference systems or coherent case) which connect the electromagnetic field components at an interface (Abelès 1950, Born and Wolf 1959, Heavens 1960 and the application of the method to thin films (Epstein 1952, Francombe and Hoffman 1971, Herpin 1947, Thelen 1989. The reformulation of these matrices in terms of coefficients relating energy magnitudes (through, e.g., the Poynting vector) allows the definition of transfer matrices as proposed herein.…”

Section: Introductionmentioning

confidence: 99%

Optical model for multilayer glazing systems: Application to laminated glass and photovoltaic modules

Baenas

Machado

2016

Solar Energy

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This article provides theoretical developments broadening the scope of previous optical simulation models for multilayer glazing systems. The applicability of existing models will be extended through additional characterization of the multilayer optical components from global spectrophotometric (UV-Vis-NIR) measurements. A more complete interlayer film characterization, including reflectivity in the film-glass interface, will be provided. Singular solutions of the related equation systems will be derived for situations involving components with very low or null transmissivity. As a contribution to the fundamentals of the formalism, the condition relating the symmetry of the transmittance of the system with the symmetry of the transmissivity of its optical components will be studied. Finally, with the extension for the calculation of energy fluxes through the components of a multilayer system, analytical expressions for the components absorptivity will be derived. These results are particularly useful to quantify differences in energy absorption of the constituents of a laminated glass, as a tool to define, from the glazing design phase, the thermal and mechanical processing needed for each glazing component. Additionally, the model provides a procedure for the calculation of the absorptivity of encapsulated photovoltaic cells, which is directly related to cell efficiency in each particular configuration.

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“…Table 2 shows refractive indexes and film thicknesses of (PDDA/SiO 2 ) 8, (PDDA/TALH) 20 and (PDDA/Na 2 SiO 3 ) 40 coated on silicon wafer measured by 632.5 nm of incident light wavelength were estimated by ellipsometer [21,22]. On the other hand, the calculated value of the refractive index and film thickness obtaied from the equations (1) to (5) was shown in Table 3.…”

Section: Self-assembled Nano Heterostructural Antireflection Filmmentioning

confidence: 99%

Highly Transparent Conductive Sheet by Self-assembled Silver Network Electrodes with Antireflective Coating via Roll-to-Roll Process

Fujimoto

Kyung

Shiratori

2013

MATEC Web of Conferences

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Abstract.A highly transparent conductive film was fabricated using self-assembled silver electrodes with anti-reflection (AR) film. The micro pore diameter of sliver nanoparticles (ca 50～60nm in diameter) network electrodes expanded to size of 200-300 μm by the increase of air voids with evaporated water. The transmittance of the silver network electrode increased was drastically increased by the optical interference from the AR film on the surface and it showed a maximal value 84％ (sheet resistance: 8.0 Ω/□). The surface resistance of silver network electrodes films did not change even after coating with the AR films because thickness of AR films (ca 100～200 nm) are extremely thin compared with the diameter of the silver wire (ca 3 µm). High performance transparent conductive film for electric and optical devic was successfully fabricated by roll to roll layer-by-layer (LBL) process.

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Recherches sur la propagation des ondes électromagnétiques sinusoïdales dans les milieux stratifiés

Cited by 211 publications

References 0 publications

Generalization of the Rouard method to an absorbing thin-film stack and application to surface plasmon resonance

Generalization of the Rouard method to an absorbing thin-film stack and application to surface plasmon resonance

Optical model for multilayer glazing systems: Application to laminated glass and photovoltaic modules

Highly Transparent Conductive Sheet by Self-assembled Silver Network Electrodes with Antireflective Coating via Roll-to-Roll Process

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