2021
DOI: 10.1111/sapm.12469
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Electromagnetic interactions of dipole distributions with a stratified medium: Power fluxes and scattering cross sections

Abstract: N magnetic dipoles radiate (inside or outside) a piecewise homogeneous (layered) and isotropic medium. The power fluxes and energy processes inside and outside the medium resulting from the various interactions between participating fields are investigated by means of the introduced interaction scattering cross sections (ISCS) and interaction power fluxes (IPF). Connections between the power flux through the excitation layers and the radiation in the far field are established by specifying the law of energy co… Show more

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Cited by 6 publications
(8 citation statements)
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“…Extinction cross‐section is the attenuation of the passing plane wave and is the result of the absorption and scattering cross‐section. [ 52,53 ] As determined through the Poynting vector, the absorption cross‐section, σ abs, and scattering cross‐sections, σ scatt , are given asσabs=4πka3Im(εεmε+2εm)$$\left(\sigma\right)_{\text{abs}} = 4 \pi k a^{3} I m \left(\right. \frac{\epsilon - \left(\epsilon\right)_{m}}{\epsilon + 2 \left(\epsilon\right)_{m}} \left.\right)$$σscatt=8π3k4a6| εεmε+2εm|2$$\left(\sigma\right)_{\text{scatt}} = \frac{8 \pi}{3} k^{4} a^{6} \left(\left|\right.…”
Section: Lspr and Plasmonic Materialsmentioning
confidence: 99%
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“…Extinction cross‐section is the attenuation of the passing plane wave and is the result of the absorption and scattering cross‐section. [ 52,53 ] As determined through the Poynting vector, the absorption cross‐section, σ abs, and scattering cross‐sections, σ scatt , are given asσabs=4πka3Im(εεmε+2εm)$$\left(\sigma\right)_{\text{abs}} = 4 \pi k a^{3} I m \left(\right. \frac{\epsilon - \left(\epsilon\right)_{m}}{\epsilon + 2 \left(\epsilon\right)_{m}} \left.\right)$$σscatt=8π3k4a6| εεmε+2εm|2$$\left(\sigma\right)_{\text{scatt}} = \frac{8 \pi}{3} k^{4} a^{6} \left(\left|\right.…”
Section: Lspr and Plasmonic Materialsmentioning
confidence: 99%
“…Extinction cross-section is the attenuation of the passing plane wave and is the result of the absorption and scattering cross-section. [52,53] As determined through the Poynting vector, the absorption cross-section, σ abs, and scattering cross-sections, σ scatt , are given as…”
Section: Fundamentals Of Plasmonic Visible Light Harvestingmentioning
confidence: 99%
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“…Inside the host medium Vh, the acoustic intensity boldIh is decomposed as follows [17]: boldIhfalse(rfalse)=boldIhprfalse(rfalse)+boldIhscfalse(rfalse)+boldIhintfalse(rfalse),where the primary intensity boldIhpr, scattered intensity boldIhsc and interaction intensity boldIhint are, respectively, given by right left right left right left right left right left right left3pt0em 2em 0em 2em 0em 2em 0em 2em 0em 2em 0emtrueIhpr=uhprϕhprfalse¯, right left right left right left right left right left right left3pt0em 2em 0em 2em 0em 2em 0em 2em 0em 2em 0emtrueIhsc=…”
Section: Multiple Scattering Problem Formulation and Geometry Settingmentioning
confidence: 99%
“…Specifically, the study of the energy process in sound propagation and scattering, in problems like propagation in acoustic waveguides [15] and reverberant spaces [16], requires the investigation of the complex form of the acoustic intensity vector. In particular, the imaginary part of the acoustic intensity accounts for the reactive intensity and enables a more global understanding of the various power exchanges occurring when more than one field coexist in the same volume [17,18]. The use of the complex form of the energy functionals reveals additional information about the energy transfer process [19,20], yet, requires an alteration in the mathematical approach for delivering scattering relations.…”
Section: Introductionmentioning
confidence: 99%