2013
DOI: 10.3390/ma6114879
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Molding of Plasmonic Resonances in Metallic Nanostructures: Dependence of the Non-Linear Electric Permittivity on System Size and Temperature

Abstract: In this paper, we review the principal theoretical models through which the dielectric function of metals can be described. Starting from the Drude assumptions for intraband transitions, we show how this model can be improved by including interband absorption and temperature effect in the damping coefficients. Electronic scattering processes are described and included in the dielectric function, showing their role in determining plasmon lifetime at resonance. Relationships among permittivity, electric conducti… Show more

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Cited by 135 publications
(167 citation statements)
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References 107 publications
(153 reference statements)
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“…[30,31] However, a rigorous solution of the matching problem is not trivial, since the SPP K z in the grating region has a dependence on all the grating parameters, including P.…”
Section: Surface Plasmon Polariton Generationmentioning
confidence: 99%
“…[30,31] However, a rigorous solution of the matching problem is not trivial, since the SPP K z in the grating region has a dependence on all the grating parameters, including P.…”
Section: Surface Plasmon Polariton Generationmentioning
confidence: 99%
“…The results indicating that the loss factor is less salient at higher thicknesses. It is clearly visible that for all metals the minor losses are with a thickness of 55 nm [13]. …”
Section: -8mentioning
confidence: 95%
“…When the grain size is large, the relaxation rate is given by 0 Γ (it is the relaxation constant of the bulk material). When the grain size is small, as in the case of thin metal films, equation 20 describes additional grain-boundary scattering [13]:…”
Section: Electron-surface Scattering Surf γmentioning
confidence: 99%
See 1 more Smart Citation
“…SPs are bounded mode decaying from the interface in both media (metal and surrounding dielectric) losing energy along the propagation. The energy loss is scattered in the environment as radiation by means of photons (surface roughness, tip-end emission) and into the metal in a multiple step process which involves photon-electron (ph-e), electron-electron (e-e) and electronphonon (e-p) interactions [26]. While e-e and e-p scattering processes eventually lead to power dissipation and consequent heating of the structure, ph-e interaction produces, at first, electron-hole pairs and thus "hot"-electrons [9].…”
Section: Adiabatic Compression For Hot Electron Nanoscopymentioning
confidence: 99%