2007
DOI: 10.1088/1464-4258/9/9/s03
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Peculiarities of light scattering by nanoparticles and nanowires near plasmon resonance frequencies in weakly dissipating materials

Abstract: Light scattering by a small spherical particle and nanowire with low dissipation rates are discussed according to the Mie theory (and similar solution for the cylinder). It is shown that near plasmon (polariton) resonance frequencies one can see non-Rayleigh anomalous light scattering with quite a complicated near-field energy flux.

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Cited by 60 publications
(44 citation statements)
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“…The above-described features of the energy flow pattern are attributed to the discontinuous behavior of the tangential component of the Poynting vector at the column surface, although the radial component S ρ of this vector remains continuous for ρ = a. As a result, the Poynting-vector lines undergo refraction at the column surface similarly to that observed at the boundary of an isotropic cylinder [18,19].…”
Section: Scattering At the Surface Plasmon Resonancesmentioning
confidence: 90%
“…The above-described features of the energy flow pattern are attributed to the discontinuous behavior of the tangential component of the Poynting vector at the column surface, although the radial component S ρ of this vector remains continuous for ρ = a. As a result, the Poynting-vector lines undergo refraction at the column surface similarly to that observed at the boundary of an isotropic cylinder [18,19].…”
Section: Scattering At the Surface Plasmon Resonancesmentioning
confidence: 90%
“…According to above theoretical analysis, the exact plasmon resonance appears when m = 0, which results in real and finite values |B m | = 1 at the resonance frequencies in both isotropic and anisotropic cases [15][16][17]19]. For a metallic cylinder, there are two different branches of optical resonances [15,19].…”
Section: Theoretical Calculationsmentioning
confidence: 90%
“…Incidentally, it is evident that the scattering coefficient B m reduces to the isotropic case by replacing ε r (ε t ) and µ z (µ t ) with ε and µ, respectively [11]. For the case of far field, the scattering efficiency of a circular cylinder can be expressed by B m [11,14,15,19],…”
Section: Formalismmentioning
confidence: 99%
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