2015
DOI: 10.3390/ma8073910
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Plasmon-Polariton Properties in Metallic Nanosphere Chains

Abstract: The propagation of collective wave type plasmonic excitations along infinite chains of metallic nanospheres has been analyzed, including near-, medium- and far-field contributions to the plasmon dipole interaction with all retardation effects taken into account. It is proven that there exist weakly-damped self-modes of plasmon-polaritons in the chain for which the propagation range is limited by relatively small Ohmic losses only. In this regime, the Lorentz friction irradiation losses on each nanosphere in th… Show more

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Cited by 22 publications
(7 citation statements)
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“…Similarly as in the case of metallic nano-chains [38], ImF α (k, ω) ≡ 0 (for α = z, x(y)), which indicates the perfect quenching of the irradiation losses at any sphere in the chain (it means that to each sphere the same amount of energy incomes from other spheres as outflows due to the Lorentz friction). One can easily verify this property as the related infinite sums in Equation (43) can be found analytically [38,39]. Equation (42) is highly nonlinear with respect to the complex ω and can be solved both perturbatively in the analytical manner [27] or numerically-more accurately [40].…”
Section: Plasmon-polariton Propagation In Linear Periodic Ionic Systemmentioning
confidence: 83%
“…Similarly as in the case of metallic nano-chains [38], ImF α (k, ω) ≡ 0 (for α = z, x(y)), which indicates the perfect quenching of the irradiation losses at any sphere in the chain (it means that to each sphere the same amount of energy incomes from other spheres as outflows due to the Lorentz friction). One can easily verify this property as the related infinite sums in Equation (43) can be found analytically [38,39]. Equation (42) is highly nonlinear with respect to the complex ω and can be solved both perturbatively in the analytical manner [27] or numerically-more accurately [40].…”
Section: Plasmon-polariton Propagation In Linear Periodic Ionic Systemmentioning
confidence: 83%
“…Note that for 1 = 4 × 10 6 1/s and a = 50 μ m, the light-cone interference conditions kd − 1 d∕c = 0 and kd + 1 d∕c = 2 are fulfilled for extremely small values of kd and 2 − kd , respectively, (of the order of 10 −6 for d∕a ∈ [2, 2.5] ) and thus are negligible with regard to the plasmon-polariton kinetics [though are important for metals (Jacak et al 2015;Jacak 2014)]. The related singularities on the light-cone induced by the far-and medium-field Fig.…”
Section: Plasmon-polariton Model Of Saltatory Conduction: Fitting Thementioning
confidence: 99%
“…Note that for 1/s and m, the light-cone interference conditions and are fulfilled for extremely small values of kd and , respectively, (of the order of for ) and thus are negligible with regard to the plasmon-polariton kinetics [though are important for metals (Jacak et al. 2015 ; Jacak 2014 )]. The related singularities on the light-cone induced by the far- and medium-field contributions to the dipole interaction are pushed to the borders of the k domain and thus are unimportant for the considered ionic system.…”
Section: Plasmon-polariton Model Of Saltatory Conduction: Fitting Thementioning
confidence: 99%
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“…For more detailed calculations, including also the transverse polarization of plasmon-polariton modes and the formation of a plasmon-polariton wave packet, cf. (17,18,22,37). The bulk plasmon frequency for ions in an electrolyte (19,20) is = 2 4 (we assumed for the model that the ion charge is = 1.6 × 10 −19 C and the ion mass is = 10 4 , where = 9.1 × 10 −31 kg is the mass of an electron) and for a concentration of = 2.1 × 10 14 1/m 3 , we obtain the Mie-type frequency for ionic dipole oscillations, 1 .…”
Section: Mathematical Description Of Plasmon-polariton Kinetics In Thmentioning
confidence: 99%