2012
DOI: 10.1126/science.1224823
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Probing the Ultimate Limits of Plasmonic Enhancement

Abstract: Metals support surface plasmons at optical wavelengths and have the ability to localize light to sub-wavelength regions. The field enhancements that occur in these regions set the ultimate limitations on a wide range of nonlinear and quantum optical phenomena. Here we show that the dominant limiting factor is not the resistive loss of the metal, but the intrinsic nonlocality of its dielectric response. A semi-classical model of the electronic response of a metal places strict bounds on the ultimate field enhan… Show more

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Cited by 1,044 publications
(1,180 citation statements)
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“…This conclusion is supported by experiments by Scholl et al 28 on silver nanoparticles, where the bonding dipole plasmon was replaced by a charge-transfer plasmon below 0.27 nm. Other experiments on film-coupled nanoparticles 29 found the energy of hybridized modes to be blue shifted relative to the classical result at separations less than 1 nm, a similar blue shifting is anticipated for nanowire dimers within a hydrodynamic description. 30 However, until now, the influence of quantum effects on the spatial shape of the hybridized modes has not been explored.…”
Section: Introductionmentioning
confidence: 66%
“…This conclusion is supported by experiments by Scholl et al 28 on silver nanoparticles, where the bonding dipole plasmon was replaced by a charge-transfer plasmon below 0.27 nm. Other experiments on film-coupled nanoparticles 29 found the energy of hybridized modes to be blue shifted relative to the classical result at separations less than 1 nm, a similar blue shifting is anticipated for nanowire dimers within a hydrodynamic description. 30 However, until now, the influence of quantum effects on the spatial shape of the hybridized modes has not been explored.…”
Section: Introductionmentioning
confidence: 66%
“…Nonetheless, for the typical noble metals used in plasmonic experiments, the centroid of the charge is indeed displaced towards the interior of the particles due to the inuence of the bound d-electrons, and the hydrodynamic approach can then be applied for practical purposes. 47 In the following, we describe briey how we introduce the hydrodynamical approach into both the classical local and QCM theoretical frameworks. First, we discuss how the nonlocality is implemented into the optical response.…”
Section: Faraday Discussion Papermentioning
confidence: 99%
“…2,[64][65][66][67][68][69][70][71][72][73] The nonlocal hydrodynamical (NLHD) description has attracted considerable interest because of its numerical efficiency for arbitrarily-shaped objects 47,[74][75][76][77][78][79][80][81][82][83][84] and the possibility to obtain semi-analytical Example of the implementation of QCM in metallic gaps. In (a), a spatially inhomogeneous effective medium whose properties depend continuously on the separation distance is introduced in the gap between two metallic spheres.…”
Section: Introductionmentioning
confidence: 99%
“…single Au nanocube-film (NC-film) resonators ( Figure 1a) that can squeeze EM fields into an extremely narrow gap (a few nanometers wide, typically less than 100 / λ ) between nanoparticles and a metallic substrate [33][34][35][36][37]. The exceptionally small V significantly enhances the density of optical states, even enabling single molecules strong coupling in the cavity [38].…”
mentioning
confidence: 99%