We present a transformation-optics approach which sheds analytical insight into the impact that spatial dispersion has on the optical response of separated dimers of metallic nanowires. We show that nonlocal effects are apparent at interparticle distances one order of magnitude larger than the longitudinal plasmon decay length, which coincides with the spatial regime where electron tunneling phenomena occur. Our method also clarifies the interplay between nonlocal and radiation effects taking place in the nanostructure, yielding the dimer dimensions that optimize its light harvesting capabilities. The impact of spatial nonlocality in the optical properties of metal nanoparticles is currently attracting great research attention. The presence of subnanometric geometric features in these nanostructures enables them to support extremely localized surface plasmon (SP) resonances. Classical electrodynamics predicts that the focusing ability of SPs is pushed to its maximum efficiency at these diminutive decorations, 1 where the extent of the electromagnetic fields become comparable to the Coulomb screening length ( ∼ 0.1 nm for noble metals). However, the local constitutive relations of macroscopic Maxwell's equations do not reflect the occurrence of significant electron-electron interactions in this spatial regime. Thus, a nonlocal treatment of the dielectric characteristics of metals, 2 beyond the free-electron Drude model, is required to clarify the limitations and guide the optimization of plasmonic devices.Although spatial dispersion in the permittivity of metals has been intensively studied in the past, 3-6 its experimental exploration has not been possible until very recently. Current fabrication and optical characterization techniques allow the probing of SP resonances below the nanometer, 7-10 which has renewed the theoretical interest in the nonlocal response of metallic nanostructures.11-13 Nanoparticle dimers are probably the system most thoroughly investigated in this context. [14][15][16] In this Rapid Communication, we revisit this geometry using a quasianalytical transformation-optics (TO) approach, 17 which was first developed within the local approximation.18-21 Lately, this method has been used to describe nonlocal effects in touching nanowires. 22 Here, we extend this TO framework to separated dimers, clarifying how spatial dispersion affects the light harvesting properties of these devices. Figure 1(a) depicts a pair of metal nanowires of radius R separated by a gap distance d, illuminated by an electric field polarized along the dimer axis. Under the logarithmic transformation indicated, the dimer maps into the metalinsulator-metal structure shown in Fig. 1(b). 18 The incident electric field maps into an array of dipole sources located at x = 0 with period 2π . The transformed parameters can be expressed in terms of the original ones as g = 4R √ ρ(1 + ρ) and a = 2 ln(is the relative gap size. The permittivity tensor of the dimer is described using the hydrodynamical model.2 Thus, the transverse co...