The generation of few-cycle laser pulses proved to be a key enabling technology in strong-field physics and ultrafast science. the question naturally arises whether one can induce few-cycle localized plasmon oscillations in optical near-fields. Here, we perform a comparative study of different plasmonic nanoresonators illuminated by few-cycle pulses. We analyze the number of cycles (noc) of the plasmonic field, the near-field enhancement (NFE) as well as the figure of merit NFE/NOC. The pulse length dependence of these quantities is also investigated. throughout the inspected pulselength interval silica-gold and silica-silver core-shell monomers have the potential to preserve the noc of the incoming pulse, silver bow-ties result in the highest nfe, whereas gold core-shell dimers have the highest NFE/NOC. Based on the analysis, silver bow-ties, gold core-shell and silver nanorod dimers proved to be the most suitable for few-cycle near-field amplification. Few-cycle laser pulses (especially with carrier-envelope phase stabilization) proved to be highly important in many experiments in strong-field physics, attosecond science and pump-probe methods with ultrahigh time resolution. Therefore, the question naturally arises whether one can combine extreme temporal concentration of electromagnetic energy (in the form of few-cycle pulses 1,2) with ultrahigh spatial localization of laser fields readily provided by localized surface plasmon (LSP) resonance. Here, we investigate the possibility of the generation of few-cycle LSPs by analyzing the temporal response of different types of plasmonic nanoparticles and nanoparticle dimers. Plasmonic metal nanorods have already been investigated extensively. They inherently show plasmonic resonances corresponding to their short and long axes. The transversal and longitudinal resonance frequencies depend on the material, axis lengths and aspect ratio of the nanorod. Hence, nanorod LSP resonance can be tuned through wide spectral intervals by changing the geometry 3,4. Dielectric-metal core-shell type nanoresonators offer unique possibility of far-field and near-field control spanning wide spectral intervals via tailoring the plasmon hybridization promoted by two metal-dielectric interfaces 5,6. An interesting possibility is that dipolar resonance can be achieved at the same wavelength in two different generalized aspect ratio (GAR = R inner /R outer) intervals by applying the same core and shell materials 7. The thick (thin) shell composition supports a plasmonic resonance, which is accompanied by a spectrally wide (narrow) scattering cross-section maximum and low (high) absorbance. Although the scattering of core-shell nanoparticles is always lower than that of a homogeneous sphere, the achievable broad bandwidth and the possibility to control the Q factor of the plasmonic resonance by varying the GAR offers the unique possibility of electric field enhancement combined with the preservation of few-cycle transients 8,9. More complex plasmonic structures were also proposed and then u...