To be Raman-active (or, more generally, detectable using optical spectroscopy techniques), a vibrational mode of a nanosystem has to modulate its optical response. For small, isolated nanospheres, this is the case for only two categories of vibrational modes, namely quadrupolar and radial ones. However, assembling nanospheres as dimers makes additional modes Raman-active, as previously demonstrated by the detection in the ultralow frequency range of a hybridized quasi-translation mode in previous measurements on single and ensembles of gold nanosphere dimers. In the present work, we use our recently developed single-particle Raman spectroscopy setup to compare inelastic light scattering by single isolated and dimerized gold nanospheres in an extended frequency range (0-40 GHz). The Raman spectra acquired on isolated nanoparticles present a single peak associated to their fundamental quadrupolar mode, consistently with previous ensemble measurements. In contrast, the spectra measured on dimers are richer and display a number of peaks increasing with decreasing interparticle distance, with all = 2 − 8 Lamb modes detected in the quasicontact case. These observations are rationalized using a recently developed classical model of inelastic light scattering by nanospheres. Importantly, our modeling approach takes into account the real electric field within the nanoparticles DID contribution and the local changes of the intrinsic microscopic polarizabilities induced by the vibrations, and second the multiple scattering processes affecting the Stokes and anti-Stokes photons. Moreover, building a full opto-mechanical model of Raman scattering by nanoparticle dimers (or oligomers) simultaneously taking into account electromagnetic (as here) and acoustic (as in our previous works 24,25) interactions between close nanoparticles would be useful to address in more detail the inelastic scattering by =1 Lamb modes, which are highly affected by acoustic hybridization. ASSOCIATED CONTENT Supporting Information Determination of the input parameters; analysis of the extinction cross-sections; analysis of the Low Frequency Raman Spectra (LFRS) of the monomer, dimer A and dimer B; dependence of the LFSR on the inter-particle distance in dimers; comments about the dipole-induced-dipole mechanism; phenomenological modeling of the multiple scattering of the Stokes and anti-Stokes photons. This material is available free of charge via the Internet at http://pubs.acs.org.