We report the first measurement of the many-body local-field factor G͑ q, v͒ for a simple metal (Al) at large wave vectors. Inelastic x-ray measurements of the dynamical structure factor are analyzed using ab initio calculations of the noninteracting polarizability. Our measured G͑ q, v͒ is in agreement with available theory for q , 1.5k F , unlike earlier electron energy-loss results; however, for q ϳ 2k F our G͑ q, v͒ is a factor of 2 stronger than most theoretical predictions. We have also measured the polarizability for noninteracting electrons at a wave vector for which G͑ q, v͒ Х 1. [S0031-9007(96)00863-0] PACS numbers: 71.45.Gm, 78.70.CkElectron-electron interactions play a central role in determining many of the physical properties of metals, including the excitation spectrum. Consideration of these interactions in terms of the random phase approximation (RPA) by Bohm and Pines [1], and the introduction of exchange-correlation corrections by Hubbard [2], dating back more than forty years, have formed the basis of an enormous theoretical effort aimed at understanding the effects of electron-electron interactions at metallic densities.In the case of the nearly-free-electron metals, the impact of the ion-core lattice (band structure) on the electronic excitations has been presumed to be small. However, recent x-ray measurements [3] and firstprinciples evaluations of the dynamical density response of Al [4,5] and Be [5] have shown that band structure effects cannot be neglected. Unfortunately, calculations of the effects of dynamical correlations for electrons propagating in the actual band structure of Al-or any other metal-are not yet available. It is then of interest that Fleszar, Quong, and Eguiluz [4] have suggested that x-ray measurements of the dynamical structure factor for large wave vectors could now be used to probe the details of the correlations in terms of a Hubbard-like many-body local-field factor (LFF) G͑ q, v͒ [6].In this Letter we report the first measurement of the many-body LFF for aluminum at large wave vectors. Our results were obtained from inelastic x-ray scattering measurements, combined with calculations of the dynamical density response for noninteracting electron-hole pairs. We find the experimentally determined LFF to be more than twice as strong as theoretical predictions [7][8][9][10][11][12][13] for the interacting electron gas in the critical 2k F region. On the other hand, and contrary to electron energy-loss determinations [14], our measured LFF is in agreement with theory [7-13] for q # 1.5k F . Our results indicate that the frequency dependence of the LFF is weak in the most interesting spectral region, in which the response contains the well-known double-peak structure of Al [15].Furthermore, we have made the first identification of a wave vector transfer for which the "experimental" G͑ q, v͒ Х 1 over a wide v interval. This finding allows unique insight into the dynamics of electrons in a metal, since for this special wave vector the x-ray photons probe the response of ...