The static local-field factor (LFF) of the 2-D electron fluid is calculated nonperturbatively using a mapping to a classical Coulomb fluid [Phys. Rev. Lett., 87, 206404 (2001)]. The LFF for the paramagnetic fluid differs markedly from perturbation theory where a peak near 2kF is expected. Our LFF has a quasi-linear small-k region leading to a peak close to 3kF , in agreement with available quantum Monte Carlo data. The structure in the LFF and its dependence on the density and temperature are interpretted as a signature of correlated scattering of electron pairs of opposite spin. The lack of structure at 2kF implies weakened Friedel oscillations, Kohn anomalies etc. Introduction.-The physics of the uniform twodimensional electron fluid (2DEF) depends crucially on the "coupling parameter" Γ = (potential energy)/(kinetic energy). The Γ for the 2DEF at T = 0 and mean density n is equal to the mean-disk radius r s = (πn) −1/2 per electron. The parameter r s , the spin polarization ζ and the temperature T are the only variables in this problem.The response function χ(k, ω) is a property of the 2DEF sensitive to exchange-correlation effects. It is expressed in terms of a reference "zeroth-order" χ