A longstanding problem in mathematical physics is the rigorous derivation of the incompressible Euler equation from Newtonian mechanics. Recently, Han-Kwan and Iacobelli [16] showed that in the monokinetic regime, one can directly obtain the Euler equation from a system of N particles interacting in T d , d ≥ 2, via Newton's second law through a supercritical mean-field limit. Namely, the coupling constant λ in front of the pair potential, which is Coulombic, scales like N −θ for some θ ∈ (0, 1), in contrast to the usual mean-field scaling λ ∼ N −1 . Assuming θ ∈ (1 − 2 d(d+1) , 1), they showed that the empirical measure of the system is effectively described by the solution to the Euler equation as N → ∞. Han-Kwan and Iacobelli asked if their range for θ was optimal. We answer this question in the negative by showing the validity of the incompressible Euler equation in the limit N → ∞ for θ ∈ (1 − 2 d , 1). For reasons of scaling, this range appears optimal in all dimensions. Our proof is based on Serfaty's modulated-energy method, but compared to that of Han-Kwan and Iacobelli, crucially uses an improved "renormalized commutator" estimate to obtain the larger range for θ.