The quasiparticle effective mass m^* of the three-dimensional uniform electron gas (UEG) is a fundamental Fermi-liquid parameter whose value and density dependence have remained controversial for decades. Using renormalized perturbation theory with explicit counterterms, we determine m^* in the metallic regime (rₛ ≤ 6) from first principles by two complementary routes -- the self-energy and the forward-scattering four-point vertex via the p-wave spin-symmetric Landau parameter F₁ˢ -- that agree within uncertainties at each density through sixth renormalized order. The resulting m^*/m remains close to unity throughout the metallic regime, with a shallow non-monotonic density dependence -- a minimum near rₛ≈ 1 followed by a gentle upturn -- reflecting the interplay of exchange and dynamical screening in the self-energy, and disfavoring strong monotonic suppression. This finding supports a physical picture for the metallic UEG in which dominant charge correlations are concentrated in nearly forward scattering and generate only a weak F₁ˢ component.
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Hou et al. (2026) studied this question.
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