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Proton and neutron electromagnetic form factors in the continuum limit using lattice QCD ensembles with physical pion masses

Constantia Alexandrou1,2, Simone Bacchio1, Giannis Koutsou1, Bhavna Prasad1, and Gregoris Spanoudes2

Phys. Rev. D 113, 114524 – Published 29 June, 2026

DOI: https://doi.org/10.1103/tt39-n1df

Abstract

We compute the electromagnetic form factors of the proton and neutron using lattice QCD. We employ Nf=2+1+1 twisted mass clover-improved fermions with quark masses tuned to their physical values. Three ensembles with lattice spacings of a=0.080  fm, 0.068 fm, and 0.057 fm and approximately the same physical volume allow us to obtain the continuum limit directly at the physical pion mass. For each ensemble, we use several values of the sink-source time separation, ranging from 0.5 to 1.5 fm, to allow for a thorough analysis of excited-state effects via multistate fits. The disconnected contributions are also analyzed using high statistics combined with techniques to mitigate stochastic noise in the estimation of the fermion loop. These techniques include low-mode deflation, dilution in the color and spin components, and hierarchical probing. We study the momentum-transfer dependence of the form factors using the z-expansion and dipole Ansätze, thereby enabling the extraction of the electric and magnetic radii and the magnetic moments, as well as the Zemach and Friar radii in the continuum limit. Results for the proton and neutron electric and magnetic mean square radii are ⟨rE2⟩p=0.860(38)(23)  fm, ⟨rE2⟩n=−0.147(48)  fm2, ⟨rM2⟩p=0.870(53)(15)  fm, and ⟨rM2⟩n=0.913(67)(19)  fm, and for the proton and neutron magnetic moments, μp=2.849(92)(52) and μn=−1.819(76)(29), respectively. In all cases, the first error is statistical, and the second is systematic, where the latter includes an estimate of the error from the fits to the momentum dependence of the form factors and from the continuum extrapolation.

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