Nucleon electromagnetic radii and magnetic moments are extracted from lattice QCD in the continuum limit directly at the physical pion mass, with disconnected contributions included.
In this case, the proton magnetic moment (µ p) is a fit parame- ter, in addition to the magnetic radius⟨r 2 M ⟩p
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Proton and neutron electromagnetic form factors from lattice QCD in the continuum limit
Nucleon electromagnetic radii and magnetic moments are extracted from lattice QCD in the continuum limit directly at the physical pion mass, with disconnected contributions included.