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Magnetic moment contributions from the coupling of the electromagnetic current directly to sea-quark loops are neglected in these simulations. However, the net effect from u d, and s sea-quark loops is small due to approximate SU(3)-flavor symmetry where the net loop contribution vanishes
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Magnetic moment contributions from the coupling of the electromagnetic current directly to sea-quark loops are neglected in these simulations. However, the net effect from u, d, and s sea-quark loops is small due to approximate SU(3)-flavor symmetry where the net loop contribution vanishes.
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This dependence on (Formula presented) will eventually be alleviated as better lattice data become smaller quark masses, allowing a three parameter fit of Eq. (4)
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This dependence on (Formula presented) will eventually be alleviated as better lattice data become available at smaller quark masses, allowing a three parameter fit of Eq. (4).
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