The hyperon magnetic moments and the magnetic transition moment μ_Σ_⁰_Λ^^_^ have been calculated under various assumptions for the electromagnetic current operator within the spectrum-generating SU(3) approach. None of these assumptions, including the conventional ones using the Gell-Mann-Nishijima formula and SU(3) symmetry, lead to an acceptable fit to the experimental data.
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Arno Böhm (1978) studied this question.
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