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The magnetic moments of the baryon decuplet are calculated in a relativistic constituent quark model using the light front formalism. Of particular interest are the magnetic moments of the Ω^- and Δ⁺⁺ for which new recent experimental measurements are available. Our calculation for the magnetic moment ratios μ(Δ⁺⁺)μ(p) and μ(Ω^-)μ(Λ⁰) is in excellent agreement with the experimental ratios.
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Felix Schlumpf (1993) studied this question.
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